electronics-engineering: the Electronics Engineering program — user guide

electronics-engineering-ai999x 1.0.0, Rust build: command line, desktop app and browser. Creator / engineer: Ibnul Jaif Farabi · Company: AI999X · support@ai999x.com

Electronics Engineering covers semiconductors and pn junctions, diode circuits and rectifiers, BJT and MOSFET biasing and amplifiers, op-amp circuits, active filters, oscillators and 555 timers, ADCs and DACs, digital timing and power supplies. This guide is about electronics-engineering, the model as a self-contained program for Windows and Linux: 92 capabilities in 11 topics, answered on your own computer with no network, no Python and nothing else to install. The same compiled model runs in the AI999X desktop app and in the browser on the model's page (https://www.ai999x.com/models/electronics-engineering-ai999x/); the Python package (pip install electronics-engineering-ai999x) has its own guide. Every command output printed here is what the program printed.

Contents

• 1. Get it: desktop app, command line, browser, Python
• 2. Quick start
• 3. Writing inputs
• 4. Outcomes and exit codes
• 5. Scripts and agents: batch and JSON
• 6. Figures
• 7. In a web page or Node.js: WebAssembly
• 8. Every capability

1. Get it

Version 1.2.0 of the AI999X desktop app and of the command-line bundle. Checksums for every file: https://www.ai999x.com/downloads/desktop/1.2.0/SHA256SUMS; the newest version is always under https://www.ai999x.com/downloads/desktop/latest/. Full instructions: https://www.ai999x.com/desktop-cli/

Desktop app

Electronics Engineering in its own app: search, questions in words, input forms, live figures and explanations. Windows: Download ai999x-electronics-engineering-1.2.0-windows-x86_64.zip, right-click it → Extract All, then open the folder and start ai999x-electronics-engineering.exe. If Windows SmartScreen asks, choose More info → Run anyway. Linux:

curl -LO https://www.ai999x.com/downloads/desktop/1.2.0/ai999x-electronics-engineering-1.2.0-linux-x86_64.tar.gz
curl -LO https://www.ai999x.com/downloads/desktop/1.2.0/SHA256SUMS
sha256sum -c --ignore-missing SHA256SUMS
tar xzf ai999x-electronics-engineering-1.2.0-linux-x86_64.tar.gz
./ai999x-electronics-engineering-1.2.0-linux-x86_64/ai999x-electronics-engineering

It opens on this model: type a question or pick a capability, fill in the form and press Compute. The AI999X desktop app with every model works the same way (choose the model first). Windows: Download ai999x-1.2.0-windows-x86_64.zip, right-click it → Extract All, then open the folder and start ai999x.exe. If Windows SmartScreen asks, choose More info → Run anyway. Linux:

curl -LO https://www.ai999x.com/downloads/desktop/1.2.0/ai999x-1.2.0-linux-x86_64.tar.gz
curl -LO https://www.ai999x.com/downloads/desktop/1.2.0/SHA256SUMS
sha256sum -c --ignore-missing SHA256SUMS
tar xzf ai999x-1.2.0-linux-x86_64.tar.gz
./ai999x-1.2.0-linux-x86_64/ai999x

Command line — Linux

The bundle holds one program per model; electronics-engineering is this one. The checksum line should print OK.

curl -LO https://www.ai999x.com/downloads/desktop/1.2.0/ai999x-cli-1.2.0-linux-x86_64.tar.gz
curl -LO https://www.ai999x.com/downloads/desktop/1.2.0/SHA256SUMS
sha256sum -c --ignore-missing SHA256SUMS
mkdir -p ~/.local/share && tar xzf ai999x-cli-1.2.0-linux-x86_64.tar.gz -C ~/.local/share
echo 'export PATH="$HOME/.local/share/ai999x-cli-1.2.0-linux-x86_64:$PATH"' >> ~/.bashrc && source ~/.bashrc
electronics-engineering --version

Command line — Windows (PowerShell)

The fourth line should print True.

$F = "ai999x-cli-1.2.0-windows-x86_64.zip"
Invoke-WebRequest "https://www.ai999x.com/downloads/desktop/1.2.0/$F" -OutFile $F
Invoke-WebRequest "https://www.ai999x.com/downloads/desktop/1.2.0/SHA256SUMS" -OutFile SHA256SUMS
(Get-FileHash $F -Algorithm SHA256).Hash.ToLower() -eq ((Select-String -SimpleMatch $F SHA256SUMS).Line -split ' ')[0]
Expand-Archive $F -DestinationPath "$env:LOCALAPPDATA\AI999X" -Force
$D = "$env:LOCALAPPDATA\AI999X\ai999x-cli-1.2.0-windows-x86_64"; $env:Path += ";$D"
[Environment]::SetEnvironmentVariable("Path", [Environment]::GetEnvironmentVariable("Path", "User") + ";$D", "User")
electronics-engineering --version

In your browser

Open https://www.ai999x.com/models/electronics-engineering-ai999x/, choose a capability and press Compute in your browser: the same program runs on your device as WebAssembly; nothing is sent anywhere.

Python

pip install electronics-engineering-ai999x

2. Quick start

2.1 Check the install

Prints the model, its version and that this is the Rust build.

$ electronics-engineering --version
electronics-engineering-ai999x 1.0.0 (Rust build, ax-engine 0.1.0)

2.2 Find a capability

Search the capabilities by what you want to know; the first column is the id to pass to info and solve.

$ electronics-engineering search "bjt voltage-divider bias: exact q-point"
elx_bjt_voltage_divider_bias         BJT voltage-divider bias: exact Q-point  (BJT / DC bias)
elx_mosfet_divider_bias              MOSFET voltage-divider bias with source resistor: Q-point  (MOSFET / DC bias)
elx_bjt_collector_feedback_bias      BJT collector-feedback bias: Q-point  (BJT / DC bias)
elx_bjt_fixed_bias                   BJT fixed (base-resistor) bias: Q-point  (BJT / DC bias)
elx_bjt_emitter_bias                 BJT dual-supply emitter bias: Q-point  (BJT / DC bias)
elx_diode_operating_point            Operating point of a diode in series with a resistor (exact)  (diodes / operating point)
elx_bjt_cascode                      BJT cascode: output resistance, transconductance and gain  (BJT / amplifiers)
elx_differential_pair                BJT differential pair: differential and common-mode gain, CMRR  (BJT / differential amplifiers)
… 12 more

2.3 List the capabilities

Every capability the program answers: its id (what you pass to solve) and its name.

$ electronics-engineering list
elx_555_astable                          555 timer astable: frequency and duty cycle
elx_555_monostable                       555 timer monostable pulse width
elx_adc_code                             ADC output code, LSB and quantisation error
elx_adc_enob                             Effective number of bits (ENOB) from SINAD
elx_adc_quantization_snr                 ADC quantisation SNR with oversampling
elx_adjustable_regulator_output          Adjustable three-terminal regulator output voltage
elx_aperture_jitter_snr                  SNR limit from sampling-clock (aperture) jitter
elx_bjt_cascode                          BJT cascode: output resistance, transconductance and gain
… 84 more

2.4 What a capability needs

The equation or method, every input and output with its SI unit. Read this before solve: it tells you the input names.

$ electronics-engineering info elx_bjt_voltage_divider_bias
BJT voltage-divider bias: exact Q-point
  VTH = VCC R2/(R1 + R2); RTH = R1 || R2; IB = (VTH - VBE)/(RTH + (beta + 1) RE); VCE = VCC - IC RC - IE RE
  in   VCC      supply voltage [V]
  in   R1       upper divider resistor (supply to base) [ohm]
  in   R2       lower divider resistor (base to ground) [ohm]
  in   RC       collector resistor [ohm]
  in   RE       emitter resistor [ohm]
  in   beta     current gain [1]
  in   VBE      base-emitter voltage [V]
  out  VTH      Thevenin voltage of the divider [V]
  out  RTH      Thevenin resistance of the divider [ohm]
  out  IB       base current [A]
  out  IC       collector current [A]
  out  IE       emitter current [A]
  out  VB       base voltage [V]
  out  VE       emitter voltage [V]
  out  VC       collector voltage [V]
  out  VCE      collector-emitter voltage [V]

2.5 Solve

Inputs as name=value, each with any unit of the right kind. The answer lists every output, the method used, each input converted to SI, and the conditions the answer assumes.

$ electronics-engineering solve elx_bjt_voltage_divider_bias "VCC=12 V" "R1=47 kohm" "R2=10 kohm" "RC=2.2 kohm" "RE=470 ohm" beta=150.0 "VBE=0.7 V"
VTH = 2.105263158 V
RTH = 8245.614035 ohm
IB = 1.773972436e-05 A
IC = 0.002660958654 A
IE = 0.002678698378 A
VB = 1.958988238 V
VE = 1.258988238 V
VC = 6.145890962 V
VCE = 4.886902724 V
  by: BJT voltage-divider bias: exact Q-point  (VTH = VCC R2/(R1 + R2); RTH = R1 || R2; IB = (VTH - VBE)/(RTH + (beta + 1) RE); VCE = VCC - IC RC - IE RE)
  VCC = 12 V
  R1 = 47000 ohm
  R2 = 10000 ohm
  RC = 2200 ohm
  RE = 470 ohm
  beta = 150
  VBE = 0.7 V
  assumes: VTH > VBE; active region: VCE >= 0.2 V

2.6 Machine-readable answer

--json prints the same answer as one line of JSON (values in SI): for scripts and other programs.

$ electronics-engineering solve elx_bjt_voltage_divider_bias "VCC=12 V" "R1=47 kohm" "R2=10 kohm" "RC=2.2 kohm" "RE=470 ohm" beta=150.0 "VBE=0.7 V" --json
{"outcome":"SOLVED","message":"","value":0.00266095865382,"unit":"A","solved_for":"IC","si":[["VCC",12.0],["R1",47000.0],["R2",10000.0],["RC",2200.0],["RE",470.0],["beta",150.0],["VBE",0.7]],"values":[["VTH",2.10526315789,"V"],["RTH",8245.61403509,"ohm"],["IB",0.0000177397243588,"A"],["IC",0.00266095865382,"A"],["IE",0.00267869837818,"A"],["VB",1.95898823774,"V"],["VE",1.25898823774,"V"],["VC",6.1458909616,"V"],["VCE",4.88690272386,"V"]],"target":"IC","phrase":"Thevenin voltage of the divider","assumptions":["VTH > VBE","active region: VCE >= 0.2 V"],"name":"BJT voltage-divider bias: exact Q-point","equation":"VTH = VCC R2/(R1 + R2); RTH = R1 || R2; IB = (VTH - VBE)/(RTH + (beta + 1) RE); VCE = VCC - IC RC - IE RE"}

2.7 When an input is missing

No number is guessed: the answer names what is missing, shows a complete call, and the program exits with status 1.

$ electronics-engineering solve elx_bjt_voltage_divider_bias "VCC=12 V" "R1=47 kohm" "R2=10 kohm" "RC=2.2 kohm" "RE=470 ohm" beta=150.0
NEEDS_INPUT: elx_bjt_voltage_divider_bias needs VBE (base-emitter voltage). Example: solve('elx_bjt_voltage_divider_bias', VCC='12 V', R1='47000 ohm', R2='10000 ohm', RC='2200 ohm', RE='470 ohm', beta=150, VBE='0.7 V').

2.8 Many questions at once

One JSON request per line in, one JSON answer per line out, in order: for scripts, notebooks and agents (the program starts once). In PowerShell: Get-Content cases.jsonl | electronics-engineering batch

cases.jsonl:

{"key": "elx_bjt_voltage_divider_bias", "inputs": {"VCC": "12 V", "R1": "47 kohm", "R2": "10 kohm", "RC": "2.2 kohm", "RE": "470 ohm", "beta": 150.0, "VBE": "0.7 V"}}
{"key": "elx_sallen_key_lowpass", "inputs": {"R1": "10 kohm", "R2": "10 kohm", "C1": "20 nF", "C2": "10 nF", "K": 1.0}}

$ electronics-engineering batch < cases.jsonl
{"outcome":"SOLVED","message":"","value":0.00266095865382,"unit":"A","solved_for":"IC","si":[["VCC",12.0],["R1",47000.0],["R2",10000.0],["RC",2200.0],["RE",470.0],["beta",150.0],["VBE",0.7]],"values":[["VTH",2.10526315789,"V"],["RTH",8245.61403509,"ohm"],["IB",0.0000177397243588,"A"],["IC",0.00266095865382,"A"],["IE",0.00267869837818,"A"],["VB",1.95898823774,"V"],["VE",1.25898823774,"V"],["VC",6.1458909616,"V"],["VCE",4.88690272386,"V"]],"target":"IC","phrase":"Thevenin voltage of the divider","assumptions":["VTH > VBE","active region: VCE >= 0.2 V"],"name":"BJT voltage-divider bias: exact Q-point","equation":"VTH = VCC R2/(R1 + R2); RTH = R1 || R2; IB = (VTH - VBE)/(RTH + (beta + 1) RE); VCE = VCC - IC RC - IE RE"}
{"outcome":"SOLVED","message":"","value":0.707106781187,"unit":"","solved_for":"Q","si":[["R1",10000.0],["R2",10000.0],["C1",2e-8],["C2",1e-8],["K",1.0]],"values":[["f0",1125.3953952,"Hz"],["Q",0.707106781187,""],["H0",1.0,""],["peak_gain",0.707106781187,""]],"target":"Q","phrase":"natural frequency","assumptions":["stable: R1 C2 + R2 C2 + R1 C1 (1 - K) > 0","ideal amplifier"],"name":"Sallen-Key low-pass filter: f0, Q and gain","equation":"w0 = 1/sqrt(R1 R2 C1 C2); Q = sqrt(R1 R2 C1 C2)/(R1 C2 + R2 C2 + R1 C1 (1 - K))"}

3. Writing inputs

Inputs are written name=value, one per argument; electronics-engineering info <capability> lists the names. Quote an argument that holds a space or brackets (bash, zsh and PowerShell all accept double quotes). The answer always states each input as it was read, converted to SI, so a misread unit is visible at once.

An equation can be solved for any of its quantities: give the others and add --target <symbol>. Without --target, the program solves for the quantity the capability is named after.

4. Outcomes and exit codes

The program never guesses a number: when it cannot answer, it says why and exits with status 1, so a script can tell an answer from a refusal without reading the text.

5. Scripts and agents: batch and JSON

electronics-engineering solve ... --json prints one answer as one line of JSON. electronics-engineering batch reads one request per line on standard input and writes one JSON answer per line, in order, starting the program once for any number of requests. A request is {"key": "<capability>", "inputs": {"name": "value", ...}, "target": null}. In PowerShell, pipe the file in: Get-Content cases.jsonl | electronics-engineering batch. electronics-engineering catalog prints every capability with its inputs as JSON, to build forms or tool definitions.

import json, subprocess

reqs = [{"key": "<capability>", "inputs": {"name": "value"}}]
out = subprocess.run(["electronics-engineering", "batch"], input="\n".join(map(json.dumps, reqs)),
                     capture_output=True, text=True, check=True).stdout
answers = [json.loads(line) for line in out.splitlines()]

6. Figures

electronics-engineering figures <capability> name=value ... --out DIR draws the live figures for those inputs and writes each as an SVG file into DIR (an existing folder); without --out the SVG text comes back as JSON. The desktop app and the model page draw the same figures as soon as you press Compute.

7. In a web page or Node.js: WebAssembly

The same model is a WebAssembly module, electronics_engineering_ai999x.wasm (https://www.ai999x.com/compute/rust/electronics_engineering_ai999x.wasm), with a small loader, ax-wasm.js (https://www.ai999x.com/compute/rust/ax-wasm.js). It runs in a browser, a Web Worker or Node.js, with no server.

<script src="ax-wasm.js"></script>
<script>
  AXWasm.load("electronics_engineering_ai999x.wasm").then(function (m) {
    var a = m.solve({key: "<capability>", inputs: {name: "value"}});
    console.log(a.outcome, a.values || a.value);
    console.log(m.catalog().capabilities.length + " capabilities");
  });
</script>

8. Every capability

By topic. For each: what it does, what it needs and gives, when it applies, and a command with what the program printed for it. electronics-engineering info <id> shows the same inputs and outputs in the terminal.

Active filters (9)

Butterworth filter: Q of each second-order section — elx_butterworth_section_q

The quality factors of the cascaded second-order sections of an n-th order Butterworth filter (all at the cutoff frequency), and whether a first-order section is needed.

Applies when: 2 <= n <= 20.

$ electronics-engineering solve elx_butterworth_section_q n=4
Q_max = 1.306562965
Q = [0.541196100146,1.30656296488]
sections = 2
first_order = 0
  by: Butterworth filter: Q of each second-order section  (Q_k = 1/(2 sin((2k - 1) pi/(2n))), k = 1 .. floor(n/2))
  assumes: 2 <= n <= 20

In the worked example, n = 4 go through the equation above and give Q_max = 1.306562965, Q = [0.5411961001, 1.306562965], sections = 2, first_order = 0. It applies only when 2 <= n <= 20: outside that it says what is wrong instead of returning a number.

Butterworth or Chebyshev low-pass filter order — elx_filter_order

The minimum order of a Butterworth or Chebyshev type I low-pass filter meeting a passband edge with at most Ap dB attenuation and a stopband edge with at least As dB.

Applies when: fs > fp; As > Ap > 0.

$ electronics-engineering solve elx_filter_order ftype=Butterworth "fp=1000 Hz" "fs=2500 Hz" Ap=1 As=40
n = 6
  by: Butterworth or Chebyshev low-pass filter order  (Butterworth: n >= log10(D)/(2 log10(fs/fp)); Chebyshev: n >= acosh(sqrt D)/acosh(fs/fp), D = (10^(As/10) - 1)/(10^(Ap/10) - 1))
  fp = 1000 Hz
  fs = 2500 Hz
  Ap = 1
  As = 40
  ftype = Butterworth
  assumes: fs > fp; As > Ap > 0

In the worked example, ftype = Butterworth, fp = 1000 Hz, fs = 2500 Hz, Ap = 1, As = 40 go through the equation above and give n = 6. It applies only when fs > fp; As > Ap > 0: outside that it says what is wrong instead of returning a number.

Chebyshev type I filter: section Q and frequencies — elx_chebyshev_sections

The quality factors and natural frequencies (relative to the passband edge) of the second-order sections of an n-th order Chebyshev type I low-pass filter with a given passband ripple, and the real pole of an odd order.

Applies when: 2 <= n <= 16; 0.001 dB <= ripple <= 6 dB.

$ electronics-engineering solve elx_chebyshev_sections n=4 ripple=0.5
Q_max = 2.940554174
Q = [0.705110236803,2.94055417439]
f0_ratio = [0.59700239512,1.03127040148]
sections = 2
real_pole = 0
  by: Chebyshev type I filter: section Q and frequencies  (eps = sqrt(10^(r/10) - 1); a = asinh(1/eps)/n; poles -sinh a sin th_k + j cosh a cos th_k; Q = |p|/(2 |Re p|))
  ripple = 0.5
  assumes: 2 <= n <= 16; 0.001 dB <= ripple <= 6 dB

In the worked example, n = 4, ripple = 0.5 go through the equation above and give Q_max = 2.940554174, Q = [0.7051102368, 2.940554174], f0_ratio = [0.5970023951, 1.031270401], sections = 2. It applies only when 2 <= n <= 16; 0.001 dB <= ripple <= 6 dB: outside that it says what is wrong instead of returning a number.

Equal-component Sallen-Key low-pass design — elx_sallen_key_equal_component_design

The resistor value and amplifier gain of an equal-component (R1 = R2 = R, C1 = C2 = C) Sallen-Key low-pass filter for a cutoff frequency and Q, with the non-inverting gain ratio Rf/Rg = K - 1.

Applies when: 0.5 <= Q <= 20.

$ electronics-engineering solve elx_sallen_key_equal_component_design "fc=1000 Hz" Q=0.7071 "C=10 nF"
R = 15915.49431 ohm
K = 1.585772875
Rf_over_Rg = 0.5857728751
  by: Equal-component Sallen-Key low-pass design  (R = 1/(2 pi fc C); K = 3 - 1/Q; Rf/Rg = K - 1)
  fc = 1000 Hz
  Q = 0.7071
  C = 1e-08 F
  assumes: 0.5 <= Q <= 20

In the worked example, fc = 1000 Hz, Q = 0.7071, C = 10 nF go through the equation above and give R = 15915.49431 ohm, K = 1.585772875, Rf_over_Rg = 0.5857728751. It applies only when 0.5 <= Q <= 20: outside that it says what is wrong instead of returning a number.

First-order active low-pass filter (inverting) — elx_first_order_active_lowpass

The passband gain -Rf/R1, the cutoff frequency 1/(2 pi Rf C) and the gain at a frequency of an inverting op-amp low-pass filter with C across the feedback resistor.

Applies when: ideal op-amp.

$ electronics-engineering solve elx_first_order_active_lowpass "R1=10000 ohm" "Rf=100000 ohm" "C=1.59 nF" "f=1000 Hz"
H0 = -10
fc = 1000.974485 Hz
gain_f = 7.074510619
gain_dB = 16.99392806
  by: First-order active low-pass filter (inverting)  (H(s) = -(Rf/R1)/(1 + s Rf C); fc = 1/(2 pi Rf C))
  R1 = 10000 ohm
  Rf = 100000 ohm
  C = 1.59e-09 F
  f = 1000 Hz
  assumes: ideal op-amp

In the worked example, R1 = 10000 ohm, Rf = 100000 ohm, C = 1.59 nF, f = 1000 Hz go through the equation above and give H0 = -10, fc = 1000.974485 Hz, gain_f = 7.074510619, gain_dB = 16.99392806. It applies only when ideal op-amp: outside that it says what is wrong instead of returning a number.

Multiple-feedback (MFB) band-pass filter — elx_mfb_bandpass

The centre frequency, quality factor, -3 dB bandwidth and peak (inverting) gain of a multiple-feedback band-pass filter.

Applies when: ideal op-amp.

$ electronics-engineering solve elx_mfb_bandpass "R1=15900 ohm" "R2=1330 ohm" "R3=31800 ohm" "C1=10 nF" "C2=10 nF"
f0 = 2547.562384 Hz
Q = 2.54508224
BW = 1000.974485 Hz
H_peak = -1
  by: Multiple-feedback (MFB) band-pass filter  (w0 = sqrt((R1 + R2)/(R1 R2 R3 C1 C2)); Q = w0 C1 C2 R3/(C1 + C2); H = -C1 R3/(R1 (C1 + C2)))
  R1 = 15900 ohm
  R2 = 1330 ohm
  R3 = 31800 ohm
  C1 = 1e-08 F
  C2 = 1e-08 F
  assumes: ideal op-amp

In the worked example, R1 = 15900 ohm, R2 = 1330 ohm, R3 = 31800 ohm, C1 = 10 nF, C2 = 10 nF go through the equation above and give f0 = 2547.562384 Hz, Q = 2.54508224, BW = 1000.974485 Hz, H_peak = -1. It applies only when ideal op-amp: outside that it says what is wrong instead of returning a number.

Multiple-feedback (MFB) low-pass filter — elx_mfb_lowpass

The natural frequency, quality factor and inverting passband gain -R2/R1 of a second-order multiple-feedback low-pass filter.

Applies when: ideal op-amp.

$ electronics-engineering solve elx_mfb_lowpass "R1=10000 ohm" "R2=10000 ohm" "R3=5000 ohm" "C1=47 nF" "C2=4.7 nF"
f0 = 1514.38839 Hz
Q = 1.118033989
H0 = -1
  by: Multiple-feedback (MFB) low-pass filter  (w0 = 1/sqrt(R2 R3 C1 C2); Q = sqrt(R2 R3 C1 C2)/(C2 (R2 + R3 + R2 R3/R1)); H0 = -R2/R1)
  R1 = 10000 ohm
  R2 = 10000 ohm
  R3 = 5000 ohm
  C1 = 4.7e-08 F
  C2 = 4.7e-09 F
  assumes: ideal op-amp

In the worked example, R1 = 10000 ohm, R2 = 10000 ohm, R3 = 5000 ohm, C1 = 47 nF, C2 = 4.7 nF go through the equation above and give f0 = 1514.38839 Hz, Q = 1.118033989, H0 = -1. It applies only when ideal op-amp: outside that it says what is wrong instead of returning a number.

Sallen-Key high-pass filter: f0, Q and gain — elx_sallen_key_highpass

The natural frequency, quality factor and high-frequency gain of a second-order Sallen-Key high-pass filter with any components and amplifier gain K.

Applies when: stable: R1 (C1 + C2) + R2 C2 (1 - K) > 0.

$ electronics-engineering solve elx_sallen_key_highpass "C1=10 nF" "C2=10 nF" "R1=11250 ohm" "R2=22500 ohm" K=1
f0 = 1000.351462 Hz
Q = 0.7071067812
H_inf = 1
  by: Sallen-Key high-pass filter: f0, Q and gain  (w0 = 1/sqrt(R1 R2 C1 C2); Q = sqrt(R1 R2 C1 C2)/(R1 (C1 + C2) + R2 C2 (1 - K)))
  C1 = 1e-08 F
  C2 = 1e-08 F
  R1 = 11250 ohm
  R2 = 22500 ohm
  K = 1
  assumes: stable: R1 (C1 + C2) + R2 C2 (1 - K) > 0

In the worked example, C1 = 10 nF, C2 = 10 nF, R1 = 11250 ohm, R2 = 22500 ohm, K = 1 go through the equation above and give f0 = 1000.351462 Hz, Q = 0.7071067812, H_inf = 1. It applies only when stable: R1 (C1 + C2) + R2 C2 (1 - K) > 0: outside that it says what is wrong instead of returning a number.

Sallen-Key low-pass filter: f0, Q and gain — elx_sallen_key_lowpass

The natural frequency, quality factor, passband gain and the gain at f0 (K Q) of a second-order Sallen-Key low-pass filter with any components and amplifier gain K.

Applies when: stable: R1 C2 + R2 C2 + R1 C1 (1 - K) > 0; ideal amplifier.

$ electronics-engineering solve elx_sallen_key_lowpass "R1=10000 ohm" "R2=10000 ohm" "C1=20 nF" "C2=10 nF" K=1
f0 = 1125.395395 Hz
Q = 0.7071067812
H0 = 1
peak_gain = 0.7071067812
  by: Sallen-Key low-pass filter: f0, Q and gain  (w0 = 1/sqrt(R1 R2 C1 C2); Q = sqrt(R1 R2 C1 C2)/(R1 C2 + R2 C2 + R1 C1 (1 - K)))
  R1 = 10000 ohm
  R2 = 10000 ohm
  C1 = 2e-08 F
  C2 = 1e-08 F
  K = 1
  assumes: stable: R1 C2 + R2 C2 + R1 C1 (1 - K) > 0; ideal amplifier

In the worked example, R1 = 10000 ohm, R2 = 10000 ohm, C1 = 20 nF, C2 = 10 nF, K = 1 go through the equation above and give f0 = 1125.395395 Hz, Q = 0.7071067812, H0 = 1, peak_gain = 0.7071067812. It applies only when stable: R1 C2 + R2 C2 + R1 C1 (1 - K) > 0; ideal amplifier: outside that it says what is wrong instead of returning a number.

BJT (16)

BJT beta cutoff and transition frequency fT — elx_transition_frequency

The beta cutoff frequency f_beta and the unity-current-gain (transition) frequency fT = gm/(2 pi (Cpi + Cmu)) of a bipolar transistor from its hybrid-pi capacitances.

Applies when: single-pole h_fe (the feed-forward zero through Cmu neglected).

$ electronics-engineering solve elx_transition_frequency "gm=40 mS" beta=100 "Cpi=10 pF" "Cmu=2 pF"
r_pi = 2500 ohm
f_beta = 5305164.77 Hz
f_T = 530516477 Hz
  by: BJT beta cutoff and transition frequency fT  (f_beta = 1/(2 pi r_pi (Cpi + Cmu)); fT = beta f_beta = gm/(2 pi (Cpi + Cmu)))
  gm = 0.04 S
  beta = 100
  Cpi = 1e-11 F
  Cmu = 2e-12 F
  assumes: single-pole h_fe (the feed-forward zero through Cmu neglected)

In the worked example, gm = 40 mS, beta = 100, Cpi = 10 pF, Cmu = 2 pF go through the equation above and give r_pi = 2500 ohm, f_beta = 5305164.77 Hz, f_T = 530516477 Hz. It applies only when single-pole h_fe (the feed-forward zero through Cmu neglected): outside that it says what is wrong instead of returning a number.

BJT cascode: output resistance, transconductance and gain — elx_bjt_cascode

The output resistance, the short-circuit transconductance and the voltage gain into a load of a cascode (common emitter driving common base) of two identical transistors at the same bias current.

Applies when: identical transistors, base of the upper one at signal ground.

$ electronics-engineering solve elx_bjt_cascode "IC=1 mA" beta=100 "VT=25 mV" "VA=100 V" "RL=1000000 ohm"
gm = 0.04 S
r_o = 100000 ohm
Rout = 9858536.585 ohm
Gm = 0.03959426027 S
Av = -35947.88859
  by: BJT cascode: output resistance, transconductance and gain  (Rout = r_o + (1 + gm r_o)(r_o || r_pi); Gm = gm (gm + 1/r_o)/(gm + 2/r_o + 1/r_pi); Av = -Gm (Rout || RL))
  IC = 0.001 A
  beta = 100
  VT = 0.025 V
  VA = 100 V
  RL = 1000000 ohm
  assumes: identical transistors, base of the upper one at signal ground

In the worked example, IC = 1 mA, beta = 100, VT = 25 mV, VA = 100 V, RL = 1000000 ohm go through the equation above and give gm = 0.04 S, r_o = 100000 ohm, Rout = 9858536.585 ohm, Gm = 0.03959426027 S. It applies only when identical transistors, base of the upper one at signal ground: outside that it says what is wrong instead of returning a number.

BJT collector-feedback bias: Q-point — elx_bjt_collector_feedback_bias

The Q-point of a transistor biased by a resistor from collector to base (collector feedback), with an optional emitter resistor.

Applies when: active region: VCE >= 0.2 V.

$ electronics-engineering solve elx_bjt_collector_feedback_bias "VCC=10 V" "RC=4700 ohm" "RF=250000 ohm" beta=90 "VBE=0.7 V"
IB = 1.372288623e-05 A
IC = 0.001235059761 A
IE = 0.001248782647 A
VC = 4.130721558 V
VCE = 4.130721558 V
  by: BJT collector-feedback bias: Q-point  (IB = (VCC - VBE)/(RF + (beta + 1)(RC + RE)); VC = VCC - IE RC)
  VCC = 10 V
  RC = 4700 ohm
  RF = 250000 ohm
  beta = 90
  VBE = 0.7 V
  assumes: active region: VCE >= 0.2 V

In the worked example, VCC = 10 V, RC = 4700 ohm, RF = 250000 ohm, beta = 90, VBE = 0.7 V go through the equation above and give IB = 1.372288623e-05 A, IC = 0.001235059761 A, IE = 0.001248782647 A, VC = 4.130721558 V. It applies only when active region: VCE >= 0.2 V: outside that it says what is wrong instead of returning a number.

BJT current mirror with finite beta — elx_current_mirror

The reference current and the output current of a basic two-transistor current mirror with a resistor to the supply, including the base-current error Iout = Iref beta/(beta + 2).

Applies when: matched transistors, Early effect neglected.

$ electronics-engineering solve elx_current_mirror "VCC=10 V" "R=9300 ohm" "VBE=0.7 V" beta=100
Iref = 0.001 A
Iout = 0.0009803921569 A
ratio = 0.9803921569
  by: BJT current mirror with finite beta  (Iref = (VCC - VBE)/R; Iout = Iref beta/(beta + 2))
  VCC = 10 V
  R = 9300 ohm
  VBE = 0.7 V
  beta = 100
  assumes: matched transistors, Early effect neglected

In the worked example, VCC = 10 V, R = 9300 ohm, VBE = 0.7 V, beta = 100 go through the equation above and give Iref = 0.001 A, Iout = 0.0009803921569 A, ratio = 0.9803921569. It applies only when matched transistors, Early effect neglected: outside that it says what is wrong instead of returning a number.

BJT differential pair: differential and common-mode gain, CMRR — elx_differential_pair

The differential gain (differential and single-ended output), the common-mode gain and the common-mode rejection ratio of a resistively loaded BJT differential pair with a tail current source of finite resistance.

Applies when: matched transistors, r_o neglected.

$ electronics-engineering solve elx_differential_pair "I_tail=1 mA" beta=100 "VT=25 mV" "RC=10000 ohm" "REE=100000 ohm"
IC = 0.000495049505 A
gm = 0.0198019802 S
Ad_diff = -198.019802
Ad_se = -99.00990099
Acm = -0.04949257735
CMRR = 2000.5
CMRR_dB = 66.02277111
  by: BJT differential pair: differential and common-mode gain, CMRR  (IC = alpha I/2; gm = IC/VT; Ad = -gm RC (/2 single-ended); Acm = -gm RC/(1 + 2 REE (beta + 1)/r_pi); CMRR = |Ad,se/Acm|)
  I_tail = 0.001 A
  beta = 100
  VT = 0.025 V
  RC = 10000 ohm
  REE = 100000 ohm
  assumes: matched transistors, r_o neglected

In the worked example, I_tail = 1 mA, beta = 100, VT = 25 mV, RC = 10000 ohm, REE = 100000 ohm go through the equation above and give IC = 0.000495049505 A, gm = 0.0198019802 S, Ad_diff = -198.019802, Ad_se = -99.00990099. It applies only when matched transistors, r_o neglected: outside that it says what is wrong instead of returning a number.

BJT dual-supply emitter bias: Q-point — elx_bjt_emitter_bias

The Q-point of a transistor with its base returned to ground through RB and its emitter returned to a negative supply -VEE through RE (emitter bias).

Applies when: VEE > VBE; active region: VCE >= 0.2 V.

$ electronics-engineering solve elx_bjt_emitter_bias "VCC=10 V" "VEE=10 V" "RB=10000 ohm" "RC=4700 ohm" "RE=10000 ohm" beta=100 "VBE=0.7 V"
IB = 9.117647059e-06 A
IC = 0.0009117647059 A
IE = 0.0009208823529 A
VB = -0.09117647059 V
VE = -0.7911764706 V
VC = 5.714705882 V
VCE = 6.505882353 V
  by: BJT dual-supply emitter bias: Q-point  (IE = (VEE - VBE)/(RE + RB/(beta + 1)); VB = -IB RB; VE = VB - VBE; VC = VCC - IC RC)
  VCC = 10 V
  VEE = 10 V
  RB = 10000 ohm
  RC = 4700 ohm
  RE = 10000 ohm
  beta = 100
  VBE = 0.7 V
  assumes: VEE > VBE; active region: VCE >= 0.2 V

In the worked example, VCC = 10 V, VEE = 10 V, RB = 10000 ohm, RC = 4700 ohm, RE = 10000 ohm, beta = 100, VBE = 0.7 V go through the equation above and give IB = 9.117647059e-06 A, IC = 0.0009117647059 A, IE = 0.0009208823529 A, VB = -0.09117647059 V. It applies only when VEE > VBE; active region: VCE >= 0.2 V: outside that it says what is wrong instead of returning a number.

BJT fixed (base-resistor) bias: Q-point — elx_bjt_fixed_bias

The quiescent base and collector currents and the collector-emitter voltage of a common-emitter stage biased by a single base resistor from the supply.

Applies when: active region: VCE >= 0.2 V (otherwise refused as saturated).

$ electronics-engineering solve elx_bjt_fixed_bias "VCC=12 V" "RB=470000 ohm" "RC=2200 ohm" beta=100 "VBE=0.7 V"
IB = 2.404255319e-05 A
IC = 0.002404255319 A
IE = 0.002428297872 A
VCE = 6.710638298 V
  by: BJT fixed (base-resistor) bias: Q-point  (IB = (VCC - VBE)/RB; IC = beta IB; VCE = VCC - IC RC)
  VCC = 12 V
  RB = 470000 ohm
  RC = 2200 ohm
  beta = 100
  VBE = 0.7 V
  assumes: active region: VCE >= 0.2 V (otherwise refused as saturated)

In the worked example, VCC = 12 V, RB = 470000 ohm, RC = 2200 ohm, beta = 100, VBE = 0.7 V go through the equation above and give IB = 2.404255319e-05 A, IC = 0.002404255319 A, IE = 0.002428297872 A, VCE = 6.710638298 V. It applies only when active region: VCE >= 0.2 V (otherwise refused as saturated): outside that it says what is wrong instead of returning a number.

BJT small-signal (hybrid-pi) parameters — elx_bjt_small_signal_parameters

The transconductance gm, the input resistance r_pi, the emitter resistance r_e, the output resistance r_o (Early voltage) and the intrinsic gain of a bipolar transistor at its bias current.

Applies when: IC, beta, VT, VA > 0; active region.

$ electronics-engineering solve elx_bjt_small_signal_parameters "IC=1 mA" beta=100 "VT=25 mV" "VA=100 V"
gm = 0.04 S
r_pi = 2500 ohm
r_e = 24.75247525 ohm
r_o = 100000 ohm
A0 = 4000
  by: BJT small-signal (hybrid-pi) parameters  (gm = IC/VT; r_pi = beta/gm; r_e = alpha/gm; r_o = VA/IC; A0 = VA/VT)
  IC = 0.001 A
  beta = 100
  VT = 0.025 V
  VA = 100 V
  assumes: IC, beta, VT, VA > 0; active region

In the worked example, IC = 1 mA, beta = 100, VT = 25 mV, VA = 100 V go through the equation above and give gm = 0.04 S, r_pi = 2500 ohm, r_e = 24.75247525 ohm, r_o = 100000 ohm. It applies only when IC, beta, VT, VA > 0; active region: outside that it says what is wrong instead of returning a number.

BJT terminal currents from beta — elx_bjt_current_relations

The collector and emitter currents and the common-base current gain alpha of a bipolar transistor in the active region from its base current and beta.

Applies when: IB > 0, beta > 0; active region.

$ electronics-engineering solve elx_bjt_current_relations "IB=20 uA" beta=100
IC = 0.002 A
IE = 0.00202 A
alpha = 0.9900990099
  by: BJT terminal currents from beta  (IC = beta IB; IE = (beta + 1) IB; alpha = beta/(beta + 1))
  IB = 2e-05 A
  beta = 100
  assumes: IB > 0, beta > 0; active region

In the worked example, IB = 20 uA, beta = 100 go through the equation above and give IC = 0.002 A, IE = 0.00202 A, alpha = 0.9900990099. It applies only when IB > 0, beta > 0; active region: outside that it says what is wrong instead of returning a number.

BJT voltage-divider bias: exact Q-point — elx_bjt_voltage_divider_bias

The Q-point (base, collector and emitter currents, node voltages and VCE) of a common-emitter stage with a base voltage divider and an emitter resistor, by the exact Thevenin analysis (base current included).

Applies when: VTH > VBE; active region: VCE >= 0.2 V.

$ electronics-engineering solve elx_bjt_voltage_divider_bias "VCC=12 V" "R1=47000 ohm" "R2=10000 ohm" "RC=2200 ohm" "RE=470 ohm" beta=150 "VBE=0.7 V"
VTH = 2.105263158 V
RTH = 8245.614035 ohm
IB = 1.773972436e-05 A
IC = 0.002660958654 A
IE = 0.002678698378 A
VB = 1.958988238 V
VE = 1.258988238 V
VC = 6.145890962 V
VCE = 4.886902724 V
  by: BJT voltage-divider bias: exact Q-point  (VTH = VCC R2/(R1 + R2); RTH = R1 || R2; IB = (VTH - VBE)/(RTH + (beta + 1) RE); VCE = VCC - IC RC - IE RE)
  VCC = 12 V
  R1 = 47000 ohm
  R2 = 10000 ohm
  RC = 2200 ohm
  RE = 470 ohm
  beta = 150
  VBE = 0.7 V
  assumes: VTH > VBE; active region: VCE >= 0.2 V

In the worked example, VCC = 12 V, R1 = 47000 ohm, R2 = 10000 ohm, RC = 2200 ohm, RE = 470 ohm, beta = 150, VBE = 0.7 V go through the equation above and give VTH = 2.105263158 V, RTH = 8245.614035 ohm, IB = 1.773972436e-05 A, IC = 0.002660958654 A. It applies only when VTH > VBE; active region: VCE >= 0.2 V: outside that it says what is wrong instead of returning a number.

Common-base amplifier — elx_common_base_amplifier

The voltage gain (emitter to collector and source to load), the low input resistance and the output resistance of a common-base stage (hybrid-pi model, r_o neglected).

Applies when: r_o neglected; base at signal ground.

$ electronics-engineering solve elx_common_base_amplifier "IC=1 mA" beta=100 "VT=25 mV" "RC=5000 ohm" "RL=5000 ohm" "RE=10000 ohm" "Rsig=50 ohm"
Av = 100
Rin = 24.69135802 ohm
Rout = 5000 ohm
Gv = 33.05785124
  by: Common-base amplifier  (Av = gm (RC || RL); Rin = RE || r_e with r_e = alpha/gm; Gv = Av Rin/(Rin + Rsig))
  IC = 0.001 A
  beta = 100
  VT = 0.025 V
  RC = 5000 ohm
  RL = 5000 ohm
  RE = 10000 ohm
  Rsig = 50 ohm
  assumes: r_o neglected; base at signal ground

In the worked example, IC = 1 mA, beta = 100, VT = 25 mV, RC = 5000 ohm, RL = 5000 ohm, RE = 10000 ohm, Rsig = 50 ohm go through the equation above and give Av = 100, Rin = 24.69135802 ohm, Rout = 5000 ohm, Gv = 33.05785124. It applies only when r_o neglected; base at signal ground: outside that it says what is wrong instead of returning a number.

Common-collector (emitter-follower) amplifier — elx_common_collector_amplifier

The voltage gain, input resistance and output resistance of an emitter follower, including the source resistance reflected into the emitter (hybrid-pi model, r_o neglected).

Applies when: r_o neglected.

$ electronics-engineering solve elx_common_collector_amplifier "IC=5 mA" beta=100 "VT=25 mV" "RE=1000 ohm" "RL=1000 ohm" "RB=100000 ohm" "Rsig=10000 ohm"
Av = 0.9901960784
Rin = 33774.83444 ohm
Rout = 86.7242088 ohm
Gv = 0.7639939486
  by: Common-collector (emitter-follower) amplifier  (Av = (beta + 1)(RE || RL)/(r_pi + (beta + 1)(RE || RL)); Rout = RE || (r_pi + Rsig || RB)/(beta + 1))
  IC = 0.005 A
  beta = 100
  VT = 0.025 V
  RE = 1000 ohm
  RL = 1000 ohm
  RB = 100000 ohm
  Rsig = 10000 ohm
  assumes: r_o neglected

In the worked example, IC = 5 mA, beta = 100, VT = 25 mV, RE = 1000 ohm, RL = 1000 ohm, RB = 100000 ohm, Rsig = 10000 ohm go through the equation above and give Av = 0.9901960784, Rin = 33774.83444 ohm, Rout = 86.7242088 ohm, Gv = 0.7639939486. It applies only when r_o neglected: outside that it says what is wrong instead of returning a number.

Common-emitter amplifier: gain, input and output resistance — elx_common_emitter_amplifier

The voltage gain (base to collector and source to load), the input and output resistances of a common-emitter stage with an optional unbypassed emitter resistance, from the bias current (hybrid-pi model, r_o neglected).

Applies when: r_o neglected; coupling and bypass capacitors short at signal frequency.

$ electronics-engineering solve elx_common_emitter_amplifier "IC=1 mA" beta=100 "VT=25 mV" "RC=5000 ohm" "RL=10000 ohm" "RE1=0 ohm" "RB=20000 ohm" "Rsig=1000 ohm"
gm = 0.04 S
r_pi = 2500 ohm
Av = -133.3333333
Rin = 2222.222222 ohm
Rout = 5000 ohm
Gv = -91.95402299
  by: Common-emitter amplifier: gain, input and output resistance  (Av = -beta (RC || RL)/(r_pi + (beta + 1) RE1); Rin = RB || (r_pi + (beta + 1) RE1); Gv = Av Rin/(Rin + Rsig))
  IC = 0.001 A
  beta = 100
  VT = 0.025 V
  RC = 5000 ohm
  RL = 10000 ohm
  RE1 = 0 ohm
  RB = 20000 ohm
  Rsig = 1000 ohm
  assumes: r_o neglected; coupling and bypass capacitors short at signal frequency

In the worked example, IC = 1 mA, beta = 100, VT = 25 mV, RC = 5000 ohm, RL = 10000 ohm, RE1 = 0 ohm, RB = 20000 ohm, Rsig = 1000 ohm go through the equation above and give gm = 0.04 S, r_pi = 2500 ohm, Av = -133.3333333, Rin = 2222.222222 ohm. It applies only when r_o neglected; coupling and bypass capacitors short at signal frequency: outside that it says what is wrong instead of returning a number.

Common-emitter high-frequency cutoff: Miller effect and open-circuit time constants — elx_miller_high_cutoff

The Miller capacitance, the upper -3 dB frequency of a common-emitter (or common-source) stage by the Miller approximation, and the open-circuit time-constant estimate that also counts the output side of Cmu.

Applies when: mid-band gain unchanged by the capacitors; dominant-pole estimate.

$ electronics-engineering solve elx_miller_high_cutoff "gm=40 mS" "r_pi=2500 ohm" "Cpi=10 pF" "Cmu=2 pF" "RLp=2500 ohm" "Rsigp=1000 ohm"
A_mid = -100
C_M = 2.02e-10 F
R_pi_eq = 714.2857143 ohm
f_H_miller = 1051023.209 Hz
tau_oc = 1.564285714e-07 s
f_H_octc = 1017428.86 Hz
  by: Common-emitter high-frequency cutoff: Miller effect and open-circuit time constants  (C_M = Cmu (1 + gm RL'); f_H = 1/(2 pi (r_pi || Rsig')(Cpi + C_M)); tau = Cpi R' + Cmu (R' + RL' + gm R' RL'))
  gm = 0.04 S
  r_pi = 2500 ohm
  Cpi = 1e-11 F
  Cmu = 2e-12 F
  RLp = 2500 ohm
  Rsigp = 1000 ohm
  assumes: mid-band gain unchanged by the capacitors; dominant-pole estimate

In the worked example, gm = 40 mS, r_pi = 2500 ohm, Cpi = 10 pF, Cmu = 2 pF, RLp = 2500 ohm, Rsigp = 1000 ohm go through the equation above and give A_mid = -100, C_M = 2.02e-10 F, R_pi_eq = 714.2857143 ohm, f_H_miller = 1051023.209 Hz. It applies only when mid-band gain unchanged by the capacitors; dominant-pole estimate: outside that it says what is wrong instead of returning a number.

Common-emitter low-frequency cutoff by short-circuit time constants — elx_low_frequency_cutoff

The resistance seen by each coupling and bypass capacitor of a common-emitter amplifier and the lower -3 dB frequency estimated as the sum of the short-circuit pole frequencies (r_o neglected).

Applies when: short-circuit time-constant estimate; r_o neglected.

$ electronics-engineering solve elx_low_frequency_cutoff "Rsig=1000 ohm" "RB=20000 ohm" "r_pi=2500 ohm" beta=100 "RE=1000 ohm" "RC=5000 ohm" "RL=10000 ohm" "C1=10 uF" "C2=10 uF" "CE=100 uF"
R_C1 = 3222.222222 ohm
R_CE = 33.05219968 ohm
R_C2 = 15000 ohm
f_C1 = 4.939291337 Hz
f_CE = 48.15260244 Hz
f_C2 = 1.061032954 Hz
f_L = 54.15292673 Hz
  by: Common-emitter low-frequency cutoff by short-circuit time constants  (R_C1 = Rsig + RB || r_pi; R_CE = RE || (r_pi + Rsig || RB)/(beta + 1); R_C2 = RC + RL; f_L = sum 1/(2 pi R C))
  Rsig = 1000 ohm
  RB = 20000 ohm
  r_pi = 2500 ohm
  beta = 100
  RE = 1000 ohm
  RC = 5000 ohm
  RL = 10000 ohm
  C1 = 1e-05 F
  C2 = 1e-05 F
  CE = 0.0001 F
  assumes: short-circuit time-constant estimate; r_o neglected

In the worked example, Rsig = 1000 ohm, RB = 20000 ohm, r_pi = 2500 ohm, beta = 100, RE = 1000 ohm, RC = 5000 ohm, RL = 10000 ohm, C1 = 10 uF, C2 = 10 uF, CE = 100 uF go through the equation above and give R_C1 = 3222.222222 ohm, R_CE = 33.05219968 ohm, R_C2 = 15000 ohm, f_C1 = 4.939291337 Hz. It applies only when short-circuit time-constant estimate; r_o neglected: outside that it says what is wrong instead of returning a number.

Wilson current mirror output current — elx_wilson_current_mirror

The output current of a three-transistor Wilson current mirror and its small base-current error, 2/(beta^2 + 2 beta + 2).

Applies when: matched transistors, Early effect neglected.

$ electronics-engineering solve elx_wilson_current_mirror "Iref=1 mA" beta=100
Iout = 0.00099980396 A
ratio = 0.99980396
error = 0.0001960399922
  by: Wilson current mirror output current  (Iout = Iref (1 - 2/(beta^2 + 2 beta + 2)))
  Iref = 0.001 A
  beta = 100
  assumes: matched transistors, Early effect neglected

In the worked example, Iref = 1 mA, beta = 100 go through the equation above and give Iout = 0.00099980396 A, ratio = 0.99980396, error = 0.0001960399922. It applies only when matched transistors, Early effect neglected: outside that it says what is wrong instead of returning a number.

CMOS (2)

CMOS gate propagation delay (switch-resistor model) — elx_cmos_propagation_delay

The high-to-low and low-to-high propagation delays (50 % points) and their average for a CMOS gate modelled as switched equivalent resistances driving a load capacitance.

Applies when: step input, RC switch model.

$ electronics-engineering solve elx_cmos_propagation_delay "Rn=10000 ohm" "Rp=20000 ohm" "CL=100 fF"
tpHL = 6.931471806e-10 s
tpLH = 1.386294361e-09 s
tp = 1.039720771e-09 s
  by: CMOS gate propagation delay (switch-resistor model)  (tpHL = ln 2 Rn CL; tpLH = ln 2 Rp CL; tp = (tpHL + tpLH)/2)
  Rn = 10000 ohm
  Rp = 20000 ohm
  CL = 1e-13 F
  assumes: step input, RC switch model

In the worked example, Rn = 10000 ohm, Rp = 20000 ohm, CL = 100 fF go through the equation above and give tpHL = 6.931471806e-10 s, tpLH = 1.386294361e-09 s, tp = 1.039720771e-09 s. It applies only when step input, RC switch model: outside that it says what is wrong instead of returning a number.

CMOS inverter switching threshold VM — elx_cmos_switching_threshold

The switching threshold of a CMOS inverter (input = output, both transistors saturated) from the supply, the two threshold voltages and the two transconductance parameters.

Applies when: Vtn + |Vtp| < VDD; lambda neglected.

$ electronics-engineering solve elx_cmos_switching_threshold "VDD=2.5 V" "Vtn=0.4 V" "Vtp=0.4 V" "kn=0.1 mA/V^2" "kp=0.1 mA/V^2"
r = 1
VM = 1.25 V
  by: CMOS inverter switching threshold VM  (VM = (Vtn + r (VDD - |Vtp|))/(1 + r), r = sqrt(kp/kn))
  VDD = 2.5 V
  Vtn = 0.4 V
  Vtp = 0.4 V
  kn = 0.0001 A/V^2
  kp = 0.0001 A/V^2
  assumes: Vtn + |Vtp| < VDD; lambda neglected

In the worked example, VDD = 2.5 V, Vtn = 0.4 V, Vtp = 0.4 V, kn = 0.1 mA/V^2, kp = 0.1 mA/V^2 go through the equation above and give r = 1, VM = 1.25 V. It applies only when Vtn + |Vtp| < VDD; lambda neglected: outside that it says what is wrong instead of returning a number.

Data converters (9)

ADC output code, LSB and quantisation error — elx_adc_code

The output code (decimal and binary) of an ideal unipolar truncating n-bit ADC for an input voltage, the LSB size, the voltage the code represents and the quantisation error.

Applies when: 0 <= Vin <= Vref; 1 <= n <= 16.

$ electronics-engineering solve elx_adc_code "Vin=3.2 V" "Vref=5 V" n=8
code = 163
bits = 10100011
LSB = 0.01953125 V
V_code = 3.18359375 V
error = 0.01640625 V
  by: ADC output code, LSB and quantisation error  (code = floor(Vin 2^n/Vref), at most 2^n - 1; LSB = Vref/2^n)
  Vin = 3.2 V
  Vref = 5 V
  assumes: 0 <= Vin <= Vref; 1 <= n <= 16

In the worked example, Vin = 3.2 V, Vref = 5 V, n = 8 go through the equation above and give code = 163, bits = 10100011, LSB = 0.01953125 V, V_code = 3.18359375 V. It applies only when 0 <= Vin <= Vref; 1 <= n <= 16: outside that it says what is wrong instead of returning a number.

ADC quantisation SNR with oversampling — elx_adc_quantization_snr

The signal-to-quantisation-noise ratio of an ideal n-bit converter for a sine input (6.02 n + 1.76 dB at full scale), with an oversampling ratio and a reduced amplitude, and the in-band noise in LSB.

Applies when: uniform quantisation noise, white over Nyquist; OSR >= 1.

$ electronics-engineering solve elx_adc_quantization_snr n=12
SNR_dB = 74.00811155
noise_rms_lsb = 0.2886751346
SNR_full_scale_dB = 74.00811155
  by: ADC quantisation SNR with oversampling  (SNR = 20 log10(A 2^n sqrt(1.5)) + 10 log10(OSR) = 6.02 n + 1.76 + 20 log10 A + 10 log10 OSR)
  assumes: uniform quantisation noise, white over Nyquist; OSR >= 1

In the worked example, n = 12 go through the equation above and give SNR_dB = 74.00811155, noise_rms_lsb = 0.2886751346, SNR_full_scale_dB = 74.00811155. It applies only when uniform quantisation noise, white over Nyquist; OSR >= 1: outside that it says what is wrong instead of returning a number.

Binary-weighted resistor DAC — elx_dac_binary_weighted

The output voltage and summing current of a binary-weighted resistor DAC with an inverting op-amp (MSB resistor R, each lower bit doubling it) and the largest resistor needed.

Applies when: ideal switches and op-amp.

$ electronics-engineering solve elx_dac_binary_weighted n=4 code=10 "Vref=5 V" "R=10000 ohm" "Rf=5000 ohm"
Vout = -3.125 V
I_total = 0.000625 A
R_LSB = 80000 ohm
  by: Binary-weighted resistor DAC  (I = Vref D/(R 2^(n-1)); Vout = -Rf I)
  Vref = 5 V
  R = 10000 ohm
  Rf = 5000 ohm
  assumes: ideal switches and op-amp

In the worked example, n = 4, code = 10, Vref = 5 V, R = 10000 ohm, Rf = 5000 ohm go through the equation above and give Vout = -3.125 V, I_total = 0.000625 A, R_LSB = 80000 ohm. It applies only when ideal switches and op-amp: outside that it says what is wrong instead of returning a number.

DAC output voltage (R-2R or any binary DAC) — elx_dac_output

The output voltage of an ideal n-bit unipolar DAC for a code, Vout = Vref D/2^n, its step size and its full-scale output.

Applies when: 0 <= code <= 2^n - 1.

$ electronics-engineering solve elx_dac_output n=8 code=200 "Vref=5 V"
Vout = 3.90625 V
LSB = 0.01953125 V
V_full_scale = 4.98046875 V
  by: DAC output voltage (R-2R or any binary DAC)  (Vout = Vref D/2^n; full scale Vref (2^n - 1)/2^n)
  Vref = 5 V
  assumes: 0 <= code <= 2^n - 1

In the worked example, n = 8, code = 200, Vref = 5 V go through the equation above and give Vout = 3.90625 V, LSB = 0.01953125 V, V_full_scale = 4.98046875 V. It applies only when 0 <= code <= 2^n - 1: outside that it says what is wrong instead of returning a number.

Dual-slope integrating ADC — elx_dual_slope_adc

The fixed integration time, the de-integration time and count, and the peak integrator voltage of a dual-slope ADC.

Applies when: 0 < Vin <= Vref.

$ electronics-engineering solve elx_dual_slope_adc "Vin=0.5 V" "Vref=1 V" N1=1000 "fclk=100000 Hz" "R=100000 ohm" "C=0.1 uF"
T1 = 0.01 s
T2 = 0.005 s
N2 = 500
V_peak = 0.5 V
  by: Dual-slope integrating ADC  (T1 = N1/fclk; T2 = T1 Vin/Vref; N2 = N1 Vin/Vref; V_peak = Vin T1/(R C))
  Vin = 0.5 V
  Vref = 1 V
  fclk = 100000 Hz
  R = 100000 ohm
  C = 1e-07 F
  assumes: 0 < Vin <= Vref

In the worked example, Vin = 0.5 V, Vref = 1 V, N1 = 1000, fclk = 100000 Hz, R = 100000 ohm, C = 0.1 uF go through the equation above and give T1 = 0.01 s, T2 = 0.005 s, N2 = 500, V_peak = 0.5 V. It applies only when 0 < Vin <= Vref: outside that it says what is wrong instead of returning a number.

Effective number of bits (ENOB) from SINAD — elx_adc_enob

The effective number of bits of a converter from its measured SINAD (IEEE 1241: ENOB = (SINAD - 1.76)/6.02) and the bits lost against its nominal resolution.

Applies when: full-scale sine test.

$ electronics-engineering solve elx_adc_enob SINAD=74 n=14
ENOB = 12
bits_lost = 2
  by: Effective number of bits (ENOB) from SINAD  (ENOB = (SINAD - 1.76)/6.02)
  SINAD = 74
  assumes: full-scale sine test

In the worked example, SINAD = 74, n = 14 go through the equation above and give ENOB = 12, bits_lost = 2. It applies only when full-scale sine test: outside that it says what is wrong instead of returning a number.

Sample-and-hold droop — elx_sample_hold_droop

The droop rate I/C of a sample-and-hold capacitor discharged by a leakage current, the droop over a hold time (in volts and LSB) and the longest hold that keeps the droop within half an LSB of an n-bit converter.

Applies when: constant leakage current.

$ electronics-engineering solve elx_sample_hold_droop "I_leak=1 nA" "C=1 nF" "t_hold=10 us" "Vref=5 V" n=12
droop_rate = 1 V/s
droop = 1e-05 V
droop_lsb = 0.008192
t_max_half_lsb = 0.0006103515625 s
  by: Sample-and-hold droop  (dV/dt = I/C; dV = I t/C; t_max = (Vref/2^(n+1)) C/I)
  I_leak = 1e-09 A
  C = 1e-09 F
  t_hold = 1e-05 s
  Vref = 5 V
  assumes: constant leakage current

In the worked example, I_leak = 1 nA, C = 1 nF, t_hold = 10 us, Vref = 5 V, n = 12 go through the equation above and give droop_rate = 1 V/s, droop = 1e-05 V, droop_lsb = 0.008192, t_max_half_lsb = 0.0006103515625 s. It applies only when constant leakage current: outside that it says what is wrong instead of returning a number.

SNR limit from sampling-clock (aperture) jitter — elx_aperture_jitter_snr

The SNR limit -20 log10(2 pi f tj) set by rms sampling-clock jitter for a full-scale sine, combined with the quantisation SNR of an n-bit converter into a total SNR and effective bits.

Applies when: full-scale sine; jitter and quantisation noise uncorrelated.

$ electronics-engineering solve elx_aperture_jitter_snr "f=100000000 Hz" "tj=1 ps" n=14
SNR_jitter_dB = 64.03640263
SNR_quant_dB = 86.04931138
SNR_total_dB = 64.00916741
ENOB_total = 10.34039326
  by: SNR limit from sampling-clock (aperture) jitter  (SNR_j = -20 log10(2 pi f tj); SNR_q = 6.02 n + 1.76; noise powers add)
  f = 100000000 Hz
  tj = 1e-12 s
  assumes: full-scale sine; jitter and quantisation noise uncorrelated

In the worked example, f = 100000000 Hz, tj = 1 ps, n = 14 go through the equation above and give SNR_jitter_dB = 64.03640263, SNR_quant_dB = 86.04931138, SNR_total_dB = 64.00916741, ENOB_total = 10.34039326. It applies only when full-scale sine; jitter and quantisation noise uncorrelated: outside that it says what is wrong instead of returning a number.

Successive-approximation (SAR) ADC conversion — elx_sar_conversion

The bit-by-bit trial voltages, the final code (decimal and binary) and the DAC voltage of an ideal n-bit successive-approximation ADC converting an input.

Applies when: 0 <= Vin < Vref.

$ electronics-engineering solve elx_sar_conversion "Vin=3.2 V" "Vref=5 V" n=4
code = 10
bits = 1010
trials = [2.5,3.75,3.125,3.4375]
V_dac = 3.125 V
cycles = 4
  by: Successive-approximation (SAR) ADC conversion  (for each bit from the MSB: set it, keep it if Vin >= DAC(trial); LSB = Vref/2^n)
  Vin = 3.2 V
  Vref = 5 V
  assumes: 0 <= Vin < Vref

In the worked example, Vin = 3.2 V, Vref = 5 V, n = 4 go through the equation above and give code = 10, bits = 1010, trials = [2.5, 3.75, 3.125, 3.4375], V_dac = 3.125 V. It applies only when 0 <= Vin < Vref: outside that it says what is wrong instead of returning a number.

Diodes (8)

Capacitor-input filter: ripple voltage and DC output — elx_capacitor_filter_ripple

The peak-to-peak ripple, the DC output, the RMS ripple and the ripple factor of a rectifier with a smoothing capacitor and resistive load (small-ripple approximation).

Applies when: Vr < Vp (small ripple).

$ electronics-engineering solve elx_capacitor_filter_ripple "Vp=16.3 V" "f=60 Hz" "RL=500 ohm" "C=1000 uF" circuit=full-wave
f_ripple = 120 Hz
Vr = 0.2716666667 V
Vdc = 16.16416667 V
Vr_rms = 0.07842341156 V
ripple_factor = 0.004851682934
  by: Capacitor-input filter: ripple voltage and DC output  (Vr = Vp/(f_r RL C); Vdc = Vp - Vr/2; Vr,rms = Vr/(2 sqrt 3))
  Vp = 16.3 V
  f = 60 Hz
  RL = 500 ohm
  C = 0.001 F
  circuit = full-wave
  assumes: Vr < Vp (small ripple)

In the worked example, Vp = 16.3 V, f = 60 Hz, RL = 500 ohm, C = 1000 uF, circuit = full-wave go through the equation above and give f_ripple = 120 Hz, Vr = 0.2716666667 V, Vdc = 16.16416667 V, Vr_rms = 0.07842341156 V. It applies only when Vr < Vp (small ripple): outside that it says what is wrong instead of returning a number.

Diode current from the Shockley equation — elx_shockley_diode_current

The current of a pn-junction diode at a terminal voltage from its saturation current, ideality factor and temperature (forward or reverse).

Applies when: Is, n, T > 0.

$ electronics-engineering solve elx_shockley_diode_current "Is=1e-14 A" n=1 "VD=0.65 V" "T=300 K"
ID = 0.0008308438348 A
VT = 0.02585199979 V
  by: Diode current from the Shockley equation  (ID = Is (exp(VD/(n VT)) - 1), VT = kT/q)
  Is = 1e-14 A
  n = 1
  VD = 0.65 V
  T = 300 K
  assumes: Is, n, T > 0

In the worked example, Is = 1e-14 A, n = 1, VD = 0.65 V, T = 300 K go through the equation above and give ID = 0.0008308438348 A, VT = 0.02585199979 V. It applies only when Is, n, T > 0: outside that it says what is wrong instead of returning a number.

Diode voltage for a given current — elx_diode_voltage

The voltage across a pn-junction diode carrying a given current (the inverse of the Shockley equation).

Applies when: ID > -Is; Is, n, T > 0.

$ electronics-engineering solve elx_diode_voltage "ID=0.001 A" "Is=1e-14 A" n=1 "T=300 K"
VD = 0.6547907227 V
VT = 0.02585199979 V
  by: Diode voltage for a given current  (VD = n VT ln(1 + ID/Is))
  ID = 0.001 A
  Is = 1e-14 A
  n = 1
  T = 300 K
  assumes: ID > -Is; Is, n, T > 0

In the worked example, ID = 0.001 A, Is = 1e-14 A, n = 1, T = 300 K go through the equation above and give VD = 0.6547907227 V, VT = 0.02585199979 V. It applies only when ID > -Is; Is, n, T > 0: outside that it says what is wrong instead of returning a number.

LED series (current-limiting) resistor — elx_led_series_resistor

The current-limiting resistor for one LED or a string of LEDs in series at a chosen forward current, and the power in the resistor and in the LEDs.

Applies when: Vs > n Vf; If > 0.

$ electronics-engineering solve elx_led_series_resistor "Vs=5 V" "Vf=2 V" "If=20 mA"
R = 150 ohm
P_R = 0.06 W
P_LED = 0.04 W
  by: LED series (current-limiting) resistor  (R = (Vs - n Vf)/If; P_R = If^2 R)
  Vs = 5 V
  Vf = 2 V
  If = 0.02 A
  assumes: Vs > n Vf; If > 0

In the worked example, Vs = 5 V, Vf = 2 V, If = 20 mA go through the equation above and give R = 150 ohm, P_R = 0.06 W, P_LED = 0.04 W. It applies only when Vs > n Vf; If > 0: outside that it says what is wrong instead of returning a number.

Operating point of a diode in series with a resistor (exact) — elx_diode_operating_point

The current and voltage of a forward-biased diode fed from a DC source through a resistor, solving the Shockley equation and Kirchhoff's voltage law together (no constant-drop approximation).

Applies when: VS > 0 (forward bias); R, Is, n, T > 0.

$ electronics-engineering solve elx_diode_operating_point "VS=5 V" "R=1000 ohm" "Is=1e-14 A" n=1 "T=300 K"
ID = 0.004307456373 A
VD = 0.6925436275 V
P_D = 0.002983101461 W
  by: Operating point of a diode in series with a resistor (exact)  (solve VS = ID R + n VT ln(1 + ID/Is) (bisection on VD))
  VS = 5 V
  R = 1000 ohm
  Is = 1e-14 A
  n = 1
  T = 300 K
  assumes: VS > 0 (forward bias); R, Is, n, T > 0

In the worked example, VS = 5 V, R = 1000 ohm, Is = 1e-14 A, n = 1, T = 300 K go through the equation above and give ID = 0.004307456373 A, VD = 0.6925436275 V, P_D = 0.002983101461 W. It applies only when VS > 0 (forward bias); R, Is, n, T > 0: outside that it says what is wrong instead of returning a number.

Rectifier output: average, RMS, ripple factor and PIV — elx_rectifier_averages

The DC (average) and RMS output voltage, ripple factor, peak inverse voltage and conduction angle of an unfiltered half-wave, bridge or centre-tapped full-wave rectifier with a constant diode drop (0 V for ideal diodes).

Applies when: diode drops below Vm; resistive load, no filter.

$ electronics-engineering solve elx_rectifier_averages "Vm=10 V" circuit=half-wave "Von=0 V"
Vp_out = 10 V
Vdc = 3.183098862 V
Vrms = 5 V
ripple_factor = 1.211363323
PIV = 10 V
conduction_deg = 180
  by: Rectifier output: average, RMS, ripple factor and PIV  (output max(0, Vm|sin| - V) with V = Von (2 Von for a bridge); averages integrated exactly; PIV Vm, Vm - Von, 2Vm - Von)
  Vm = 10 V
  Von = 0 V
  circuit = half-wave
  assumes: diode drops below Vm; resistive load, no filter

In the worked example, Vm = 10 V, circuit = half-wave, Von = 0 V go through the equation above and give Vp_out = 10 V, Vdc = 3.183098862 V, Vrms = 5 V, ripple_factor = 1.211363323. It applies only when diode drops below Vm; resistive load, no filter: outside that it says what is wrong instead of returning a number.

Zener regulator design: series resistor and Zener rating — elx_zener_series_resistor_design

The largest series resistance that keeps a Zener regulator in regulation at the lowest input and largest load, and the resulting worst-case Zener current and power (highest input, smallest load) and resistor power.

Applies when: Vin_min > Vz; Vin_max >= Vin_min, IL_max >= IL_min >= 0.

$ electronics-engineering solve elx_zener_series_resistor_design "Vin_min=12 V" "Vin_max=15 V" "Vz=9.1 V" "IL_min=0 mA" "IL_max=50 mA" "Iz_min=5 mA"
Rs_max = 52.72727273 ohm
Iz_max = 0.1118965517 A
Pz_max = 1.018258621 W
PRs_max = 0.6601896552 W
  by: Zener regulator design: series resistor and Zener rating  (Rs = (Vin,min - Vz)/(Iz,min + IL,max); Iz,max = (Vin,max - Vz)/Rs - IL,min; Pz = Vz Iz,max)
  Vin_min = 12 V
  Vin_max = 15 V
  Vz = 9.1 V
  IL_min = 0 A
  IL_max = 0.05 A
  Iz_min = 0.005 A
  assumes: Vin_min > Vz; Vin_max >= Vin_min, IL_max >= IL_min >= 0

In the worked example, Vin_min = 12 V, Vin_max = 15 V, Vz = 9.1 V, IL_min = 0 mA, IL_max = 50 mA, Iz_min = 5 mA go through the equation above and give Rs_max = 52.72727273 ohm, Iz_max = 0.1118965517 A, Pz_max = 1.018258621 W, PRs_max = 0.6601896552 W. It applies only when Vin_min > Vz; Vin_max >= Vin_min, IL_max >= IL_min >= 0: outside that it says what is wrong instead of returning a number.

Zener shunt regulator: load voltage and currents — elx_zener_regulator

The output voltage and the source, load and Zener currents and the Zener power of a Zener shunt regulator (series resistor, Zener across the load), with an optional Zener resistance.

Applies when: the Zener must be in breakdown: Vin RL/(Rs + RL) > Vz.

$ electronics-engineering solve elx_zener_regulator "Vin=20 V" "Rs=220 ohm" "Vz=10 V" "RL=1000 ohm"
Vout = 10 V
I_s = 0.04545454545 A
I_L = 0.01 A
I_z = 0.03545454545 A
P_z = 0.3545454545 W
  by: Zener shunt regulator: load voltage and currents  (ideal: Vout = Vz, Iz = (Vin - Vz)/Rs - Vz/RL; with rz: node equation at the load)
  Vin = 20 V
  Rs = 220 ohm
  Vz = 10 V
  RL = 1000 ohm
  assumes: the Zener must be in breakdown: Vin RL/(Rs + RL) > Vz

In the worked example, Vin = 20 V, Rs = 220 ohm, Vz = 10 V, RL = 1000 ohm go through the equation above and give Vout = 10 V, I_s = 0.04545454545 A, I_L = 0.01 A, I_z = 0.03545454545 A. It applies only when the Zener must be in breakdown: Vin RL/(Rs + RL) > Vz: outside that it says what is wrong instead of returning a number.

MOSFET (6)

Common-source amplifier with source degeneration and ro — elx_common_source_amplifier

The voltage gain, input and output resistances and overall gain of a common-source stage, exact with the transistor's output resistance ro and an optional unbypassed source resistor.

Applies when: gm, ro, RD, RL, RG, Rsig > 0; RS >= 0.

$ electronics-engineering solve elx_common_source_amplifier "gm=2 mS" "ro=100000 ohm" "RD=10000 ohm" "RL=10000 ohm" "RS=0 ohm" "RG=1000000 ohm" "Rsig=10000 ohm"
Av = -9.523809524
Rin = 1000000 ohm
Rout = 9090.909091 ohm
Gv = -9.42951438
  by: Common-source amplifier with source degeneration and ro  (Av = -gm ro RD'/(RD' + ro + RS (1 + gm ro)) with RD' = RD || RL; Rout = RD || (ro + RS(1 + gm ro)))
  gm = 0.002 S
  ro = 100000 ohm
  RD = 10000 ohm
  RL = 10000 ohm
  RS = 0 ohm
  RG = 1000000 ohm
  Rsig = 10000 ohm
  assumes: gm, ro, RD, RL, RG, Rsig > 0; RS >= 0

In the worked example, gm = 2 mS, ro = 100000 ohm, RD = 10000 ohm, RL = 10000 ohm, RS = 0 ohm, RG = 1000000 ohm, Rsig = 10000 ohm go through the equation above and give Av = -9.523809524, Rin = 1000000 ohm, Rout = 9090.909091 ohm, Gv = -9.42951438. It applies only when gm, ro, RD, RL, RG, Rsig > 0; RS >= 0: outside that it says what is wrong instead of returning a number.

MOSFET drain current (cutoff, triode, saturation) — elx_mosfet_drain_current

The operating region and drain current of an enhancement NMOS transistor by the square law: cutoff, triode or saturation with optional channel-length modulation (use magnitudes for PMOS).

Applies when: kn, Vt > 0; VDS >= 0; long-channel square law.

$ electronics-engineering solve elx_mosfet_drain_current "kn=2 mA/V^2" "Vt=1 V" "VGS=3 V" "VDS=5 V"
region = saturation
ID = 0.004 A
VOV = 2 V
VDS_sat = 2 V
  by: MOSFET drain current (cutoff, triode, saturation)  (cutoff VOV <= 0; triode VDS < VOV: ID = kn (VOV VDS - VDS^2/2); saturation: ID = (kn/2) VOV^2 (1 + lambda VDS))
  kn = 0.002 A/V^2
  Vt = 1 V
  VGS = 3 V
  VDS = 5 V
  assumes: kn, Vt > 0; VDS >= 0; long-channel square law

In the worked example, kn = 2 mA/V^2, Vt = 1 V, VGS = 3 V, VDS = 5 V go through the equation above and give region = saturation, ID = 0.004 A, VOV = 2 V, VDS_sat = 2 V. It applies only when kn, Vt > 0; VDS >= 0; long-channel square law: outside that it says what is wrong instead of returning a number.

MOSFET small-signal gm, ro and intrinsic gain — elx_mosfet_gm_ro

The overdrive voltage, gate-source voltage, transconductance gm = sqrt(2 kn ID), output resistance ro = 1/(lambda ID) and intrinsic gain of a MOSFET in saturation at a drain current.

Applies when: saturation; ID taken without the (1 + lambda VDS) factor.

$ electronics-engineering solve elx_mosfet_gm_ro "kn=2 mA/V^2" "ID=1 mA" "lam=0.01 1/V" "Vt=0.7 V"
VOV = 1 V
VGS = 1.7 V
gm = 0.002 S
r_o = 100000 ohm
A0 = 200
  by: MOSFET small-signal gm, ro and intrinsic gain  (VOV = sqrt(2 ID/kn); gm = sqrt(2 kn ID) = 2 ID/VOV; ro = 1/(lambda ID))
  kn = 0.002 A/V^2
  ID = 0.001 A
  lam = 0.01 1/V
  Vt = 0.7 V
  assumes: saturation; ID taken without the (1 + lambda VDS) factor

In the worked example, kn = 2 mA/V^2, ID = 1 mA, lam = 0.01 1/V, Vt = 0.7 V go through the equation above and give VOV = 1 V, VGS = 1.7 V, gm = 0.002 S, r_o = 100000 ohm. It applies only when saturation; ID taken without the (1 + lambda VDS) factor: outside that it says what is wrong instead of returning a number.

MOSFET threshold voltage with body effect — elx_mosfet_body_effect

The threshold voltage of a MOSFET whose source is above its body, Vt = Vt0 + gamma (sqrt(2 phiF + VSB) - sqrt(2 phiF)).

Applies when: VSB >= 0; uniform substrate doping.

$ electronics-engineering solve elx_mosfet_body_effect "Vt0=0.7 V" gamma=0.4 "phi2F=0.7 V" "VSB=3 V"
Vt = 1.134751352 V
dVt = 0.4347513519 V
  by: MOSFET threshold voltage with body effect  (Vt = Vt0 + gamma (sqrt(2 phiF + VSB) - sqrt(2 phiF)))
  Vt0 = 0.7 V
  gamma = 0.4
  phi2F = 0.7 V
  VSB = 3 V
  assumes: VSB >= 0; uniform substrate doping

In the worked example, Vt0 = 0.7 V, gamma = 0.4, phi2F = 0.7 V, VSB = 3 V go through the equation above and give Vt = 1.134751352 V, dVt = 0.4347513519 V. It applies only when VSB >= 0; uniform substrate doping: outside that it says what is wrong instead of returning a number.

MOSFET voltage-divider bias with source resistor: Q-point — elx_mosfet_divider_bias

The Q-point (gate voltage, VGS, drain current, node voltages and VDS) of an NMOS stage with a gate divider and a source resistor, solving the square law and the gate loop (the physical root), with a saturation check.

Applies when: VG > Vt; saturation: VDS >= VOV (otherwise refused); lambda neglected.

$ electronics-engineering solve elx_mosfet_divider_bias "VDD=15 V" "R1=1000000 ohm" "R2=500000 ohm" "RD=3300 ohm" "RS=1000 ohm" "kn=2 mA/V^2" "Vt=1.5 V"
VG = 5 V
VGS = 2.936491673 V
VOV = 1.436491673 V
ID = 0.002063508327 A
VS = 2.063508327 V
VD = 8.190422521 V
VDS = 6.126914194 V
  by: MOSFET voltage-divider bias with source resistor: Q-point  (VG = VDD R2/(R1 + R2); (kn RS/2) VOV^2 + VOV - (VG - Vt) = 0, positive root; ID = (kn/2) VOV^2)
  VDD = 15 V
  R1 = 1000000 ohm
  R2 = 500000 ohm
  RD = 3300 ohm
  RS = 1000 ohm
  kn = 0.002 A/V^2
  Vt = 1.5 V
  assumes: VG > Vt; saturation: VDS >= VOV (otherwise refused); lambda neglected

In the worked example, VDD = 15 V, R1 = 1000000 ohm, R2 = 500000 ohm, RD = 3300 ohm, RS = 1000 ohm, kn = 2 mA/V^2, Vt = 1.5 V go through the equation above and give VG = 5 V, VGS = 2.936491673 V, VOV = 1.436491673 V, ID = 0.002063508327 A. It applies only when VG > Vt; saturation: VDS >= VOV (otherwise refused); lambda neglected: outside that it says what is wrong instead of returning a number.

Source follower (common drain) — elx_source_follower

The voltage gain, input resistance, output resistance and overall gain of a MOSFET source follower, including ro.

Applies when: drain at signal ground.

$ electronics-engineering solve elx_source_follower "gm=2 mS" "ro=50000 ohm" "RS=2000 ohm" "RL=2000 ohm" "RG=1000000 ohm" "Rsig=10000 ohm"
Av = 0.6622516556
Rin = 1000000 ohm
Rout = 396.8253968 ohm
Gv = 0.6556947085
  by: Source follower (common drain)  (Av = gm R/(1 + gm R) with R = RS || RL || ro; Rout = RS || ro || 1/gm)
  gm = 0.002 S
  ro = 50000 ohm
  RS = 2000 ohm
  RL = 2000 ohm
  RG = 1000000 ohm
  Rsig = 10000 ohm
  assumes: drain at signal ground

In the worked example, gm = 2 mS, ro = 50000 ohm, RS = 2000 ohm, RL = 2000 ohm, RG = 1000000 ohm, Rsig = 10000 ohm go through the equation above and give Av = 0.6622516556, Rin = 1000000 ohm, Rout = 396.8253968 ohm, Gv = 0.6556947085. It applies only when drain at signal ground: outside that it says what is wrong instead of returning a number.

Op-amps (14)

Closed-loop bandwidth from the gain-bandwidth product — elx_closed_loop_bandwidth

The closed-loop gain, the noise gain 1 + Rf/R1 and the -3 dB bandwidth GBW/(noise gain) of an inverting or non-inverting amplifier built with a single-pole op-amp.

Applies when: single-pole op-amp with open-loop gain much larger than the closed-loop gain.

$ electronics-engineering solve elx_closed_loop_bandwidth "GBW=1000000 Hz" config=non-inverting "Rf=90000 ohm" "R1=10000 ohm"
G0 = 10
noise_gain = 10
f_3dB = 100000 Hz
  by: Closed-loop bandwidth from the gain-bandwidth product  (f_3dB = GBW/(1 + Rf/R1) for both configurations)
  GBW = 1000000 Hz
  Rf = 90000 ohm
  R1 = 10000 ohm
  config = non-inverting
  assumes: single-pole op-amp with open-loop gain much larger than the closed-loop gain

In the worked example, GBW = 1000000 Hz, config = non-inverting, Rf = 90000 ohm, R1 = 10000 ohm go through the equation above and give G0 = 10, noise_gain = 10, f_3dB = 100000 Hz. It applies only when single-pole op-amp with open-loop gain much larger than the closed-loop gain: outside that it says what is wrong instead of returning a number.

Inverting amplifier with finite open-loop gain — elx_inverting_amplifier_finite_gain

The exact closed-loop gain of an inverting amplifier built with an op-amp of finite open-loop gain A0, its relative gain error and output.

Applies when: A0 > 0 (ratio); infinite input resistance, zero output resistance.

$ electronics-engineering solve elx_inverting_amplifier_finite_gain "Rf=100000 ohm" "R1=1000 ohm" A0=10000 "Vin=0.01 V"
G = -99.000099
G_ideal = -100
Vout = -0.99000099 V
error = 0.009999009999
  by: Inverting amplifier with finite open-loop gain  (G = -(Rf/R1)/(1 + (1 + Rf/R1)/A0))
  Rf = 100000 ohm
  R1 = 1000 ohm
  A0 = 10000
  Vin = 0.01 V
  assumes: A0 > 0 (ratio); infinite input resistance, zero output resistance

In the worked example, Rf = 100000 ohm, R1 = 1000 ohm, A0 = 10000, Vin = 0.01 V go through the equation above and give G = -99.000099, G_ideal = -100, Vout = -0.99000099 V, error = 0.009999009999. It applies only when A0 > 0 (ratio); infinite input resistance, zero output resistance: outside that it says what is wrong instead of returning a number.

Inverting op-amp amplifier — elx_inverting_amplifier

The closed-loop gain, output voltage and input resistance of an ideal inverting amplifier.

Applies when: ideal op-amp, output not saturated.

$ electronics-engineering solve elx_inverting_amplifier "Rf=100000 ohm" "Rin=10000 ohm" "Vin=0.5 V"
G = -10
Vout = -5 V
Zin = 10000 ohm
  by: Inverting op-amp amplifier  (G = -Rf/Rin; Vout = G Vin; Zin = Rin)
  Rf = 100000 ohm
  Rin = 10000 ohm
  Vin = 0.5 V
  assumes: ideal op-amp, output not saturated

In the worked example, Rf = 100000 ohm, Rin = 10000 ohm, Vin = 0.5 V go through the equation above and give G = -10, Vout = -5 V, Zin = 10000 ohm. It applies only when ideal op-amp, output not saturated: outside that it says what is wrong instead of returning a number.

Inverting Schmitt trigger thresholds — elx_schmitt_trigger

The upper and lower switching thresholds, the hysteresis width and the centre of an inverting op-amp Schmitt trigger whose positive feedback divider (Rf from the output, R1 to a reference) sets the + input.

Applies when: VsatH > VsatL; input on the inverting terminal.

$ electronics-engineering solve elx_schmitt_trigger "Rf=90000 ohm" "R1=10000 ohm" "VsatH=12 V" "VsatL=-12 V" "Vref=0 V"
V_TH = 1.2 V
V_TL = -1.2 V
hysteresis = 2.4 V
center = 0 V
  by: Inverting Schmitt trigger thresholds  (V_T = (Vsat R1 + Vref Rf)/(R1 + Rf); hysteresis = (VsatH - VsatL) R1/(R1 + Rf))
  Rf = 90000 ohm
  R1 = 10000 ohm
  VsatH = 12 V
  VsatL = -12 V
  Vref = 0 V
  assumes: VsatH > VsatL; input on the inverting terminal

In the worked example, Rf = 90000 ohm, R1 = 10000 ohm, VsatH = 12 V, VsatL = -12 V, Vref = 0 V go through the equation above and give V_TH = 1.2 V, V_TL = -1.2 V, hysteresis = 2.4 V, center = 0 V. It applies only when VsatH > VsatL; input on the inverting terminal: outside that it says what is wrong instead of returning a number.

Inverting summing amplifier — elx_summing_amplifier

The output of an ideal inverting summing amplifier with several inputs, each through its own resistor, and the feedback current.

Applies when: one resistor per input; ideal op-amp.

$ electronics-engineering solve elx_summing_amplifier "V=[1, 2, -0.5]" "R=[10, 20, 5]" "Rf=10000 ohm"
Vout = -1 V
I_f = 0.0001 A
  by: Inverting summing amplifier  (Vout = -Rf sum(Vi/Ri))
  Rf = 10000 ohm
  assumes: one resistor per input; ideal op-amp

In the worked example, V = [1, 2, -0.5], R = [10, 20, 5], Rf = 10000 ohm go through the equation above and give Vout = -1 V, I_f = 0.0001 A. It applies only when one resistor per input; ideal op-amp: outside that it says what is wrong instead of returning a number.

Negative feedback: closed-loop gain and bandwidth extension — elx_negative_feedback

The closed-loop gain A/(1 + A beta), the loop gain, the desensitivity factor (also in dB) and the extended bandwidth of a single-pole amplifier with negative feedback.

Applies when: single-pole open-loop response; frequency-independent beta.

$ electronics-engineering solve elx_negative_feedback A=10000 beta=0.01 "fH=1000 Hz"
Af = 99.00990099
loop_gain = 100
desensitivity = 101
desensitivity_dB = 40.08642748
fH_closed = 101000 Hz
  by: Negative feedback: closed-loop gain and bandwidth extension  (Af = A/(1 + A beta); fH,f = fH (1 + A beta))
  A = 10000
  beta = 0.01
  fH = 1000 Hz
  assumes: single-pole open-loop response; frequency-independent beta

In the worked example, A = 10000, beta = 0.01, fH = 1000 Hz go through the equation above and give Af = 99.00990099, loop_gain = 100, desensitivity = 101, desensitivity_dB = 40.08642748. It applies only when single-pole open-loop response; frequency-independent beta: outside that it says what is wrong instead of returning a number.

Non-inverting op-amp amplifier — elx_noninverting_amplifier

The closed-loop gain 1 + Rf/Rg and the output voltage of an ideal non-inverting amplifier.

Applies when: ideal op-amp.

$ electronics-engineering solve elx_noninverting_amplifier "Rf=90000 ohm" "Rg=10000 ohm" "Vin=0.3 V"
G = 10
Vout = 3 V
  by: Non-inverting op-amp amplifier  (G = 1 + Rf/Rg; Vout = G Vin)
  Rf = 90000 ohm
  Rg = 10000 ohm
  Vin = 0.3 V
  assumes: ideal op-amp

In the worked example, Rf = 90000 ohm, Rg = 10000 ohm, Vin = 0.3 V go through the equation above and give G = 10, Vout = 3 V. It applies only when ideal op-amp: outside that it says what is wrong instead of returning a number.

Op-amp difference amplifier (with resistor mismatch) — elx_difference_amplifier

The output of a one-op-amp difference amplifier with any four resistors, and its differential and common-mode gains (the common-mode gain is zero only when R4/R3 = R2/R1).

Applies when: ideal op-amp.

$ electronics-engineering solve elx_difference_amplifier "R1=10000 ohm" "R2=100000 ohm" "R3=10000 ohm" "R4=100000 ohm" "V1=1 V" "V2=1.2 V"
Vout = 2 V
Ad = 10
Acm = 0
  by: Op-amp difference amplifier (with resistor mismatch)  (Vout = -(R2/R1) V1 + (R4/(R3 + R4))(1 + R2/R1) V2; Ad = (a2 - a1)/2; Acm = a1 + a2)
  R1 = 10000 ohm
  R2 = 100000 ohm
  R3 = 10000 ohm
  R4 = 100000 ohm
  V1 = 1 V
  V2 = 1.2 V
  assumes: ideal op-amp

In the worked example, R1 = 10000 ohm, R2 = 100000 ohm, R3 = 10000 ohm, R4 = 100000 ohm, V1 = 1 V, V2 = 1.2 V go through the equation above and give Vout = 2 V, Ad = 10, Acm = 0. It applies only when ideal op-amp: outside that it says what is wrong instead of returning a number.

Op-amp differentiator: gain and output amplitude — elx_opamp_differentiator

The gain |H| = 2 pi f R C of an ideal inverting differentiator at a frequency and the peak output for a sinusoidal input of given amplitude.

Applies when: ideal op-amp (no high-frequency limiting).

$ electronics-engineering solve elx_opamp_differentiator "R=10000 ohm" "C=10 nF" "A=1 V" "f=1000 Hz"
gain = 0.6283185307
Vout_peak = 0.6283185307 V
gain_dB = -4.036402633
  by: Op-amp differentiator: gain and output amplitude  (|H| = 2 pi f R C; Vout,peak = |H| A)
  R = 10000 ohm
  C = 1e-08 F
  A = 1 V
  f = 1000 Hz
  assumes: ideal op-amp (no high-frequency limiting)

In the worked example, R = 10000 ohm, C = 10 nF, A = 1 V, f = 1000 Hz go through the equation above and give gain = 0.6283185307, Vout_peak = 0.6283185307 V, gain_dB = -4.036402633. It applies only when ideal op-amp (no high-frequency limiting): outside that it says what is wrong instead of returning a number.

Op-amp integrator: output ramp and unity-gain frequency — elx_opamp_integrator

The output of an ideal inverting integrator after a time with a constant input, its ramp rate, and the frequency at which its gain is one.

Applies when: ideal op-amp, output not saturated.

$ electronics-engineering solve elx_opamp_integrator "R=10000 ohm" "C=1 uF" "Vin=0.5 V" "t=2 ms"
Vout = -0.1 V
slope = -50 V/s
f_unity = 15.91549431 Hz
  by: Op-amp integrator: output ramp and unity-gain frequency  (Vout = V0 - Vin t/(R C); f = 1/(2 pi R C))
  R = 10000 ohm
  C = 1e-06 F
  Vin = 0.5 V
  t = 0.002 s
  assumes: ideal op-amp, output not saturated

In the worked example, R = 10000 ohm, C = 1 uF, Vin = 0.5 V, t = 2 ms go through the equation above and give Vout = -0.1 V, slope = -50 V/s, f_unity = 15.91549431 Hz. It applies only when ideal op-amp, output not saturated: outside that it says what is wrong instead of returning a number.

Op-amp output offset from input offset voltage and bias currents — elx_opamp_dc_offset

The DC output error of an inverting or non-inverting amplifier (input grounded) caused by the input offset voltage and the input bias and offset currents, and the compensating resistor that cancels the bias-current error.

Applies when: currents flow into the inputs; IB- = IB + Ios/2, IB+ = IB - Ios/2.

$ electronics-engineering solve elx_opamp_dc_offset "Vos=2 mV" "IB=100 nA" "Ios=10 nA" "Rf=100000 ohm" "R1=10000 ohm" "Rp=0 ohm"
Vout_Vos = 0.022 V
Vout_bias = 0.0105 V
Vout_total = 0.0325 V
Rp_optimal = 9090.909091 ohm
  by: Op-amp output offset from input offset voltage and bias currents  (Vout = Vos (1 + Rf/R1) + IB- Rf - IB+ Rp (1 + Rf/R1))
  Vos = 0.002 V
  IB = 1e-07 A
  Ios = 1e-08 A
  Rf = 100000 ohm
  R1 = 10000 ohm
  Rp = 0 ohm
  assumes: currents flow into the inputs; IB- = IB + Ios/2, IB+ = IB - Ios/2

In the worked example, Vos = 2 mV, IB = 100 nA, Ios = 10 nA, Rf = 100000 ohm, R1 = 10000 ohm, Rp = 0 ohm go through the equation above and give Vout_Vos = 0.022 V, Vout_bias = 0.0105 V, Vout_total = 0.0325 V, Rp_optimal = 9090.909091 ohm. It applies only when currents flow into the inputs; IB- = IB + Ios/2, IB+ = IB - Ios/2: outside that it says what is wrong instead of returning a number.

Phase margin of a two-pole amplifier with feedback — elx_two_pole_phase_margin

The loop-gain crossover frequency and the phase margin of an amplifier with two real poles and a frequency-independent feedback factor, and its closed-loop DC gain.

Applies when: A0 beta > 1; two real left-half-plane poles.

$ electronics-engineering solve elx_two_pole_phase_margin A0=100000 "f1=10 Hz" "f2=1000000 Hz" beta=0.1
f_c = 99508.54868 Hz
PM_deg = 84.32304539
Af = 9.9990001
  by: Phase margin of a two-pole amplifier with feedback  (|A0 beta|^2 = (1 + (fc/f1)^2)(1 + (fc/f2)^2) solved for fc^2; PM = 180 - atan(fc/f1) - atan(fc/f2))
  A0 = 100000
  f1 = 10 Hz
  f2 = 1000000 Hz
  beta = 0.1
  assumes: A0 beta > 1; two real left-half-plane poles

In the worked example, A0 = 100000, f1 = 10 Hz, f2 = 1000000 Hz, beta = 0.1 go through the equation above and give f_c = 99508.54868 Hz, PM_deg = 84.32304539, Af = 9.9990001. It applies only when A0 beta > 1; two real left-half-plane poles: outside that it says what is wrong instead of returning a number.

Slew-rate limit: full-power bandwidth — elx_slew_rate_limit

The full-power bandwidth SR/(2 pi Vp) of an op-amp, the largest undistorted amplitude at a frequency, the slope a sine wave needs and whether it is slew-limited.

Applies when: sinusoidal output.

$ electronics-engineering solve elx_slew_rate_limit "SR=0.5 V/us" "Vp=10 V" "f=20000 Hz"
f_max = 7957.747155 Hz
Vp_max = 3.978873577 V
slope_needed = 1256637.061 V/s
limited = slew-limited
  by: Slew-rate limit: full-power bandwidth  (f_max = SR/(2 pi Vp); Vp,max = SR/(2 pi f); slope = 2 pi f Vp)
  SR = 500000 V/s
  Vp = 10 V
  f = 20000 Hz
  assumes: sinusoidal output

In the worked example, SR = 0.5 V/us, Vp = 10 V, f = 20000 Hz go through the equation above and give f_max = 7957.747155 Hz, Vp_max = 3.978873577 V, slope_needed = 1256637.061 V/s, limited = slew-limited. It applies only when sinusoidal output: outside that it says what is wrong instead of returning a number.

Three-op-amp instrumentation amplifier — elx_instrumentation_amplifier

The gain and output of the classic three-op-amp instrumentation amplifier: input stage gain 1 + 2 R1/RG times the difference stage gain R3/R2.

Applies when: ideal op-amps, matched resistors.

$ electronics-engineering solve elx_instrumentation_amplifier "R1=25000 ohm" "RG=1000 ohm" "R2=10000 ohm" "R3=10000 ohm" "V1=1 V" "V2=1.01 V"
G = 51
G_stage1 = 51
Vout = 0.51 V
  by: Three-op-amp instrumentation amplifier  (G = (1 + 2 R1/RG)(R3/R2); Vout = G (V2 - V1))
  R1 = 25000 ohm
  RG = 1000 ohm
  R2 = 10000 ohm
  R3 = 10000 ohm
  V1 = 1 V
  V2 = 1.01 V
  assumes: ideal op-amps, matched resistors

In the worked example, R1 = 25000 ohm, RG = 1000 ohm, R2 = 10000 ohm, R3 = 10000 ohm, V1 = 1 V, V2 = 1.01 V go through the equation above and give G = 51, G_stage1 = 51, Vout = 0.51 V. It applies only when ideal op-amps, matched resistors: outside that it says what is wrong instead of returning a number.

Oscillators (9)

555 timer astable: frequency and duty cycle — elx_555_astable

The high and low times, period, frequency and duty cycle of a 555 timer in astable mode with resistors RA and RB and timing capacitor C.

Applies when: thresholds Vcc/3 and 2Vcc/3.

$ electronics-engineering solve elx_555_astable "RA=1000 ohm" "RB=10000 ohm" "C=10 uF"
t_high = 0.07624618986 s
t_low = 0.06931471806 s
T = 0.1455609079 s
f = 6.869976385 Hz
duty = 0.5238095238
  by: 555 timer astable: frequency and duty cycle  (t_H = ln2 (RA + RB) C; t_L = ln2 RB C; f = 1/(t_H + t_L))
  RA = 1000 ohm
  RB = 10000 ohm
  C = 1e-05 F
  assumes: thresholds Vcc/3 and 2Vcc/3

In the worked example, RA = 1000 ohm, RB = 10000 ohm, C = 10 uF go through the equation above and give t_high = 0.07624618986 s, t_low = 0.06931471806 s, T = 0.1455609079 s, f = 6.869976385 Hz. It applies only when thresholds Vcc/3 and 2Vcc/3: outside that it says what is wrong instead of returning a number.

555 timer monostable pulse width — elx_555_monostable

The output pulse width T = ln 3 R C (about 1.1 R C) of a 555 timer in monostable (one-shot) mode.

Applies when: threshold at 2Vcc/3; trigger pulse shorter than T.

$ electronics-engineering solve elx_555_monostable "R=100000 ohm" "C=10 uF"
T = 1.098612289 s
  by: 555 timer monostable pulse width  (T = ln 3 R C)
  R = 100000 ohm
  C = 1e-05 F
  assumes: threshold at 2Vcc/3; trigger pulse shorter than T

In the worked example, R = 100000 ohm, C = 10 uF go through the equation above and give T = 1.098612289 s. It applies only when threshold at 2Vcc/3; trigger pulse shorter than T: outside that it says what is wrong instead of returning a number.

Colpitts oscillator frequency and feedback ratio — elx_colpitts_oscillator

The oscillation frequency of a Colpitts oscillator from its inductor and the series combination of its two tank capacitors, the feedback fraction C1/C2 and the minimum amplifier gain C2/C1.

Applies when: lossless tank, amplifier does not load the tank.

$ electronics-engineering solve elx_colpitts_oscillator "L=100 uH" "C1=1 nF" "C2=10 nF"
C_eq = 9.090909091e-10 F
f0 = 527857.2298 Hz
beta = 0.1
A_min = 10
  by: Colpitts oscillator frequency and feedback ratio  (C_eq = C1 C2/(C1 + C2); f0 = 1/(2 pi sqrt(L C_eq)); beta = C1/C2)
  L = 0.0001 H
  C1 = 1e-09 F
  C2 = 1e-08 F
  assumes: lossless tank, amplifier does not load the tank

In the worked example, L = 100 uH, C1 = 1 nF, C2 = 10 nF go through the equation above and give C_eq = 9.090909091e-10 F, f0 = 527857.2298 Hz, beta = 0.1, A_min = 10. It applies only when lossless tank, amplifier does not load the tank: outside that it says what is wrong instead of returning a number.

Hartley oscillator frequency — elx_hartley_oscillator

The oscillation frequency of a Hartley oscillator with a tapped (or two coupled) inductors and a tank capacitor, and the gain ratio (L1 + M)/(L2 + M).

Applies when: series-aiding coils, lossless tank; M <= sqrt(L1 L2).

$ electronics-engineering solve elx_hartley_oscillator "L1=100 uH" "L2=20 uH" "M=0 uH" "C=1 nF"
L_eq = 0.00012 H
f0 = 459440.7462 Hz
A_min = 5
  by: Hartley oscillator frequency  (L_eq = L1 + L2 + 2M; f0 = 1/(2 pi sqrt(L_eq C)))
  L1 = 0.0001 H
  L2 = 2e-05 H
  M = 0 H
  C = 1e-09 F
  assumes: series-aiding coils, lossless tank; M <= sqrt(L1 L2)

In the worked example, L1 = 100 uH, L2 = 20 uH, M = 0 uH, C = 1 nF go through the equation above and give L_eq = 0.00012 H, f0 = 459440.7462 Hz, A_min = 5. It applies only when series-aiding coils, lossless tank; M <= sqrt(L1 L2): outside that it says what is wrong instead of returning a number.

Op-amp relaxation (astable) oscillator — elx_opamp_relaxation_oscillator

The period and frequency of a square-wave op-amp astable: an RC timing network on the inverting input and positive feedback R1/(R1 + R2) to the non-inverting input, symmetric supplies.

Applies when: symmetric output levels; ideal comparator action.

$ electronics-engineering solve elx_opamp_relaxation_oscillator "R=10000 ohm" "C=100 nF" "R1=10000 ohm" "R2=10000 ohm"
beta = 0.5
T = 0.002197224577 s
f = 455.1196133 Hz
  by: Op-amp relaxation (astable) oscillator  (T = 2 R C ln((1 + beta)/(1 - beta)) = 2 R C ln(1 + 2 R1/R2))
  R = 10000 ohm
  C = 1e-07 F
  R1 = 10000 ohm
  R2 = 10000 ohm
  assumes: symmetric output levels; ideal comparator action

In the worked example, R = 10000 ohm, C = 100 nF, R1 = 10000 ohm, R2 = 10000 ohm go through the equation above and give beta = 0.5, T = 0.002197224577 s, f = 455.1196133 Hz. It applies only when symmetric output levels; ideal comparator action: outside that it says what is wrong instead of returning a number.

Quartz crystal: series and parallel resonance, Q — elx_crystal_oscillator

The series and parallel (anti-) resonant frequencies, their spacing and the quality factor of a quartz crystal from its Butterworth-Van Dyke equivalent circuit.

Applies when: resonances of the lossless circuit; Q from Rm.

$ electronics-engineering solve elx_crystal_oscillator "Lm=0.05 H" "Cm=20 fF" "Rm=20 ohm" "C0=5 pF"
fs = 5032921.21 Hz
fp = 5042977.007 Hz
delta_f = 10055.79666 Hz
Q = 79056.9415
  by: Quartz crystal: series and parallel resonance, Q  (fs = 1/(2 pi sqrt(Lm Cm)); fp = fs sqrt(1 + Cm/C0); Q = sqrt(Lm/Cm)/Rm)
  Lm = 0.05 H
  Cm = 2e-14 F
  Rm = 20 ohm
  C0 = 5e-12 F
  assumes: resonances of the lossless circuit; Q from Rm

In the worked example, Lm = 0.05 H, Cm = 20 fF, Rm = 20 ohm, C0 = 5 pF go through the equation above and give fs = 5032921.21 Hz, fp = 5042977.007 Hz, delta_f = 10055.79666 Hz, Q = 79056.9415. It applies only when resonances of the lossless circuit; Q from Rm: outside that it says what is wrong instead of returning a number.

RC phase-shift oscillator frequency and gain — elx_rc_phase_shift_oscillator

The oscillation frequency of a three-section RC phase-shift oscillator (high-pass ladder: series C, shunt R; or low-pass ladder) and the amplifier gain of 29 it needs.

Applies when: unloaded ladder (driven by a voltage source, feeding a high impedance).

$ electronics-engineering solve elx_rc_phase_shift_oscillator "R=10000 ohm" "C=10 nF" ladder=high-pass
f0 = 649.7473344 Hz
A_min = 29
beta = 0.03448275862
  by: RC phase-shift oscillator frequency and gain  (high-pass ladder f = 1/(2 pi sqrt(6) R C); low-pass ladder f = sqrt(6)/(2 pi R C); |beta| = 1/29)
  R = 10000 ohm
  C = 1e-08 F
  ladder = high-pass
  assumes: unloaded ladder (driven by a voltage source, feeding a high impedance)

In the worked example, R = 10000 ohm, C = 10 nF, ladder = high-pass go through the equation above and give f0 = 649.7473344 Hz, A_min = 29, beta = 0.03448275862. It applies only when unloaded ladder (driven by a voltage source, feeding a high impedance): outside that it says what is wrong instead of returning a number.

Type-2 PLL with active PI loop filter: natural frequency and damping — elx_pll_loop_dynamics

The natural frequency and damping factor of a second-order (type-2) phase-locked loop with phase-detector gain Kd, VCO gain Ko and an active PI loop filter F(s) = (1 + s tau2)/(s tau1).

Applies when: linear phase model, ideal integrator.

$ electronics-engineering solve elx_pll_loop_dynamics Kd=0.5 Ko=20000 "tau1=10 ms" "tau2=1 ms"
wn = 1000 rad/s
fn = 159.1549431 Hz
zeta = 0.5
  by: Type-2 PLL with active PI loop filter: natural frequency and damping  (H(s) = K (1 + s tau2)/tau1 / (s^2 + s K tau2/tau1 + K/tau1), K = Kd Ko; wn = sqrt(K/tau1); zeta = tau2 wn/2)
  Kd = 0.5
  Ko = 20000
  tau1 = 0.01 s
  tau2 = 0.001 s
  assumes: linear phase model, ideal integrator

In the worked example, Kd = 0.5, Ko = 20000, tau1 = 10 ms, tau2 = 1 ms go through the equation above and give wn = 1000 rad/s, fn = 159.1549431 Hz, zeta = 0.5. It applies only when linear phase model, ideal integrator: outside that it says what is wrong instead of returning a number.

Wien-bridge oscillator frequency and required gain — elx_wien_bridge_oscillator

The oscillation frequency of a Wien-bridge oscillator (series R1 C1, parallel R2 C2) and the non-inverting gain it needs (3 for equal components).

Applies when: ideal amplifier.

$ electronics-engineering solve elx_wien_bridge_oscillator "R1=10000 ohm" "C1=16 nF" "R2=10000 ohm" "C2=16 nF"
f0 = 994.7183943 Hz
beta = 0.3333333333
A_min = 3
Rf_over_Rg = 2
  by: Wien-bridge oscillator frequency and required gain  (f0 = 1/(2 pi sqrt(R1 R2 C1 C2)); A = 1 + R1/R2 + C2/C1)
  R1 = 10000 ohm
  C1 = 1.6e-08 F
  R2 = 10000 ohm
  C2 = 1.6e-08 F
  assumes: ideal amplifier

In the worked example, R1 = 10000 ohm, C1 = 16 nF, R2 = 10000 ohm, C2 = 16 nF go through the equation above and give f0 = 994.7183943 Hz, beta = 0.3333333333, A_min = 3, Rf_over_Rg = 2. It applies only when ideal amplifier: outside that it says what is wrong instead of returning a number.

Power supplies (5)

Adjustable three-terminal regulator output voltage — elx_adjustable_regulator_output

The output voltage of an adjustable three-terminal regulator (LM317 type: reference between OUT and ADJ, R1 from OUT to ADJ, R2 from ADJ to ground), including the adjust-pin current.

Applies when: regulator in regulation (input high enough).

$ electronics-engineering solve elx_adjustable_regulator_output "R1=240 ohm" "R2=720 ohm" "Vref=1.25 V"
Vout = 5 V
I_R1 = 0.005208333333 A
  by: Adjustable three-terminal regulator output voltage  (Vout = Vref (1 + R2/R1) + Iadj R2)
  R1 = 240 ohm
  R2 = 720 ohm
  Vref = 1.25 V
  assumes: regulator in regulation (input high enough)

In the worked example, R1 = 240 ohm, R2 = 720 ohm, Vref = 1.25 V go through the equation above and give Vout = 5 V, I_R1 = 0.005208333333 A. It applies only when regulator in regulation (input high enough): outside that it says what is wrong instead of returning a number.

Heat-sink thermal path: junction, case and sink temperatures — elx_heat_sink_temperatures

The junction, case and heat-sink temperatures of a power device dissipating P through junction-to-case, case-to-sink (interface) and sink-to-ambient thermal resistances.

Applies when: steady state, series thermal path.

$ electronics-engineering solve elx_heat_sink_temperatures "P=15 W" "Ta=25 degC" "theta_jc=1.5 K/W" "theta_cs=0.5 K/W" "theta_sa=3 K/W"
Tj = 373.15 K
Tc = 350.65 K
Ts = 343.15 K
Tj_C = 100
theta_ja = 5 K/W
  by: Heat-sink thermal path: junction, case and sink temperatures  (Tj = Ta + P (theta_jc + theta_cs + theta_sa))
  P = 15 W
  Ta = 298.15 K
  theta_jc = 1.5 K/W
  theta_cs = 0.5 K/W
  theta_sa = 3 K/W
  assumes: steady state, series thermal path

In the worked example, P = 15 W, Ta = 25 degC, theta_jc = 1.5 K/W, theta_cs = 0.5 K/W, theta_sa = 3 K/W go through the equation above and give Tj = 373.15 K, Tc = 350.65 K, Ts = 343.15 K, Tj_C = 100. It applies only when steady state, series thermal path: outside that it says what is wrong instead of returning a number.

Linear regulator dissipation and efficiency — elx_linear_regulator_efficiency

The input and output power, the dissipation in the pass element and the efficiency of a linear (series) regulator including its quiescent current.

Applies when: Vin > Vout.

$ electronics-engineering solve elx_linear_regulator_efficiency "Vin=12 V" "Vout=5 V" "Iload=500 mA" "Iq=5 mA"
P_in = 6.06 W
P_out = 2.5 W
P_diss = 3.56 W
efficiency = 0.4125412541
efficiency_pct = 41.25412541
  by: Linear regulator dissipation and efficiency  (P_in = Vin (IL + Iq); P_out = Vout IL; P_diss = P_in - P_out; eta = P_out/P_in)
  Vin = 12 V
  Vout = 5 V
  Iload = 0.5 A
  Iq = 0.005 A
  assumes: Vin > Vout

In the worked example, Vin = 12 V, Vout = 5 V, Iload = 500 mA, Iq = 5 mA go through the equation above and give P_in = 6.06 W, P_out = 2.5 W, P_diss = 3.56 W, efficiency = 0.4125412541. It applies only when Vin > Vout: outside that it says what is wrong instead of returning a number.

Required heat-sink thermal resistance — elx_heat_sink_required

The largest sink-to-ambient thermal resistance (and total junction-to-ambient resistance) that keeps a device dissipating P below its maximum junction temperature.

Applies when: a positive result (otherwise no heat sink suffices).

$ electronics-engineering solve elx_heat_sink_required "P=20 W" "Ta=40 degC" "Tj_max=150 degC" "theta_jc=1 K/W" "theta_cs=0.5 K/W"
theta_ja_max = 5.5 K/W
theta_sa_max = 4 K/W
  by: Required heat-sink thermal resistance  (theta_sa = (Tj,max - Ta)/P - theta_jc - theta_cs)
  P = 20 W
  Ta = 313.15 K
  Tj_max = 423.15 K
  theta_jc = 1 K/W
  theta_cs = 0.5 K/W
  assumes: a positive result (otherwise no heat sink suffices)

In the worked example, P = 20 W, Ta = 40 degC, Tj_max = 150 degC, theta_jc = 1 K/W, theta_cs = 0.5 K/W go through the equation above and give theta_ja_max = 5.5 K/W, theta_sa_max = 4 K/W. It applies only when a positive result (otherwise no heat sink suffices): outside that it says what is wrong instead of returning a number.

Zener-referenced series-pass (emitter-follower) regulator — elx_series_pass_regulator

The output voltage, load, base, Zener and resistor currents and the pass-transistor dissipation of a regulator in which a Zener diode biased through Rs sets the base of an emitter-follower pass transistor.

Applies when: Vin > Vz > VBE; the Zener stays in breakdown (Iz > 0).

$ electronics-engineering solve elx_series_pass_regulator "Vin=15 V" "Vz=10 V" "Rs=1000 ohm" "RL=100 ohm" beta=100 "VBE=0.7 V"
Vout = 9.3 V
I_L = 0.093 A
I_B = 0.0009207920792 A
I_z = 0.004079207921 A
I_Rs = 0.005 A
P_Q = 0.5248514851 W
  by: Zener-referenced series-pass (emitter-follower) regulator  (Vout = Vz - VBE; IB = IL/(beta + 1); Iz = (Vin - Vz)/Rs - IB; P = (Vin - Vout) IC)
  Vin = 15 V
  Vz = 10 V
  Rs = 1000 ohm
  RL = 100 ohm
  beta = 100
  VBE = 0.7 V
  assumes: Vin > Vz > VBE; the Zener stays in breakdown (Iz > 0)

In the worked example, Vin = 15 V, Vz = 10 V, Rs = 1000 ohm, RL = 100 ohm, beta = 100, VBE = 0.7 V go through the equation above and give Vout = 9.3 V, I_L = 0.093 A, I_B = 0.0009207920792 A, I_z = 0.004079207921 A. It applies only when Vin > Vz > VBE; the Zener stays in breakdown (Iz > 0): outside that it says what is wrong instead of returning a number.

Semiconductors (9)

Built-in potential of a pn junction — elx_builtin_potential

The built-in (contact) potential of an abrupt pn junction from the doping on each side, the intrinsic concentration and the temperature.

Applies when: NA, ND >= 100 ni; non-degenerate, complete ionisation.

$ electronics-engineering solve elx_builtin_potential "NA=1e+17 cm^-3" "ND=1e+16 cm^-3" "ni=1.5e+10 cm^-3" "T=300 K"
Vbi = 0.7528794135 V
  by: Built-in potential of a pn junction  (Vbi = (kT/q) ln(NA ND / ni^2))
  NA = 1e+23 1/m^3
  ND = 1e+22 1/m^3
  ni = 1.5e+16 1/m^3
  T = 300 K
  assumes: NA, ND >= 100 ni; non-degenerate, complete ionisation

In the worked example, NA = 1e+17 cm^-3, ND = 1e+16 cm^-3, ni = 1.5e+10 cm^-3, T = 300 K go through the equation above and give Vbi = 0.7528794135 V. It applies only when NA, ND >= 100 ni; non-degenerate, complete ionisation: outside that it says what is wrong instead of returning a number.

Conductivity and resistivity of a semiconductor — elx_semiconductor_conductivity

The conductivity sigma = q (n mu_n + p mu_p) and the resistivity of a semiconductor from its electron and hole concentrations and mobilities.

Applies when: n, p >= 0 (not both zero); mobilities > 0.

$ electronics-engineering solve elx_semiconductor_conductivity "n=1e+16 cm^-3" "p=22500 cm^-3" "mu_n=1350 cm^2/(V*s)" "mu_p=480 cm^2/(V*s)"
sigma = 216.2938456 1/(ohm*m)
rho = 0.004623340055 ohm*m
rho_ohm_cm = 0.4623340055
  by: Conductivity and resistivity of a semiconductor  (sigma = q (n mu_n + p mu_p); rho = 1/sigma)
  n = 1e+22 1/m^3
  p = 2.25e+10 1/m^3
  mu_n = 0.135 m^2/(V*s)
  mu_p = 0.048 m^2/(V*s)
  assumes: n, p >= 0 (not both zero); mobilities > 0

In the worked example, n = 1e+16 cm^-3, p = 22500 cm^-3, mu_n = 1350 cm^2/(V*s), mu_p = 480 cm^2/(V*s) go through the equation above and give sigma = 216.2938456 1/(ohm*m), rho = 0.004623340055 ohm*m, rho_ohm_cm = 0.4623340055. It applies only when n, p >= 0 (not both zero); mobilities > 0: outside that it says what is wrong instead of returning a number.

Depletion width, field and capacitance of an abrupt pn junction — elx_depletion_width

The depletion-region width (and its parts on each side), the peak electric field and the depletion capacitance per area of an abrupt pn junction at a reverse bias (negative VR for a forward bias below Vbi).

Applies when: Vbi + VR > 0; abrupt junction, depletion approximation.

$ electronics-engineering solve elx_depletion_width "NA=1e+17 cm^-3" "ND=1e+16 cm^-3" "Vbi=0.81 V" "VR=5 V" eps_r=11.7
W = 9.090996814e-07 m
W_um = 0.9090996814
xn = 8.264542558e-07 m
xp = 8.264542558e-08 m
Emax = 12781876.66 N/C
Cj_area = 0.0001139522976 F/m^2
  by: Depletion width, field and capacitance of an abrupt pn junction  (W = sqrt(2 eps (Vbi + VR)/q (1/NA + 1/ND)); xn = W NA/(NA+ND); Emax = q ND xn/eps; C' = eps/W)
  NA = 1e+23 1/m^3
  ND = 1e+22 1/m^3
  Vbi = 0.81 V
  VR = 5 V
  eps_r = 11.7
  assumes: Vbi + VR > 0; abrupt junction, depletion approximation

In the worked example, NA = 1e+17 cm^-3, ND = 1e+16 cm^-3, Vbi = 0.81 V, VR = 5 V, eps_r = 11.7 go through the equation above and give W = 9.090996814e-07 m, W_um = 0.9090996814, xn = 8.264542558e-07 m, xp = 8.264542558e-08 m. It applies only when Vbi + VR > 0; abrupt junction, depletion approximation: outside that it says what is wrong instead of returning a number.

Drift velocity and drift current in a semiconductor bar — elx_drift_current

The electric field, the carrier drift velocity, the drift current density and the current when a voltage is applied along a uniformly doped bar.

Applies when: n, mu, L, A > 0; low field (constant mobility).

$ electronics-engineering solve elx_drift_current "n=1e+16 cm^-3" "mu=1350 cm^2/(V*s)" "V=5 V" "L=0.001 m" "A=1e-08 m^2"
E = 5000 N/C
v_d = 675 m/s
J = 1081469.228 A/m^2
I = 0.01081469228 A
  by: Drift velocity and drift current in a semiconductor bar  (E = V/L; v_d = mu E; J = q n v_d; I = J A)
  n = 1e+22 1/m^3
  mu = 0.135 m^2/(V*s)
  V = 5 V
  L = 0.001 m
  A = 1e-08 m^2
  assumes: n, mu, L, A > 0; low field (constant mobility)

In the worked example, n = 1e+16 cm^-3, mu = 1350 cm^2/(V*s), V = 5 V, L = 0.001 m, A = 1e-08 m^2 go through the equation above and give E = 5000 N/C, v_d = 675 m/s, J = 1081469.228 A/m^2, I = 0.01081469228 A. It applies only when n, mu, L, A > 0; low field (constant mobility): outside that it says what is wrong instead of returning a number.

Einstein relation and diffusion length — elx_einstein_diffusion

The diffusion coefficient D = mu kT/q of carriers from their mobility (Einstein relation) and the diffusion length L = sqrt(D tau) from the minority-carrier lifetime.

Applies when: mu, T, tau > 0; non-degenerate material.

$ electronics-engineering solve elx_einstein_diffusion "mu=1350 cm^2/(V*s)" "T=300 K" "tau=1 us"
D = 0.003490019971 m^2/s
D_cm2 = 34.90019971
L_diff = 5.907639098e-05 m
L_um = 59.07639098
  by: Einstein relation and diffusion length  (D = mu kT/q; L = sqrt(D tau))
  mu = 0.135 m^2/(V*s)
  T = 300 K
  tau = 1e-06 s
  assumes: mu, T, tau > 0; non-degenerate material

In the worked example, mu = 1350 cm^2/(V*s), T = 300 K, tau = 1 us go through the equation above and give D = 0.003490019971 m^2/s, D_cm2 = 34.90019971, L_diff = 5.907639098e-05 m, L_um = 59.07639098. It applies only when mu, T, tau > 0; non-degenerate material: outside that it says what is wrong instead of returning a number.

Electron and hole concentrations of doped (compensated) material — elx_doped_carrier_concentrations

The equilibrium electron and hole concentrations of a semiconductor with donors and acceptors, from charge neutrality and the mass-action law (exact, so it also holds for light or compensated doping).

Applies when: ND, NA >= 0; ni > 0; complete ionisation, non-degenerate.

$ electronics-engineering solve elx_doped_carrier_concentrations "ND=1e+16 cm^-3" "NA=0 cm^-3" "ni=1.5e+10 cm^-3"
n = 1e+22 1/m^3
p = 2.25e+10 1/m^3
n_cm3 = 1e+16
p_cm3 = 22500
type = n-type
  by: Electron and hole concentrations of doped (compensated) material  (n - p = ND - NA and n p = ni^2: majority = |ND-NA|/2 + sqrt((ND-NA)^2/4 + ni^2), minority = ni^2/majority)
  ND = 1e+22 1/m^3
  NA = 0 1/m^3
  ni = 1.5e+16 1/m^3
  assumes: ND, NA >= 0; ni > 0; complete ionisation, non-degenerate

In the worked example, ND = 1e+16 cm^-3, NA = 0 cm^-3, ni = 1.5e+10 cm^-3 go through the equation above and give n = 1e+22 1/m^3, p = 2.25e+10 1/m^3, n_cm3 = 1e+16, p_cm3 = 22500. It applies only when ND, NA >= 0; ni > 0; complete ionisation, non-degenerate: outside that it says what is wrong instead of returning a number.

Intrinsic carrier concentration — elx_intrinsic_carrier_concentration

The intrinsic carrier concentration ni = sqrt(Nc Nv) exp(-Eg/2kT) at a temperature, from the effective densities of states at 300 K (scaled as T^1.5) and the band gap; also the intrinsic level's offset from midgap.

Applies when: Nc, Nv, Eg, T > 0; non-degenerate statistics, band gap independent of T.

$ electronics-engineering solve elx_intrinsic_carrier_concentration "Nc=2.8e+19 cm^-3" "Nv=1.04e+19 cm^-3" "Eg=1.12 eV" "T=300 K"
ni = 6.67589872e+15 1/m^3
ni_cm3 = 6675898720
Ei_minus_midgap_eV = -0.01280189354
Nc_T = 2.8e+25 1/m^3
Nv_T = 1.04e+25 1/m^3
  by: Intrinsic carrier concentration  (Nc(T) = Nc (T/300)^1.5, Nv likewise; ni = sqrt(Nc Nv) exp(-Eg/(2kT)); Ei - Emid = (kT/2) ln(Nv/Nc))
  Nc = 2.8e+25 1/m^3
  Nv = 1.04e+25 1/m^3
  Eg = 1.79443783e-19 J
  T = 300 K
  assumes: Nc, Nv, Eg, T > 0; non-degenerate statistics, band gap independent of T

In the worked example, Nc = 2.8e+19 cm^-3, Nv = 1.04e+19 cm^-3, Eg = 1.12 eV, T = 300 K go through the equation above and give ni = 6.67589872e+15 1/m^3, ni_cm3 = 6675898720, Ei_minus_midgap_eV = -0.01280189354, Nc_T = 2.8e+25 1/m^3. It applies only when Nc, Nv, Eg, T > 0; non-degenerate statistics, band gap independent of T: outside that it says what is wrong instead of returning a number.

Junction (depletion) capacitance versus bias — elx_junction_capacitance

The depletion capacitance of a pn junction at a reverse bias from its zero-bias value, the built-in potential and the grading coefficient (1/2 abrupt, 1/3 linearly graded), as used for varactors.

Applies when: 0 < m < 1; VR > -Vbi.

$ electronics-engineering solve elx_junction_capacitance "Cj0=2 pF" "Vbi=0.75 V" "VR=5 V" m=0.5
Cj = 7.223151185e-13 F
ratio = 0.3611575593
  by: Junction (depletion) capacitance versus bias  (Cj = Cj0 / (1 + VR/Vbi)^m)
  Cj0 = 2e-12 F
  Vbi = 0.75 V
  VR = 5 V
  m = 0.5
  assumes: 0 < m < 1; VR > -Vbi

In the worked example, Cj0 = 2 pF, Vbi = 0.75 V, VR = 5 V, m = 0.5 go through the equation above and give Cj = 7.223151185e-13 F, ratio = 0.3611575593. It applies only when 0 < m < 1; VR > -Vbi: outside that it says what is wrong instead of returning a number.

Thermal voltage kT/q — elx_thermal_voltage

The thermal voltage VT = kT/q at an absolute temperature (about 25.85 mV at 300 K), the voltage scale of every diode and transistor equation.

Applies when: T > 0 K.

$ electronics-engineering solve elx_thermal_voltage "T=300 K"
VT = 0.02585199979 V
VT_mV = 25.85199979
  by: Thermal voltage kT/q  (VT = k T / q)
  T = 300 K
  assumes: T > 0 K

In the worked example, T = 300 K go through the equation above and give VT = 0.02585199979 V, VT_mV = 25.85199979. It applies only when T > 0 K: outside that it says what is wrong instead of returning a number.

Timing (5)

CMOS dynamic (switching) power — elx_cmos_dynamic_power

The dynamic power alpha C VDD^2 f of CMOS logic, the energy drawn from the supply per 0 -> 1 transition, the energy stored on the load and the average supply current.

Applies when: 0 <= alpha <= 1; full-swing switching, short-circuit and leakage power not included.

$ electronics-engineering solve elx_cmos_dynamic_power alpha=0.1 "C=1000 pF" "VDD=1 V" "f=1000000000 Hz"
P = 0.1 W
E_supply = 1e-09 J
E_stored = 5e-10 J
I_avg = 0.1 A
  by: CMOS dynamic (switching) power  (P = alpha C VDD^2 f)
  alpha = 0.1
  C = 1e-09 F
  VDD = 1 V
  f = 1000000000 Hz
  assumes: 0 <= alpha <= 1; full-swing switching, short-circuit and leakage power not included

In the worked example, alpha = 0.1, C = 1000 pF, VDD = 1 V, f = 1000000000 Hz go through the equation above and give P = 0.1 W, E_supply = 1e-09 J, E_stored = 5e-10 J, I_avg = 0.1 A. It applies only when 0 <= alpha <= 1; full-swing switching, short-circuit and leakage power not included: outside that it says what is wrong instead of returning a number.

Elmore delay of an RC ladder (interconnect) — elx_elmore_delay

The Elmore delay to every node of an RC ladder (a driver resistance and wire segments, each followed by a capacitance to ground), the delay at the far end and its 50 % estimate ln 2 tau.

Applies when: one capacitance per resistor; step input.

$ electronics-engineering solve elx_elmore_delay "R=[100, 50, 50]" "C=[0.1, 0.1, 0.2]"
tau_D = 6.5e-11 s
t50 = 4.505456674e-11 s
delays = [4e-11,5.5e-11,6.5e-11]
  by: Elmore delay of an RC ladder (interconnect)  (tau_k = sum_i C_i R(shared path of nodes i and k))
  assumes: one capacitance per resistor; step input

In the worked example, R = [100, 50, 50], C = [0.1, 0.1, 0.2] go through the equation above and give tau_D = 6.5e-11 s, t50 = 4.505456674e-11 s, delays = [4e-11, 5.5e-11, 6.5e-11]. It applies only when one capacitance per resistor; step input: outside that it says what is wrong instead of returning a number.

Flip-flop setup and hold slack, maximum clock frequency — elx_setup_hold_timing

The setup slack, hold slack, maximum clock frequency and a verdict for a register-to-register path from clock-to-Q, logic delays, setup and hold times and clock skew (positive when the capture clock is late).

Applies when: edge-triggered registers, single clock.

$ electronics-engineering solve elx_setup_hold_timing "T=5 ns" "tcq=0.3 ns" "tpd=3.5 ns" "tsu=0.2 ns" "tskew=0.1 ns" "tccq=0.1 ns" "tcd=0.2 ns" "th=0.1 ns"
setup_slack = 1.1e-09 s
hold_slack = 1e-10 s
f_max = 256410256.4 Hz
verdict = meets timing
  by: Flip-flop setup and hold slack, maximum clock frequency  (setup slack = T + skew - (tcq + tpd + tsu); hold slack = tccq + tcd - th - skew; f_max = 1/(tcq + tpd + tsu - skew))
  T = 5e-09 s
  tcq = 3e-10 s
  tpd = 3.5e-09 s
  tsu = 2e-10 s
  tskew = 1e-10 s
  tccq = 1e-10 s
  tcd = 2e-10 s
  th = 1e-10 s
  assumes: edge-triggered registers, single clock

In the worked example, T = 5 ns, tcq = 0.3 ns, tpd = 3.5 ns, tsu = 0.2 ns, tskew = 0.1 ns, tccq = 0.1 ns, tcd = 0.2 ns, th = 0.1 ns go through the equation above and give setup_slack = 1.1e-09 s, hold_slack = 1e-10 s, f_max = 256410256.4 Hz, verdict = meets timing. It applies only when edge-triggered registers, single clock: outside that it says what is wrong instead of returning a number.

RC delay, 10-90 % rise time and bandwidth — elx_rc_delay_rise_time

The time constant, the 50 % delay (ln 2 RC), the 10-90 % rise time (ln 9 RC = 2.2 RC), the -3 dB bandwidth and the rise-time-bandwidth product (0.35) of a first-order RC low-pass.

Applies when: step input, first-order RC.

$ electronics-engineering solve elx_rc_delay_rise_time "R=1000 ohm" "C=10 pF"
tau = 1e-08 s
t50 = 6.931471806e-09 s
t_rise = 2.197224577e-08 s
f_3dB = 15915494.31 Hz
tr_times_bw = 0.3496991526
  by: RC delay, 10-90 % rise time and bandwidth  (t50 = ln 2 RC; tr = ln 9 RC; f = 1/(2 pi RC); tr f = ln 9/(2 pi))
  R = 1000 ohm
  C = 1e-11 F
  assumes: step input, first-order RC

In the worked example, R = 1000 ohm, C = 10 pF go through the equation above and give tau = 1e-08 s, t50 = 6.931471806e-09 s, t_rise = 2.197224577e-08 s, f_3dB = 15915494.31 Hz. It applies only when step input, first-order RC: outside that it says what is wrong instead of returning a number.

Synchronizer metastability MTBF — elx_metastability_mtbf

The mean time between synchronizer failures MTBF = exp(tr/tau)/(T0 fclk fdata) from the resolution time allowed, the flip-flop's time constant and window, and the clock and data rates.

Applies when: tr/tau <= 700.

$ electronics-engineering solve elx_metastability_mtbf "tr=2 ns" "tau=50 ps" "T0=100 ps" "fclk=500000000 Hz" "fdata=10000000 Hz"
MTBF_s = 4.707705337e+11 s
MTBF_years = 14917.81801
log10_MTBF_s = 11.67280927
  by: Synchronizer metastability MTBF  (MTBF = exp(tr/tau)/(T0 fclk fdata))
  tr = 2e-09 s
  tau = 5e-11 s
  T0 = 1e-10 s
  fclk = 500000000 Hz
  fdata = 10000000 Hz
  assumes: tr/tau <= 700

In the worked example, tr = 2 ns, tau = 50 ps, T0 = 100 ps, fclk = 500000000 Hz, fdata = 10000000 Hz go through the equation above and give MTBF_s = 4.707705337e+11 s, MTBF_years = 14917.81801, log10_MTBF_s = 11.67280927. It applies only when tr/tau <= 700: outside that it says what is wrong instead of returning a number.

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