size int64 2 8 | keys stringlengths 10 106 | symbols stringlengths 3 29 | domains stringclasses 62
values | pi stringlengths 3 46 | equation stringlengths 10 59 | name stringclasses 19
values | n_const int64 0 4 | n_domains int64 1 6 | max_exp int64 1 34 | exp_l1 int64 2 134 | complexity float64 0 113 | score float64 -104.8 10 | plausible bool 2
classes | exponents stringlengths 27 177 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
4 | force,length,mass,time | m·ℓ·t·F | mechanics | m·ℓ·t⁻²·F⁻¹ | m = k₀ · ℓ⁻¹·t²·F | null | 0 | 1 | 2 | 5 | 3.2 | 6.8 | true | {"mass": "1", "length": "1", "time": "-2", "force": "-1"} |
4 | energy,length,mass,time | m·ℓ·t·E | mechanics | m·ℓ²·t⁻²·E⁻¹ | m = k₀ · ℓ⁻²·t²·E | null | 0 | 1 | 2 | 6 | 3.9 | 6.1 | true | {"mass": "1", "length": "2", "time": "-2", "energy": "-1"} |
4 | length,mass,time,torque | m·ℓ·t·τ | mechanics | m·ℓ²·t⁻²·τ⁻¹ | m = k₀ · ℓ⁻²·t²·τ | null | 0 | 1 | 2 | 6 | 3.9 | 6.1 | true | {"mass": "1", "length": "2", "time": "-2", "torque": "-1"} |
4 | length,mass,power,time | m·ℓ·t·P | mechanics | m·ℓ²·t⁻³·P⁻¹ | m = k₀ · ℓ⁻²·t³·P | null | 0 | 1 | 3 | 7 | 5.1 | 4.9 | true | {"mass": "1", "length": "2", "time": "-3", "power": "-1"} |
4 | length,mass,momentum,time | m·ℓ·t·p | mechanics | m·ℓ·t⁻¹·p⁻¹ | m = k₀ · ℓ⁻¹·t·p | null | 0 | 1 | 1 | 4 | 2 | 8 | true | {"mass": "1", "length": "1", "time": "-1", "momentum": "-1"} |
4 | ang_momentum,length,mass,time | m·ℓ·t·Lₐ | mechanics | m·ℓ²·t⁻¹·Lₐ⁻¹ | m = k₀ · ℓ⁻²·t·Lₐ | null | 0 | 1 | 2 | 5 | 3.2 | 6.8 | true | {"mass": "1", "length": "2", "time": "-1", "ang_momentum": "-1"} |
4 | action,length,mass,time | m·ℓ·t·S | mechanics | m·ℓ²·t⁻¹·S⁻¹ | m = k₀ · ℓ⁻²·t·S | null | 0 | 1 | 2 | 5 | 3.2 | 6.8 | true | {"mass": "1", "length": "2", "time": "-1", "action": "-1"} |
4 | length,mass,pressure,time | m·ℓ·t·P_p | mechanics | m·ℓ⁻¹·t⁻²·P_p⁻¹ | m = k₀ · ℓ·t²·P_p | null | 0 | 1 | 2 | 5 | 3.2 | 6.8 | true | {"mass": "1", "length": "-1", "time": "-2", "pressure": "-1"} |
4 | length,mass,time,viscosity | m·ℓ·t·μ | mechanics | m·ℓ⁻¹·t⁻¹·μ⁻¹ | m = k₀ · ℓ·t·μ | null | 0 | 1 | 1 | 4 | 2 | 8 | true | {"mass": "1", "length": "-1", "time": "-1", "viscosity": "-1"} |
5 | entropy,length,mass,temperature,time | m·ℓ·t·Θ·S_e | mechanics,thermo | m·ℓ²·t⁻²·Θ⁻¹·S_e⁻¹ | m = k₀ · ℓ⁻²·t²·Θ·S_e | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-2", "temperature": "-1", "entropy": "-1"} |
5 | heat_capacity,length,mass,temperature,time | m·ℓ·t·Θ·C | mechanics,thermo | m·ℓ²·t⁻²·Θ⁻¹·C⁻¹ | m = k₀ · ℓ⁻²·t²·Θ·C | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-2", "temperature": "-1", "heat_capacity": "-1"} |
5 | length,mass,temperature,thermal_cond,time | m·ℓ·t·Θ·κ | mechanics,thermo | m·ℓ·t⁻³·Θ⁻¹·κ⁻¹ | m = k₀ · ℓ⁻¹·t³·Θ·κ | null | 0 | 2 | 3 | 7 | 6 | 3.5 | true | {"mass": "1", "length": "1", "time": "-3", "temperature": "-1", "thermal_cond": "-1"} |
6 | amount,gas_constant,length,mass,temperature,time | m·ℓ·t·Θ·n·R | chemistry,mechanics,thermo | m·ℓ²·t⁻²·Θ⁻¹·n⁻¹·R⁻¹ | m = k₀ · ℓ⁻²·t²·Θ·n·R | null | 0 | 3 | 2 | 8 | 7.1 | 1.9 | false | {"mass": "1", "length": "2", "time": "-2", "temperature": "-1", "amount": "-1", "gas_constant": "-1"} |
6 | concentration,gas_constant,length,mass,temperature,time | m·ℓ·t·Θ·c_n·R | chemistry,mechanics,thermo | m·ℓ⁻¹·t⁻²·Θ⁻¹·c_n⁻¹·R⁻¹ | m = k₀ · ℓ·t²·Θ·c_n·R | null | 0 | 3 | 2 | 7 | 6.4 | 2.6 | false | {"mass": "1", "length": "-1", "time": "-2", "temperature": "-1", "concentration": "-1", "gas_constant": "-1"} |
6 | cat_activity,gas_constant,length,mass,temperature,time | m·ℓ·t·Θ·R·z | chemistry,mechanics,thermo | m·ℓ²·t⁻³·Θ⁻¹·R⁻¹·z⁻¹ | m = k₀ · ℓ⁻²·t³·Θ·R·z | null | 0 | 3 | 3 | 9 | 8.3 | 0.7 | false | {"mass": "1", "length": "2", "time": "-3", "temperature": "-1", "gas_constant": "-1", "cat_activity": "-1"} |
6 | avogadro,gas_constant,length,mass,temperature,time | m·ℓ·t·Θ·R·N_A | chemistry,constants,mechanics,thermo | m·ℓ²·t⁻²·Θ⁻¹·R⁻¹·N_A | m = k₀ · ℓ⁻²·t²·Θ·R·N_A⁻¹ | null | 1 | 4 | 2 | 8 | 7.7 | 0.8 | false | {"mass": "1", "length": "2", "time": "-2", "temperature": "-1", "gas_constant": "-1", "avogadro": "1"} |
5 | boltzmann,length,mass,temperature,time | m·ℓ·t·Θ·k_B | constants,mechanics,thermo | m·ℓ²·t⁻²·Θ⁻¹·k_B⁻¹ | m = k₀ · ℓ⁻²·t²·Θ·k_B | null | 1 | 3 | 2 | 7 | 6.1 | 2.9 | false | {"mass": "1", "length": "2", "time": "-2", "temperature": "-1", "boltzmann": "-1"} |
5 | entropy,expansion,length,mass,time | m·ℓ·t·S_e·β | mechanics,thermo | m·ℓ²·t⁻²·S_e⁻¹·β | m = k₀ · ℓ⁻²·t²·S_e·β⁻¹ | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-2", "entropy": "-1", "expansion": "1"} |
6 | entropy,gas_constant,length,mass,molar_energy,time | m·ℓ·t·S_e·E_m·R | chemistry,mechanics,thermo | m·ℓ²·t⁻²·S_e⁻¹·E_m⁻¹·R | m = k₀ · ℓ⁻²·t²·S_e·E_m·R⁻¹ | null | 0 | 3 | 2 | 8 | 7.1 | 1.9 | false | {"mass": "1", "length": "2", "time": "-2", "entropy": "-1", "molar_energy": "-1", "gas_constant": "1"} |
5 | expansion,heat_capacity,length,mass,time | m·ℓ·t·C·β | mechanics,thermo | m·ℓ²·t⁻²·C⁻¹·β | m = k₀ · ℓ⁻²·t²·C·β⁻¹ | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-2", "heat_capacity": "-1", "expansion": "1"} |
6 | gas_constant,heat_capacity,length,mass,molar_energy,time | m·ℓ·t·C·E_m·R | chemistry,mechanics,thermo | m·ℓ²·t⁻²·C⁻¹·E_m⁻¹·R | m = k₀ · ℓ⁻²·t²·C·E_m·R⁻¹ | null | 0 | 3 | 2 | 8 | 7.1 | 1.9 | false | {"mass": "1", "length": "2", "time": "-2", "heat_capacity": "-1", "molar_energy": "-1", "gas_constant": "1"} |
5 | length,mass,specific_heat,thermal_cond,time | m·ℓ·t·c·κ | mechanics,thermo | m·ℓ⁻¹·t⁻¹·c·κ⁻¹ | m = k₀ · ℓ·t·c⁻¹·κ | null | 0 | 2 | 1 | 5 | 3.6 | 5.9 | true | {"mass": "1", "length": "-1", "time": "-1", "specific_heat": "1", "thermal_cond": "-1"} |
5 | expansion,length,mass,thermal_cond,time | m·ℓ·t·κ·β | mechanics,thermo | m·ℓ·t⁻³·κ⁻¹·β | m = k₀ · ℓ⁻¹·t³·κ·β⁻¹ | null | 0 | 2 | 3 | 7 | 6 | 3.5 | true | {"mass": "1", "length": "1", "time": "-3", "thermal_cond": "-1", "expansion": "1"} |
6 | gas_constant,length,mass,molar_mass,thermal_cond,time | m·ℓ·t·κ·M_m·R | chemistry,mechanics,thermo | m·ℓ⁻¹·t⁻¹·κ⁻¹·M_m⁻¹·R | m = k₀ · ℓ·t·κ·M_m·R⁻¹ | null | 0 | 3 | 1 | 6 | 5.2 | 3.8 | false | {"mass": "1", "length": "-1", "time": "-1", "thermal_cond": "-1", "molar_mass": "-1", "gas_constant": "1"} |
6 | gas_constant,length,mass,molar_energy,thermal_cond,time | m·ℓ·t·κ·E_m·R | chemistry,mechanics,thermo | m·ℓ·t⁻³·κ⁻¹·E_m⁻¹·R | m = k₀ · ℓ⁻¹·t³·κ·E_m·R⁻¹ | null | 0 | 3 | 3 | 8 | 7.6 | 1.4 | false | {"mass": "1", "length": "1", "time": "-3", "thermal_cond": "-1", "molar_energy": "-1", "gas_constant": "1"} |
6 | amount,expansion,gas_constant,length,mass,time | m·ℓ·t·β·n·R | chemistry,mechanics,thermo | m·ℓ²·t⁻²·β·n⁻¹·R⁻¹ | m = k₀ · ℓ⁻²·t²·β⁻¹·n·R | null | 0 | 3 | 2 | 8 | 7.1 | 1.9 | false | {"mass": "1", "length": "2", "time": "-2", "expansion": "1", "amount": "-1", "gas_constant": "-1"} |
6 | concentration,expansion,gas_constant,length,mass,time | m·ℓ·t·β·c_n·R | chemistry,mechanics,thermo | m·ℓ⁻¹·t⁻²·β·c_n⁻¹·R⁻¹ | m = k₀ · ℓ·t²·β⁻¹·c_n·R | null | 0 | 3 | 2 | 7 | 6.4 | 2.6 | false | {"mass": "1", "length": "-1", "time": "-2", "expansion": "1", "concentration": "-1", "gas_constant": "-1"} |
6 | cat_activity,expansion,gas_constant,length,mass,time | m·ℓ·t·β·R·z | chemistry,mechanics,thermo | m·ℓ²·t⁻³·β·R⁻¹·z⁻¹ | m = k₀ · ℓ⁻²·t³·β⁻¹·R·z | null | 0 | 3 | 3 | 9 | 8.3 | 0.7 | false | {"mass": "1", "length": "2", "time": "-3", "expansion": "1", "gas_constant": "-1", "cat_activity": "-1"} |
6 | avogadro,expansion,gas_constant,length,mass,time | m·ℓ·t·β·R·N_A | chemistry,constants,mechanics,thermo | m·ℓ²·t⁻²·β·R⁻¹·N_A | m = k₀ · ℓ⁻²·t²·β⁻¹·R·N_A⁻¹ | null | 1 | 4 | 2 | 8 | 7.7 | 0.8 | false | {"mass": "1", "length": "2", "time": "-2", "expansion": "1", "gas_constant": "-1", "avogadro": "1"} |
5 | boltzmann,expansion,length,mass,time | m·ℓ·t·β·k_B | constants,mechanics,thermo | m·ℓ²·t⁻²·β·k_B⁻¹ | m = k₀ · ℓ⁻²·t²·β⁻¹·k_B | null | 1 | 3 | 2 | 7 | 6.1 | 2.9 | false | {"mass": "1", "length": "2", "time": "-2", "expansion": "1", "boltzmann": "-1"} |
5 | charge,length,mass,time,voltage | m·ℓ·t·q·U | em,mechanics | m·ℓ²·t⁻²·q⁻¹·U⁻¹ | m = k₀ · ℓ⁻²·t²·q·U | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-2", "charge": "-1", "voltage": "-1"} |
5 | charge,length,mass,resistance,time | m·ℓ·t·q·R | em,mechanics | m·ℓ²·t⁻¹·q⁻²·R⁻¹ | m = k₀ · ℓ⁻²·t·q²·R | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-1", "charge": "-2", "resistance": "-1"} |
5 | capacitance,charge,length,mass,time | m·ℓ·t·q·C_e | em,mechanics | m·ℓ²·t⁻²·q⁻²·C_e | m = k₀ · ℓ⁻²·t²·q²·C_e⁻¹ | null | 0 | 2 | 2 | 8 | 6.2 | 3.3 | true | {"mass": "1", "length": "2", "time": "-2", "charge": "-2", "capacitance": "1"} |
5 | charge,efield,length,mass,time | m·ℓ·t·q·E_f | em,mechanics | m·ℓ·t⁻²·q⁻¹·E_f⁻¹ | m = k₀ · ℓ⁻¹·t²·q·E_f | null | 0 | 2 | 2 | 6 | 4.8 | 4.7 | true | {"mass": "1", "length": "1", "time": "-2", "charge": "-1", "efield": "-1"} |
5 | charge,length,mag_flux,mass,time | m·ℓ·t·q·Φ | em,mechanics | m·ℓ²·t⁻¹·q⁻¹·Φ⁻¹ | m = k₀ · ℓ⁻²·t·q·Φ | null | 0 | 2 | 2 | 6 | 4.8 | 4.7 | true | {"mass": "1", "length": "2", "time": "-1", "charge": "-1", "mag_flux": "-1"} |
5 | charge,length,mass,permittivity,time | m·ℓ·t·q·ε | em,mechanics | m·ℓ³·t⁻²·q⁻²·ε | m = k₀ · ℓ⁻³·t²·q²·ε⁻¹ | null | 0 | 2 | 3 | 9 | 7.4 | 2.1 | false | {"mass": "1", "length": "3", "time": "-2", "charge": "-2", "permittivity": "1"} |
5 | charge,conductivity,length,mass,time | m·ℓ·t·q·σ | em,mechanics | m·ℓ³·t⁻¹·q⁻²·σ | m = k₀ · ℓ⁻³·t·q²·σ⁻¹ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "3", "time": "-1", "charge": "-2", "conductivity": "1"} |
5 | charge,length,mass,resistivity,time | m·ℓ·t·q·ρ_e | em,mechanics | m·ℓ³·t⁻¹·q⁻²·ρ_e⁻¹ | m = k₀ · ℓ⁻³·t·q²·ρ_e | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "3", "time": "-1", "charge": "-2", "resistivity": "-1"} |
5 | current,length,mass,time,voltage | m·ℓ·t·i·U | em,mechanics | m·ℓ²·t⁻³·i⁻¹·U⁻¹ | m = k₀ · ℓ⁻²·t³·i·U | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "2", "time": "-3", "current": "-1", "voltage": "-1"} |
5 | current,length,mass,resistance,time | m·ℓ·t·i·R | em,mechanics | m·ℓ²·t⁻³·i⁻²·R⁻¹ | m = k₀ · ℓ⁻²·t³·i²·R | null | 0 | 2 | 3 | 9 | 7.4 | 2.1 | false | {"mass": "1", "length": "2", "time": "-3", "current": "-2", "resistance": "-1"} |
5 | capacitance,current,length,mass,time | m·ℓ·t·i·C_e | em,mechanics | m·ℓ²·t⁻⁴·i⁻²·C_e | m = k₀ · ℓ⁻²·t⁴·i²·C_e⁻¹ | null | 0 | 2 | 4 | 10 | 8.6 | 0.9 | false | {"mass": "1", "length": "2", "time": "-4", "current": "-2", "capacitance": "1"} |
5 | current,inductance,length,mass,time | m·ℓ·t·i·L_e | em,mechanics | m·ℓ²·t⁻²·i⁻²·L_e⁻¹ | m = k₀ · ℓ⁻²·t²·i²·L_e | null | 0 | 2 | 2 | 8 | 6.2 | 3.3 | true | {"mass": "1", "length": "2", "time": "-2", "current": "-2", "inductance": "-1"} |
5 | current,efield,length,mass,time | m·ℓ·t·i·E_f | em,mechanics | m·ℓ·t⁻³·i⁻¹·E_f⁻¹ | m = k₀ · ℓ⁻¹·t³·i·E_f | null | 0 | 2 | 3 | 7 | 6 | 3.5 | true | {"mass": "1", "length": "1", "time": "-3", "current": "-1", "efield": "-1"} |
5 | current,length,mag_flux,mass,time | m·ℓ·t·i·Φ | em,mechanics | m·ℓ²·t⁻²·i⁻¹·Φ⁻¹ | m = k₀ · ℓ⁻²·t²·i·Φ | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-2", "current": "-1", "mag_flux": "-1"} |
5 | current,length,mass,permittivity,time | m·ℓ·t·i·ε | em,mechanics | m·ℓ³·t⁻⁴·i⁻²·ε | m = k₀ · ℓ⁻³·t⁴·i²·ε⁻¹ | null | 0 | 2 | 4 | 11 | 9.3 | 0.2 | false | {"mass": "1", "length": "3", "time": "-4", "current": "-2", "permittivity": "1"} |
5 | current,length,mass,permeability,time | m·ℓ·t·i·μ₀ | em,mechanics | m·ℓ·t⁻²·i⁻²·μ₀⁻¹ | m = k₀ · ℓ⁻¹·t²·i²·μ₀ | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "1", "time": "-2", "current": "-2", "permeability": "-1"} |
5 | conductivity,current,length,mass,time | m·ℓ·t·i·σ | em,mechanics | m·ℓ³·t⁻³·i⁻²·σ | m = k₀ · ℓ⁻³·t³·i²·σ⁻¹ | null | 0 | 2 | 3 | 10 | 8.1 | 1.4 | false | {"mass": "1", "length": "3", "time": "-3", "current": "-2", "conductivity": "1"} |
5 | current,length,mass,resistivity,time | m·ℓ·t·i·ρ_e | em,mechanics | m·ℓ³·t⁻³·i⁻²·ρ_e⁻¹ | m = k₀ · ℓ⁻³·t³·i²·ρ_e | null | 0 | 2 | 3 | 10 | 8.1 | 1.4 | false | {"mass": "1", "length": "3", "time": "-3", "current": "-2", "resistivity": "-1"} |
5 | length,mass,resistance,time,voltage | m·ℓ·t·U·R | em,mechanics | m·ℓ²·t⁻³·U⁻²·R | m = k₀ · ℓ⁻²·t³·U²·R⁻¹ | null | 0 | 2 | 3 | 9 | 7.4 | 2.1 | false | {"mass": "1", "length": "2", "time": "-3", "voltage": "-2", "resistance": "1"} |
5 | capacitance,length,mass,time,voltage | m·ℓ·t·U·C_e | em,mechanics | m·ℓ²·t⁻²·U⁻²·C_e⁻¹ | m = k₀ · ℓ⁻²·t²·U²·C_e | null | 0 | 2 | 2 | 8 | 6.2 | 3.3 | true | {"mass": "1", "length": "2", "time": "-2", "voltage": "-2", "capacitance": "-1"} |
5 | inductance,length,mass,time,voltage | m·ℓ·t·U·L_e | em,mechanics | m·ℓ²·t⁻⁴·U⁻²·L_e | m = k₀ · ℓ⁻²·t⁴·U²·L_e⁻¹ | null | 0 | 2 | 4 | 10 | 8.6 | 0.9 | false | {"mass": "1", "length": "2", "time": "-4", "voltage": "-2", "inductance": "1"} |
5 | length,mass,permittivity,time,voltage | m·ℓ·t·U·ε | em,mechanics | m·ℓ·t⁻²·U⁻²·ε⁻¹ | m = k₀ · ℓ⁻¹·t²·U²·ε | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "1", "time": "-2", "voltage": "-2", "permittivity": "-1"} |
5 | length,mass,permeability,time,voltage | m·ℓ·t·U·μ₀ | em,mechanics | m·ℓ³·t⁻⁴·U⁻²·μ₀ | m = k₀ · ℓ⁻³·t⁴·U²·μ₀⁻¹ | null | 0 | 2 | 4 | 11 | 9.3 | 0.2 | false | {"mass": "1", "length": "3", "time": "-4", "voltage": "-2", "permeability": "1"} |
5 | conductivity,length,mass,time,voltage | m·ℓ·t·U·σ | em,mechanics | m·ℓ·t⁻³·U⁻²·σ⁻¹ | m = k₀ · ℓ⁻¹·t³·U²·σ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "1", "time": "-3", "voltage": "-2", "conductivity": "-1"} |
5 | length,mass,resistivity,time,voltage | m·ℓ·t·U·ρ_e | em,mechanics | m·ℓ·t⁻³·U⁻²·ρ_e | m = k₀ · ℓ⁻¹·t³·U²·ρ_e⁻¹ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "1", "time": "-3", "voltage": "-2", "resistivity": "1"} |
5 | elem_charge,length,mass,time,voltage | m·ℓ·t·U·e | constants,em,mechanics | m·ℓ²·t⁻²·U⁻¹·e⁻¹ | m = k₀ · ℓ⁻²·t²·U·e | null | 1 | 3 | 2 | 7 | 6.1 | 2.9 | false | {"mass": "1", "length": "2", "time": "-2", "voltage": "-1", "elem_charge": "-1"} |
5 | bfield,length,mass,resistance,time | m·ℓ·t·R·B | em,mechanics | m·ℓ⁻²·t⁻¹·R·B⁻² | m = k₀ · ℓ²·t·R⁻¹·B² | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "-2", "time": "-1", "resistance": "1", "bfield": "-2"} |
5 | length,mag_flux,mass,resistance,time | m·ℓ·t·R·Φ | em,mechanics | m·ℓ²·t⁻¹·R·Φ⁻² | m = k₀ · ℓ⁻²·t·R⁻¹·Φ² | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-1", "resistance": "1", "mag_flux": "-2"} |
5 | elem_charge,length,mass,resistance,time | m·ℓ·t·R·e | constants,em,mechanics | m·ℓ²·t⁻¹·R⁻¹·e⁻² | m = k₀ · ℓ⁻²·t·R·e² | null | 1 | 3 | 2 | 7 | 6.1 | 2.9 | false | {"mass": "1", "length": "2", "time": "-1", "resistance": "-1", "elem_charge": "-2"} |
5 | capacitance,elem_charge,length,mass,time | m·ℓ·t·C_e·e | constants,em,mechanics | m·ℓ²·t⁻²·C_e·e⁻² | m = k₀ · ℓ⁻²·t²·C_e⁻¹·e² | null | 1 | 3 | 2 | 8 | 6.8 | 2.2 | false | {"mass": "1", "length": "2", "time": "-2", "capacitance": "1", "elem_charge": "-2"} |
5 | bfield,inductance,length,mass,time | m·ℓ·t·L_e·B | em,mechanics | m·ℓ⁻²·t⁻²·L_e·B⁻² | m = k₀ · ℓ²·t²·L_e⁻¹·B² | null | 0 | 2 | 2 | 8 | 6.2 | 3.3 | true | {"mass": "1", "length": "-2", "time": "-2", "inductance": "1", "bfield": "-2"} |
5 | inductance,length,mag_flux,mass,time | m·ℓ·t·L_e·Φ | em,mechanics | m·ℓ²·t⁻²·L_e·Φ⁻² | m = k₀ · ℓ⁻²·t²·L_e⁻¹·Φ² | null | 0 | 2 | 2 | 8 | 6.2 | 3.3 | true | {"mass": "1", "length": "2", "time": "-2", "inductance": "1", "mag_flux": "-2"} |
5 | efield,length,mass,permittivity,time | m·ℓ·t·E_f·ε | em,mechanics | m·ℓ⁻¹·t⁻²·E_f⁻²·ε⁻¹ | m = k₀ · ℓ·t²·E_f²·ε | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "-1", "time": "-2", "efield": "-2", "permittivity": "-1"} |
5 | efield,length,mass,permeability,time | m·ℓ·t·E_f·μ₀ | em,mechanics | m·ℓ·t⁻⁴·E_f⁻²·μ₀ | m = k₀ · ℓ⁻¹·t⁴·E_f²·μ₀⁻¹ | null | 0 | 2 | 4 | 9 | 7.9 | 1.6 | false | {"mass": "1", "length": "1", "time": "-4", "efield": "-2", "permeability": "1"} |
5 | conductivity,efield,length,mass,time | m·ℓ·t·E_f·σ | em,mechanics | m·ℓ⁻¹·t⁻³·E_f⁻²·σ⁻¹ | m = k₀ · ℓ·t³·E_f²·σ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "-1", "time": "-3", "efield": "-2", "conductivity": "-1"} |
5 | efield,length,mass,resistivity,time | m·ℓ·t·E_f·ρ_e | em,mechanics | m·ℓ⁻¹·t⁻³·E_f⁻²·ρ_e | m = k₀ · ℓ·t³·E_f²·ρ_e⁻¹ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "-1", "time": "-3", "efield": "-2", "resistivity": "1"} |
5 | efield,elem_charge,length,mass,time | m·ℓ·t·E_f·e | constants,em,mechanics | m·ℓ·t⁻²·E_f⁻¹·e⁻¹ | m = k₀ · ℓ⁻¹·t²·E_f·e | null | 1 | 3 | 2 | 6 | 5.4 | 3.6 | false | {"mass": "1", "length": "1", "time": "-2", "efield": "-1", "elem_charge": "-1"} |
5 | bfield,length,mass,permeability,time | m·ℓ·t·B·μ₀ | em,mechanics | m·ℓ⁻¹·t⁻²·B⁻²·μ₀ | m = k₀ · ℓ·t²·B²·μ₀⁻¹ | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "-1", "time": "-2", "bfield": "-2", "permeability": "1"} |
5 | bfield,conductivity,length,mass,time | m·ℓ·t·B·σ | em,mechanics | m·ℓ⁻³·t⁻¹·B⁻²·σ⁻¹ | m = k₀ · ℓ³·t·B²·σ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "-3", "time": "-1", "bfield": "-2", "conductivity": "-1"} |
5 | bfield,length,mass,resistivity,time | m·ℓ·t·B·ρ_e | em,mechanics | m·ℓ⁻³·t⁻¹·B⁻²·ρ_e | m = k₀ · ℓ³·t·B²·ρ_e⁻¹ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "-3", "time": "-1", "bfield": "-2", "resistivity": "1"} |
5 | length,mag_flux,mass,permeability,time | m·ℓ·t·Φ·μ₀ | em,mechanics | m·ℓ³·t⁻²·Φ⁻²·μ₀ | m = k₀ · ℓ⁻³·t²·Φ²·μ₀⁻¹ | null | 0 | 2 | 3 | 9 | 7.4 | 2.1 | false | {"mass": "1", "length": "3", "time": "-2", "mag_flux": "-2", "permeability": "1"} |
5 | conductivity,length,mag_flux,mass,time | m·ℓ·t·Φ·σ | em,mechanics | m·ℓ·t⁻¹·Φ⁻²·σ⁻¹ | m = k₀ · ℓ⁻¹·t·Φ²·σ | null | 0 | 2 | 2 | 6 | 4.8 | 4.7 | true | {"mass": "1", "length": "1", "time": "-1", "mag_flux": "-2", "conductivity": "-1"} |
5 | length,mag_flux,mass,resistivity,time | m·ℓ·t·Φ·ρ_e | em,mechanics | m·ℓ·t⁻¹·Φ⁻²·ρ_e | m = k₀ · ℓ⁻¹·t·Φ²·ρ_e⁻¹ | null | 0 | 2 | 2 | 6 | 4.8 | 4.7 | true | {"mass": "1", "length": "1", "time": "-1", "mag_flux": "-2", "resistivity": "1"} |
5 | elem_charge,length,mag_flux,mass,time | m·ℓ·t·Φ·e | constants,em,mechanics | m·ℓ²·t⁻¹·Φ⁻¹·e⁻¹ | m = k₀ · ℓ⁻²·t·Φ·e | null | 1 | 3 | 2 | 6 | 5.4 | 3.6 | false | {"mass": "1", "length": "2", "time": "-1", "mag_flux": "-1", "elem_charge": "-1"} |
5 | elem_charge,length,mass,permittivity,time | m·ℓ·t·ε·e | constants,em,mechanics | m·ℓ³·t⁻²·ε·e⁻² | m = k₀ · ℓ⁻³·t²·ε⁻¹·e² | null | 1 | 3 | 3 | 9 | 8 | 1 | false | {"mass": "1", "length": "3", "time": "-2", "permittivity": "1", "elem_charge": "-2"} |
5 | conductivity,elem_charge,length,mass,time | m·ℓ·t·σ·e | constants,em,mechanics | m·ℓ³·t⁻¹·σ·e⁻² | m = k₀ · ℓ⁻³·t·σ⁻¹·e² | null | 1 | 3 | 3 | 8 | 7.3 | 1.7 | false | {"mass": "1", "length": "3", "time": "-1", "conductivity": "1", "elem_charge": "-2"} |
5 | elem_charge,length,mass,resistivity,time | m·ℓ·t·ρ_e·e | constants,em,mechanics | m·ℓ³·t⁻¹·ρ_e⁻¹·e⁻² | m = k₀ · ℓ⁻³·t·ρ_e·e² | null | 1 | 3 | 3 | 8 | 7.3 | 1.7 | false | {"mass": "1", "length": "3", "time": "-1", "resistivity": "-1", "elem_charge": "-2"} |
5 | amount,length,mass,molar_energy,time | m·ℓ·t·n·E_m | chemistry,mechanics | m·ℓ²·t⁻²·n⁻¹·E_m⁻¹ | m = k₀ · ℓ⁻²·t²·n·E_m | null | 0 | 2 | 2 | 7 | 5.5 | 4 | true | {"mass": "1", "length": "2", "time": "-2", "amount": "-1", "molar_energy": "-1"} |
5 | concentration,length,mass,molar_energy,time | m·ℓ·t·c_n·E_m | chemistry,mechanics | m·ℓ⁻¹·t⁻²·c_n⁻¹·E_m⁻¹ | m = k₀ · ℓ·t²·c_n·E_m | null | 0 | 2 | 2 | 6 | 4.8 | 4.7 | true | {"mass": "1", "length": "-1", "time": "-2", "concentration": "-1", "molar_energy": "-1"} |
6 | boltzmann,gas_constant,length,mass,molar_energy,time | m·ℓ·t·E_m·R·k_B | chemistry,constants,mechanics | m·ℓ²·t⁻²·E_m⁻¹·R·k_B⁻¹ | m = k₀ · ℓ⁻²·t²·E_m·R⁻¹·k_B | null | 1 | 3 | 2 | 8 | 7.1 | 1.9 | false | {"mass": "1", "length": "2", "time": "-2", "molar_energy": "-1", "gas_constant": "1", "boltzmann": "-1"} |
5 | cat_activity,length,mass,molar_energy,time | m·ℓ·t·E_m·z | chemistry,mechanics | m·ℓ²·t⁻³·E_m⁻¹·z⁻¹ | m = k₀ · ℓ⁻²·t³·E_m·z | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "2", "time": "-3", "molar_energy": "-1", "cat_activity": "-1"} |
5 | avogadro,length,mass,molar_energy,time | m·ℓ·t·E_m·N_A | chemistry,constants,mechanics | m·ℓ²·t⁻²·E_m⁻¹·N_A | m = k₀ · ℓ⁻²·t²·E_m·N_A⁻¹ | null | 1 | 3 | 2 | 7 | 6.1 | 2.9 | false | {"mass": "1", "length": "2", "time": "-2", "molar_energy": "-1", "avogadro": "1"} |
4 | grav_const,length,mass,time | m·ℓ·t·G | constants,mechanics | m·ℓ⁻³·t²·G | m = k₀ · ℓ³·t⁻²·G⁻¹ | null | 1 | 2 | 3 | 7 | 5.7 | 3.8 | true | {"mass": "1", "length": "-3", "time": "2", "grav_const": "1"} |
4 | length,mass,planck,time | m·ℓ·t·h | constants,mechanics | m·ℓ²·t⁻¹·h⁻¹ | m = k₀ · ℓ⁻²·t·h | null | 1 | 2 | 2 | 5 | 3.8 | 5.7 | true | {"mass": "1", "length": "2", "time": "-1", "planck": "-1"} |
4 | force,length,mass,velocity | m·ℓ·v·F | mechanics | m·ℓ⁻¹·v²·F⁻¹ | m = k₀ · ℓ·v⁻²·F | null | 0 | 1 | 2 | 5 | 3.2 | 6.8 | true | {"mass": "1", "length": "-1", "velocity": "2", "force": "-1"} |
4 | length,mass,power,velocity | m·ℓ·v·P | mechanics | m·ℓ⁻¹·v³·P⁻¹ | m = k₀ · ℓ·v⁻³·P | null | 0 | 1 | 3 | 6 | 4.4 | 5.6 | true | {"mass": "1", "length": "-1", "velocity": "3", "power": "-1"} |
4 | ang_momentum,length,mass,velocity | m·ℓ·v·Lₐ | mechanics | m·ℓ·v·Lₐ⁻¹ | m = k₀ · ℓ⁻¹·v⁻¹·Lₐ | null | 0 | 1 | 1 | 4 | 2 | 8 | true | {"mass": "1", "length": "1", "velocity": "1", "ang_momentum": "-1"} |
4 | action,length,mass,velocity | m·ℓ·v·S | mechanics | m·ℓ·v·S⁻¹ | m = k₀ · ℓ⁻¹·v⁻¹·S | null | 0 | 1 | 1 | 4 | 2 | 8 | true | {"mass": "1", "length": "1", "velocity": "1", "action": "-1"} |
4 | length,mass,pressure,velocity | m·ℓ·v·P_p | mechanics | m·ℓ⁻³·v²·P_p⁻¹ | m = k₀ · ℓ³·v⁻²·P_p | null | 0 | 1 | 3 | 7 | 5.1 | 4.9 | true | {"mass": "1", "length": "-3", "velocity": "2", "pressure": "-1"} |
4 | length,mass,velocity,viscosity | m·ℓ·v·μ | mechanics | m·ℓ⁻²·v·μ⁻¹ | m = k₀ · ℓ²·v⁻¹·μ | null | 0 | 1 | 2 | 5 | 3.2 | 6.8 | true | {"mass": "1", "length": "-2", "velocity": "1", "viscosity": "-1"} |
4 | length,mass,stiffness,velocity | m·ℓ·v·k | mechanics | m·ℓ⁻²·v²·k⁻¹ | m = k₀ · ℓ²·v⁻²·k | null | 0 | 1 | 2 | 6 | 3.9 | 6.1 | true | {"mass": "1", "length": "-2", "velocity": "2", "stiffness": "-1"} |
4 | length,mass,surf_tension,velocity | m·ℓ·v·γ | mechanics | m·ℓ⁻²·v²·γ⁻¹ | m = k₀ · ℓ²·v⁻²·γ | null | 0 | 1 | 2 | 6 | 3.9 | 6.1 | true | {"mass": "1", "length": "-2", "velocity": "2", "surf_tension": "-1"} |
5 | length,mass,temperature,thermal_cond,velocity | m·ℓ·v·Θ·κ | mechanics,thermo | m·ℓ⁻²·v³·Θ⁻¹·κ⁻¹ | m = k₀ · ℓ²·v⁻³·Θ·κ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "-2", "velocity": "3", "temperature": "-1", "thermal_cond": "-1"} |
6 | concentration,gas_constant,length,mass,temperature,velocity | m·ℓ·v·Θ·c_n·R | chemistry,mechanics,thermo | m·ℓ⁻³·v²·Θ⁻¹·c_n⁻¹·R⁻¹ | m = k₀ · ℓ³·v⁻²·Θ·c_n·R | null | 0 | 3 | 3 | 9 | 8.3 | 0.7 | false | {"mass": "1", "length": "-3", "velocity": "2", "temperature": "-1", "concentration": "-1", "gas_constant": "-1"} |
6 | cat_activity,gas_constant,length,mass,temperature,velocity | m·ℓ·v·Θ·R·z | chemistry,mechanics,thermo | m·ℓ⁻¹·v³·Θ⁻¹·R⁻¹·z⁻¹ | m = k₀ · ℓ·v⁻³·Θ·R·z | null | 0 | 3 | 3 | 8 | 7.6 | 1.4 | false | {"mass": "1", "length": "-1", "velocity": "3", "temperature": "-1", "gas_constant": "-1", "cat_activity": "-1"} |
5 | length,mass,specific_heat,thermal_cond,velocity | m·ℓ·v·c·κ | mechanics,thermo | m·ℓ⁻²·v·c·κ⁻¹ | m = k₀ · ℓ²·v⁻¹·c⁻¹·κ | null | 0 | 2 | 2 | 6 | 4.8 | 4.7 | true | {"mass": "1", "length": "-2", "velocity": "1", "specific_heat": "1", "thermal_cond": "-1"} |
6 | cat_activity,gas_constant,length,mass,specific_heat,velocity | m·ℓ·v·c·R·z | chemistry,mechanics,thermo | m·ℓ⁻¹·v·c·R⁻¹·z⁻¹ | m = k₀ · ℓ·v⁻¹·c⁻¹·R·z | null | 0 | 3 | 1 | 6 | 5.2 | 3.8 | false | {"mass": "1", "length": "-1", "velocity": "1", "specific_heat": "1", "gas_constant": "-1", "cat_activity": "-1"} |
5 | expansion,length,mass,thermal_cond,velocity | m·ℓ·v·κ·β | mechanics,thermo | m·ℓ⁻²·v³·κ⁻¹·β | m = k₀ · ℓ²·v⁻³·κ·β⁻¹ | null | 0 | 2 | 3 | 8 | 6.7 | 2.8 | true | {"mass": "1", "length": "-2", "velocity": "3", "thermal_cond": "-1", "expansion": "1"} |
6 | gas_constant,length,mass,molar_mass,thermal_cond,velocity | m·ℓ·v·κ·M_m·R | chemistry,mechanics,thermo | m·ℓ⁻²·v·κ⁻¹·M_m⁻¹·R | m = k₀ · ℓ²·v⁻¹·κ·M_m·R⁻¹ | null | 0 | 3 | 2 | 7 | 6.4 | 2.6 | false | {"mass": "1", "length": "-2", "velocity": "1", "thermal_cond": "-1", "molar_mass": "-1", "gas_constant": "1"} |
6 | gas_constant,length,mass,molar_energy,thermal_cond,velocity | m·ℓ·v·κ·E_m·R | chemistry,mechanics,thermo | m·ℓ⁻²·v³·κ⁻¹·E_m⁻¹·R | m = k₀ · ℓ²·v⁻³·κ·E_m·R⁻¹ | null | 0 | 3 | 3 | 9 | 8.3 | 0.7 | false | {"mass": "1", "length": "-2", "velocity": "3", "thermal_cond": "-1", "molar_energy": "-1", "gas_constant": "1"} |
PhysicsBabel — A Complete Catalogue of Dimensionally-Consistent Physics Equations
Vashy is an exhaustive, machine-generated catalogue of every irreducible dimensionless relation that can be formed from a curated pool of 60 physical quantities spanning all of classical physics. It is built directly from the Vaschy–Buckingham π theorem: any physically meaningful equation must be dimensionally homogeneous, so the set of dimensionally-consistent monomials is exactly the set of dimensionless products the theorem describes.
Each of the 2,325,320 rows is one such relation — for example
F = k₀ · m·a (Newton's second law), ℓ = k₀ · v⁻¹·ρ⁻¹·μ (the Reynolds
number), or m = k₀ · E·c₀⁻² (mass–energy equivalence) — annotated with
metrics that let you filter the physically meaningful laws out of the vast space
of mere dimensional coincidences.
k₀denotes the dimensionless constant of order unity that dimensional analysis cannot determine (e.g. the ½ in kinetic energy, or 6π in Stokes' drag). This is an intrinsic limitation of the method, not of the dataset.
What is in the dataset
The catalogue is complete: it contains every minimal dimensionless
relation of size 2 to 8 over the quantity pool. Size 8 is a hard mathematical
ceiling — with 7 SI base dimensions, no irreducible relation can involve more
than 8 quantities (a relation of k quantities needs rank k−1 ≤ 7).
| # quantities | rows | note |
|---|---|---|
| 2 | 22 | pairs with identical dimensions (e.g. energy vs torque) |
| 3 | 593 | e.g. F = k₀·m·a, E = k₀·m·v² |
| 4 | 17,325 | e.g. Reynolds, Weber, Strouhal numbers |
| 5 | 280,646 | |
| 6 | 813,919 | |
| 7 | 1,140,445 | |
| 8 | 72,370 | must span all 7 base dimensions at once (rare) |
| Total | 2,325,320 |
Of these, 46,720 are flagged plausible (a conservative gate for genuine
physical candidates) and 20 correspond to classically named laws / numbers.
Provenance & method
Every quantity is represented as a vector of integer exponents over the seven SI base dimensions. A dimensionless relation among a set of quantities is an integer null vector of the matrix whose columns are those dimension vectors.
A row in this dataset is a circuit of that "dimensional matroid": a
minimal dependent set, where every quantity is essential (removing any one
destroys the dimensionless product) and which is not a product of smaller
relations. Formally, a set of n quantities is a circuit iff its dimension
matrix has rank n−1 and the (unique) null vector has full support. Each
circuit corresponds to exactly one irreducible dimensionless number, and the
catalogue enumerates all of them without duplication.
Dimensional analysis fixes only the form of a law up to k₀; it does not
prove physical existence. That is why the dataset ships with relevance metrics
rather than claiming every row is a real law.
Dataset structure
A single split (default) backed by data/circuits.parquet (~108 MB, zstd).
| column | type | description |
|---|---|---|
size |
int | number of quantities in the relation (2–8) |
keys |
string | sorted, comma-separated quantity keys (the relation's identity) |
symbols |
string | the quantities' symbols, ·-joined |
domains |
string | distinct physics domains involved, comma-separated |
pi |
string | the dimensionless number (Π group), e.g. ℓ·v·ρ·μ⁻¹ |
equation |
string | the relation solved for one quantity, e.g. ℓ = k₀ · v⁻¹·ρ⁻¹·μ |
name |
string | null | recognized name of the law / dimensionless number, if any |
n_const |
int | number of universal constants (c₀, G, h, k_B, e, N_A) involved |
n_domains |
int | number of distinct physics domains bridged |
max_exp |
int | largest absolute exponent in the monomial |
exp_l1 |
int | sum of absolute exponents (monomial "weight") |
complexity |
float | composite complexity score (lower = simpler) |
score |
float | composite physicality score (higher = more plausible) |
plausible |
bool | passes the conservative physicality gate (see below) |
exponents |
string (JSON) | {quantity_key: integer_exponent} for the dimensionless monomial |
The plausible gate
A row is flagged plausible = true when it satisfies all of:
size ≤ 5— real laws rarely couple more than five quantities;n_const ≤ 1— a genuine law uses at most one universal constant;n_domains ≤ 2— at most one cross-domain bridge;max_exp ≤ 3andexp_l1 ≤ 8— small integer exponents.
This is intentionally conservative: it favours precision over recall. The
remaining ~2.28 M rows are kept so that the catalogue stays complete and
auditable, but the overwhelming majority are dimensional coincidences (e.g.
m = k₀ · c⁻¹·k_B), not physical laws.
The score
A heuristic that rewards simplicity (few quantities, small exponents, single
domain, at most one constant). Sorting plausible rows by score DESC surfaces
textbook laws and named dimensionless numbers first.
Example rows
| equation | pi | name | size | score | plausible |
|---|---|---|---|---|---|
m = k₀ · a⁻¹·F |
m·a·F⁻¹ |
Newton 2nd law | 3 | 9.0 | ✅ |
m = k₀ · v⁻²·E |
m·v²·E⁻¹ |
kinetic energy | 3 | 7.8 | ✅ |
m = k₀ · E·c₀⁻² |
m·E⁻¹·c₀² |
mass-energy (E=mc²) | 3 | 6.7 | ✅ |
ℓ = k₀ · v⁻¹·ρ⁻¹·μ |
ℓ·v·ρ·μ⁻¹ |
Reynolds number | 4 | 8.0 | ✅ |
E = k₀ · f·h |
E·f⁻¹·h⁻¹ |
Planck relation (E=hf) | 3 | — | ✅ |
i = k₀ · U·R⁻¹ |
i·U⁻¹·R |
Ohm's law | 3 | — | ✅ |
The quantity pool (60 quantities, 7 base dimensions)
Base dimensions: M (mass), L (length), T (time), Θ (temperature), I (electric current), N (amount of substance), J (luminous intensity).
Mechanics
| symbol | quantity | dimensions |
|---|---|---|
| m | mass | M |
| ℓ | length | L |
| t | time | T |
| v | velocity | L·T⁻¹ |
| a | acceleration | L·T⁻² |
| g | gravitational acceleration | L·T⁻² |
| F | force | M·L·T⁻² |
| E | energy | M·L²·T⁻² |
| τ | torque | M·L²·T⁻² |
| P | power | M·L²·T⁻³ |
| p | momentum | M·L·T⁻¹ |
| Lₐ | angular momentum | M·L²·T⁻¹ |
| S | action | M·L²·T⁻¹ |
| J | moment of inertia | M·L² |
| P_p | pressure | M·L⁻¹·T⁻² |
| ρ | mass density | M·L⁻³ |
| μ | dynamic viscosity | M·L⁻¹·T⁻¹ |
| ν | kinematic viscosity | L²·T⁻¹ |
| ω | angular velocity | T⁻¹ |
| f | frequency | T⁻¹ |
| k | spring constant | M·T⁻² |
| γ | surface tension | M·T⁻² |
| A | area | L² |
| V | volume | L³ |
| Q | volumetric flow rate | L³·T⁻¹ |
Thermodynamics
| symbol | quantity | dimensions |
|---|---|---|
| Θ | temperature | Θ |
| S_e | entropy | M·L²·T⁻²·Θ⁻¹ |
| C | heat capacity | M·L²·T⁻²·Θ⁻¹ |
| c | specific heat capacity | L²·T⁻²·Θ⁻¹ |
| κ | thermal conductivity | M·L·T⁻³·Θ⁻¹ |
| α | thermal diffusivity | L²·T⁻¹ |
| β | thermal expansion coefficient | Θ⁻¹ |
Electromagnetism
| symbol | quantity | dimensions |
|---|---|---|
| q | electric charge | T·I |
| i | electric current | I |
| U | electric potential | M·L²·T⁻³·I⁻¹ |
| R | electric resistance | M·L²·T⁻³·I⁻² |
| C_e | capacitance | M⁻¹·L⁻²·T⁴·I² |
| L_e | inductance | M·L²·T⁻²·I⁻² |
| E_f | electric field | M·L·T⁻³·I⁻¹ |
| B | magnetic flux density | M·T⁻²·I⁻¹ |
| Φ | magnetic flux | M·L²·T⁻²·I⁻¹ |
| ε | permittivity | M⁻¹·L⁻³·T⁴·I² |
| μ₀ | permeability | M·L·T⁻²·I⁻² |
| σ | electrical conductivity | M⁻¹·L⁻³·T³·I² |
| ρ_e | electrical resistivity | M·L³·T⁻³·I⁻² |
Chemistry
| symbol | quantity | dimensions |
|---|---|---|
| n | amount of substance | N |
| M_m | molar mass | M·N⁻¹ |
| c_n | molar concentration | L⁻³·N |
| E_m | molar energy | M·L²·T⁻²·N⁻¹ |
| R | molar gas constant | M·L²·T⁻²·Θ⁻¹·N⁻¹ |
| z | catalytic activity | T⁻¹·N |
Photometry
| symbol | quantity | dimensions |
|---|---|---|
| I_v | luminous intensity | J |
| E_v | illuminance | L⁻²·J |
| L_v | luminance | L⁻²·J |
Universal constants
| symbol | quantity | dimensions |
|---|---|---|
| c₀ | speed of light | L·T⁻¹ |
| G | gravitational constant | M⁻¹·L³·T⁻² |
| h | Planck constant | M·L²·T⁻¹ |
| k_B | Boltzmann constant | M·L²·T⁻²·Θ⁻¹ |
| e | elementary charge | T·I |
| N_A | Avogadro constant | N⁻¹ |
Loading
import pandas as pd
df = pd.read_parquet("data/circuits.parquet")
# the physically-plausible laws, best first
laws = df[df.plausible].sort_values("score", ascending=False)
# every relation involving viscosity, within mechanics
df[df["keys"].str.contains("viscosity") & (df.domains == "mechanics")]
Or with the 🤗 datasets library:
from datasets import load_dataset
ds = load_dataset("<user>/vashy", split="train")
Intended uses
- Symbolic regression & scientific ML: a dimensionally-valid hypothesis space / prior over candidate equations.
- Physics education: browsing dimensionless numbers and their structure.
- Benchmarking: testing whether models can recover known laws from dimensional constraints.
Limitations & caveats
- Dimensional consistency ≠ physical truth. Most rows are coincidences; use
plausibleandscore, and validate against physics. - The constant
k₀is undetermined by dimensional analysis. - Only single dimensionless numbers are represented. When a phenomenon needs
two or more independent Π groups, the true law is
Π₁ = f(Π₂, …)with an arbitrary functionf; the dataset lists the individual irreducible Π groups (the circuits), not the functional relation between them. - Pool-dependent. The catalogue is exhaustive for this 60-quantity pool; a different pool yields a different catalogue.
- Deliberate dimensional collisions in the pool (energy vs torque, action vs angular momentum, entropy vs heat capacity, acceleration vs gravity) are real and produce legitimate size-2 identities.
License
Released under CC-BY-4.0. The underlying facts are mathematical consequences of SI dimensional definitions.
Citation
@misc{r&d_mediation_2026,
author = { R&D Mediation },
title = { PhysicsBabel (Revision 963a461) },
year = 2026,
url = { https://huggingface.co/datasets/RANDMEDIATION/PhysicsBabel },
doi = { 10.57967/hf/9544 },
publisher = { Hugging Face }
}
Discovering equations by AI
For instance, charge × flux = angular momentum
The product of charge × magnetic flux has the dimensions of an action and of an angular momentum: [C]·[Wb] = [J·s]. This isn't a coincidence — it's the backbone of three chapters of quantum physics:
est une phase → l'effet Aharonov–Bohm ;
: le champ électromagnétique...
→ la quantification du flux...
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