original_non_native_audio audioduration (s) 1.2 24.9 | parallel_native_audio audioduration (s) 0.17 29 | golden_speaker_audio audioduration (s) 1.2 24.9 | transcript stringlengths 1 537 | speaker_id stringclasses 30 values | utterance_id stringlengths 16 19 |
|---|---|---|---|---|---|
(()) (25:14) I am telling you why armature should be in the stator for that I am giving so much of justification | c76CnTH8_y4 | 01010292_st1513p200 | |||
Please note, very clearly induction machine is going to draw a higher current as compared to the synchronous machine | c76CnTH8_y4 | 01010467_st2935p040 | |||
So, I might have to bring the neutral also which will correspond to the 4 slip rings | c76CnTH8_y4 | 01010271_st1317p760 | |||
So, I say that 1 megawatt synchronous machine and 1 megawatt induction machine | c76CnTH8_y4 | 01010458_st2880p880 | |||
So essentially the speed at which my prime mover is rotating the magnet that is basically known as the synchronous speed, which will decide what frequency is induce in each of the phase windings | c76CnTH8_y4 | 01010180_st475p920 | |||
So this is one of the greatest advantages of the synchronous machine | c76CnTH8_y4 | 01010450_st2834p400 | |||
So you are going to have basically the brushes connected through the slip rings back to the winding | c76CnTH8_y4 | 01010275_st1342p560 | |||
So the DC excitation actually is going to allow me to adjust the power factor of the stator side of a synchronous machine | c76CnTH8_y4 | 01010430_st2633p760 | |||
So, if I have two poles, I should have this rotating in such a way that I am going to have basically positive half cycle is induced here and negative half cycle is induced at the same point in A dash at the same instant of time in A dash | c76CnTH8_y4 | 01010172_st413p760 | |||
This is the synchronous speed, what we were talking about, even in the case of induction machine | c76CnTH8_y4 | 01010310_st1653p040 | |||
Induction machine cost is normally 1 hp cost Rs | c76CnTH8_y4 | 01010475_st3023p520 | |||
That is when I will be able to get exactly 50 hertz verse the induce EMF in my actual, you know the winding itself | c76CnTH8_y4 | 01010170_st391p520 | |||
So the construction is not easy when if it has to be in the rotor | c76CnTH8_y4 | 01010301_st1562p080 | |||
I am rather saying if it is 50 hp machine, roughly it is Rs | c76CnTH8_y4 | 01010479_st3040p080 | |||
So in the stator I am probably going to have three phase windings, so let me call this as A and A dash | c76CnTH8_y4 | 01010141_st152p640 | |||
So, what I require from the rotor, if I say that this is essentially armature in the rotor | c76CnTH8_y4 | 01010287_st1476p480 | |||
So, if I am talking about a 400 MVA alternator with let us say 11 kilo volt generating voltage, right, maybe three phase star connected | c76CnTH8_y4 | 01010258_st1199p920 | |||
It is number of poles | c76CnTH8_y4 | 01010312_st1663p440 | |||
If the rotor excitation, so if I am going to have the rotor excitation providing phi needed | c76CnTH8_y4 | 01010413_st2448p320 | |||
Normally, most of the synchronous machines are going to have a rating of several hundreds of MVA | c76CnTH8_y4 | 01010256_st1179p440 | |||
I have not really checked, it should be close to about 2500 or 3000 amperes I should be getting quite a large value flowing as it is, if it is something like 2500 amperes, and if I am having, by chance, the armature in the rotor, if I just wanted to construct it for the heck of it with the armature in the stator | c76CnTH8_y4 | 01010264_st1246p000 | |||
I am going to have essentially a structure like this and I am going to have one pole here, one more pole here | c76CnTH8_y4 | 01010208_st769p920 | |||
The rotor has some weight; it is not weightless | c76CnTH8_y4 | 01010424_st2569p360 | |||
So, we are going to generally see that wherever very large capacity applications are talked about, where I am extremely concerned about the efficiency, synchronous machines generally are the first choices | c76CnTH8_y4 | 01010472_st2989p360 | |||
5, if I go slow, then I gave rotor enough time to catch up with the stator revolving magnetic field | c76CnTH8_y4 | 01010375_st2124p160 | |||
But it will be at a different frequency, if the speed is different | c76CnTH8_y4 | 01010328_st1761p360 | |||
So the revolutions per second or revolutions per minute indirectly decide what is the frequency which is being induced in individual phase windings | c76CnTH8_y4 | 01010171_st401p920 | |||
I will be able to make the rotor catch up with the stator reporting magnetic fields speed | c76CnTH8_y4 | 01010380_st2143p440 | |||
1000, generally, roughly | c76CnTH8_y4 | 01010476_st3032p480 | |||
So, cylindrical pole rotor is normally used in high speed alternator which is corresponding to steam turbine, right | c76CnTH8_y4 | 01010206_st750p160 | |||
These are the three phase voltages, so there are going to be three phase voltages that are generated | c76CnTH8_y4 | 01010148_st198p320 | |||
I am going to have the shaft here | c76CnTH8_y4 | 01010165_st339p360 | |||
I am going to get it only for more than 1 lakh rupees, so it is very costly compared to the induction machine | c76CnTH8_y4 | 01010489_st3067p280 | |||
If I am talking about the 30 hp synchronous motor, it will be greater than about 1 | c76CnTH8_y4 | 01010484_st3049p920 | |||
5, 2, 2 | c76CnTH8_y4 | 01010374_st2122p560 | |||
So because of which I am going to have the power factor lagging | c76CnTH8_y4 | 01010439_st2703p200 | |||
Maybe, I will have to bring out the neutral as well; very often I might have to bring out the neutral because the neutral will be normally grounded and the ground will also be connected to the body of the machine | c76CnTH8_y4 | 01010268_st1294p640 | |||
I was having field was always in the stator and armature was always in the rotor right | c76CnTH8_y4 | 01010248_st1124p720 | |||
We said that f divided by P by 2 is going to be the revolutions per second or I would say 2 f by P is the revolutions per second or I can say 120 f by P, many of the books say this | c76CnTH8_y4 | 01010308_st1623p440 | |||
If we increase the number of poles will it help in starting | c76CnTH8_y4 | 01010382_st2154p320 | |||
So, I would be able to get more and more frequencies, if I rotate the field system at a, you know higher speed or if I multiply the number of poles | c76CnTH8_y4 | 01010185_st527p360 | |||
So the construction becomes much more strenuous and cumbersome, when I am actually looking at all the 4 conductors being brought out to the external world through slip ring and brush arrangement | c76CnTH8_y4 | 01010280_st1384p240 | |||
So, I am looking at it this way, the total flux needed, I will call this as phi needed | c76CnTH8_y4 | 01010412_st2441p520 | |||
So, if I had to bring the field connections out, if it is residing in the rotor I have to bring the field connections out and the field connections when I bring out again, it will come through slip ring and brush, if I am talking about it sitting in the rotor | c76CnTH8_y4 | 01010284_st1434p240 | |||
So, synchronous motor has one major negative point that is, it is not self starting, especially, I am trying to start with 50 hertz | c76CnTH8_y4 | 01010371_st2106p400 | |||
In the case of synchronous machine, I am going to give three phase excitation to the stator and DC excitation to the rotor | c76CnTH8_y4 | 01010337_st1842p720 | |||
Either way, I should be able to get a higher frequency | c76CnTH8_y4 | 01010186_st540p720 | |||
And I am ultimately going to look at the torque produced because of the interaction between the rotor flux and maybe the stator current | c76CnTH8_y4 | 01010405_st2350p720 | |||
But I am going to have definitely no control over the excitation; the excitation is almost like a constant value | c76CnTH8_y4 | 01010241_st1059p360 | |||
Now, if I look at actually the synchronous machine, please understand that I am going to have excitation, especially in the motor; excitation is provided from the stator, excitation provided from the rotor, both sides | c76CnTH8_y4 | 01010392_st2236p560 | |||
I am going to have very clearly 1 into 10 power 6 divided by root 3 into 11 into 10 power 3 multiplied by 0 | c76CnTH8_y4 | 01010464_st2918p000 | |||
If it is a large structure rotating at a very high speed and if you actually look at the linear velocity what is going on around the rim of or around the peripheral surface of the rotor that is going to be enormously high | c76CnTH8_y4 | 01010195_st656p480 | |||
Now, it is going to draw reactive current, which means the power factor of the stator side is going to be actually lagging | c76CnTH8_y4 | 01010417_st2521p200 | |||
So I am going to give excitation in both the cases | c76CnTH8_y4 | 01010397_st2282p320 | |||
That is the reason why invariably we may simply have a cylindrical structure as the pole | c76CnTH8_y4 | 01010201_st714p080 | |||
So, whenever I am going to have a leading power factor operation of the synchronous motor it may work as a synchronous condenser, which will compensate for any reactive power drawn by any of the other induction machines and so on, or any other inductor in my factory | c76CnTH8_y4 | 01010449_st2810p880 | |||
So both of them put together ultimately makes up for the torque production | c76CnTH8_y4 | 01010437_st2687p600 | |||
5 hertz, 1 hertz, 1 | c76CnTH8_y4 | 01010378_st2139p920 | |||
So, synchronous motor is not going to be self starting | c76CnTH8_y4 | 01010387_st2206p320 | |||
So, we can have the other way round also it would have work | c76CnTH8_y4 | 01010299_st1553p600 | |||
So, it should happen 50 times probably in 1 second, right | c76CnTH8_y4 | 01010169_st386p480 | |||
Armature reaction here is much more complex than what we see in a DC machine because it is a phasor, right | c76CnTH8_y4 | 01010400_st2300p800 | |||
So the overall flux in the air gap or magnetism in the air gap is resultant of the stator flux and rotor flux | c76CnTH8_y4 | 01010398_st2285p600 | |||
Now, this flux, when they are aligning with each other that is what actually creates my overall torque | c76CnTH8_y4 | 01010402_st2321p680 | |||
So, that actually gives me definitely the advantage of not having any winding, I will not have any I square R losses corresponding to the field | c76CnTH8_y4 | 01010240_st1049p440 | |||
Whereas for a synchronous machine | c76CnTH8_y4 | 01010483_st3047p920 | |||
In this particular case, it works, as though the rotor current component is actually drawn from the armature three phase supply | c76CnTH8_y4 | 01010434_st2660p320 | |||
Then what is going to happen is the North Pole is going to be faced by A phase winding itself twice in which case the frequency of the induced EMF can increase further | c76CnTH8_y4 | 01010184_st515p120 | |||
When they are trying to align with each other, that is what is creating the torque in my machine | c76CnTH8_y4 | 01010403_st2331p440 | |||
And maybe the magnet is rotated in this direction | c76CnTH8_y4 | 01010317_st1698p240 | |||
It is not singly excited; this is doubly excited | c76CnTH8_y4 | 01010394_st2260p320 | |||
And I am going to have the A phase, B phase and C phase windings sitting here | c76CnTH8_y4 | 01010316_st1691p200 | |||
It has to have certain magnitude, unless it has sufficient magnitude | c76CnTH8_y4 | 01010422_st2561p440 | |||
So, if I want is 50 hertz, basically I should also have these North Pole coming into contact with A phase winding corresponding to 50 hertz | c76CnTH8_y4 | 01010168_st374p400 | |||
We talked about disadvantage, so I wanted to tell you about the advantage as well | c76CnTH8_y4 | 01010451_st2839p520 | |||
So, if I am going to several hundreds of MVA – Mega Volt Ampere, maybe I am going to have 500 400 MVA minimum | c76CnTH8_y4 | 01010257_st1189p920 | |||
The rotor has to catch up with the stator revolving magnetic field, which it will not be able to do right away because it has certain inertia | c76CnTH8_y4 | 01010347_st1901p280 | |||
It will not have a power rating more than that, which means the currents and the voltages; everything will be somewhat limited in the field | c76CnTH8_y4 | 01010283_st1424p560 | |||
I am not going to be able to pull the rotor right | c76CnTH8_y4 | 01010423_st2565p840 | |||
Synchronous condenser, condenser is a word for capacitor | c76CnTH8_y4 | 01010447_st2802p240 | |||
So, I have excited both stator as well as rotor windings | c76CnTH8_y4 | 01010338_st1860p400 | |||
So, I would say around 500 rpm it can be sometimes less as well | c76CnTH8_y4 | 01010136_st118p640 | |||
So 120 f by P is the revolutions per minute, okay | c76CnTH8_y4 | 01010309_st1645p760 | |||
First, I am going to have induced EMF in A and A dash, then after 120 degrees because exactly B phase winding is displaced by 120 degrees, I am going to have induced EMF in B | c76CnTH8_y4 | 01010157_st266p160 | |||
Cylindrical rotor structure generally conforms to very large velocity, whereas salient pole structure generally will correspond to smaller velocities and smaller speeds are generally in hydro alternator and larger speeds are normally in steam turbine based power stations that is NTPC and NPC power station | c76CnTH8_y4 | 01010217_st834p960 | |||
If I have North Pole South Pole, North Pole South Pole created by the revolving magnetic field, correspondingly, I should have North Pole South Pole, North Pole South Pole in the rotor | c76CnTH8_y4 | 01010384_st2171p600 | |||
So that is something definitely called armature reaction here also, no doubt | c76CnTH8_y4 | 01010399_st2295p920 | |||
Now, what is going to happen is, I will have the three phase winding deciding in the stator, rotor and windings will be brought out and I have to put 3 slip rings | c76CnTH8_y4 | 01010265_st1270p160 | |||
If I have 2 pole machine, it is going to run at 3000 rpm or run, not run at all | c76CnTH8_y4 | 01010494_st3113p680 | |||
Induction motor is inherently self starting because it works on induction principle and the induced EMF that is happening actually in the rotor circuit is dependent upon the relative velocity | c76CnTH8_y4 | 01010361_st2034p640 | |||
Lately they have been produced for megawatts levels of rating | c76CnTH8_y4 | 01010224_st926p640 | |||
So, I am going to have essentially the voltages created which are shifted from each other by 120 degrees | c76CnTH8_y4 | 01010319_st1709p280 | |||
When I use a synchronous motor for providing for the reactive power, we may call that as synchronous condenser | c76CnTH8_y4 | 01010446_st2794p400 | |||
I am going to have one more pair which is actually B and B dash | c76CnTH8_y4 | 01010142_st164p160 | |||
So, the sprain is very precisely controlled for the prime over in all the power stations normally | c76CnTH8_y4 | 01010332_st1792p720 | |||
And second thing is permanent magnets are not very freely available and it is actually horded by China | c76CnTH8_y4 | 01010242_st1067p920 | |||
So, I would say that synchronous motor is a doubly excited machine | c76CnTH8_y4 | 01010393_st2254p480 | |||
I am trying to first of all discuss qualitatively the plus point, minus point, the basic working operation and things like that | c76CnTH8_y4 | 01010390_st2223p280 | |||
So, I will have depending upon how much is the excitation, the excitation is in excess some portion of the reactive power will be returned back to the main, three phase mains | c76CnTH8_y4 | 01010426_st2584p560 | |||
So if they are acting towards the protruding surfaces they can deform the winding, we do not want the deformation to happen, especially when they are working at very large speeds | c76CnTH8_y4 | 01010200_st702p640 |
GAPS: Golden-Aligned Parallel Speech Corpus
Overview
GAPS (Golden-Aligned Parallel Speech) is a multi-corpus dataset designed for foreign accent conversion.
The dataset provides parallel speech triplets consisting of:
- Original non-native speech
- Parallel native speech
- Golden speaker speech — synthetic speech that preserves the non-native speaker’s timbre and timing (including pauses) while exhibiting native pronunciation
along with the corresponding text transcript.
GAPS is constructed to support both offline accent conversion and streaming, low-latency pronunciation correction, and is used in our work on streaming foreign accent conversion for voice anonymization.
Dataset Structure
This repository extends the GAPS(https://huggingface.co/datasets/warisqr007/GAPS) to the NPTEL lecture corpus
The dataset contains the following main columns:
| Column name | Type | Description |
|---|---|---|
original |
Audio | Original non-native speech |
parallel_native |
Audio | Parallel native speech |
golden_speaker |
Audio | Golden speaker speech (synthetic) |
transcript |
string | Text transcription |
All audio is single-channel, 16 kHz.
Dataset Statistics
| Speakers | Duration (approx.) |
|---|---|
| TBD | TBD hours |
(Statistics will be updated soon.)
Data Construction
Source Corpora
GAPS-nptel extends GAPS to include NPTEL (BhasaAnuvaad) that contains lecture speech from Indian English speakers.
The original datasets are not redistributed in raw form.
GAPS provides processed, aligned, and synthesized derivatives, following the original licenses.
Golden Speaker Generation
Golden speaker utterances are generated entirely offline using a two-stage, reference-free accent conversion pipeline, redesigned for duration preservation and streaming compatibility.
For each non-native / native utterance pair:
1. Content Extraction
Linguistic content representations are extracted independently from the native and non-native utterances using a speaker-independent content encoder.
2. Silence-Aware DTW Alignment
- Voice Activity Detection (VAD) is applied to remove silence regions.
- Dynamic Time Warping (DTW) is performed in the content embedding space.
- Native content embeddings are temporally aligned to the non-native utterance.
- Silence segments are re-inserted to preserve the original non-native timing and rhythm.
3. Golden Speaker Synthesis
- Aligned native content embeddings provide native pronunciation.
- Non-native speaker embeddings provide speaker identity (timbre).
- Duration and rhythm follow the non-native utterance.
- Waveforms are synthesized using a zero-shot voice conversion system and neural vocoder.
The resulting golden speaker speech differs from the original non-native speech only in accent, making it suitable as supervision for pronunciation correction and accent translation.
Intended Use
GAPS is intended for research on:
- Foreign accent conversion (FAC)
- Accent-aware speaker anonymization
- Streaming pronunciation correction
- Accent analysis and evaluation
The dataset is not intended for commercial use, unless explicitly permitted under the original licenses.
Example Usage
from datasets import load_dataset
ds = load_dataset("warisqr007/GAPS-nptel")
# Access a specific split
sample = ds[0]
# Audio is loaded lazily
audio = sample["original"]
print(audio["sampling_rate"], audio["array"].shape)
print(sample["transcript"])
Licenses and Usage Terms
Each subset of GAPS follows the same license as its original dataset.
NPTEL / BhasaAnuvaad
- License: CC BY-NC 4.0
- Summary: https://creativecommons.org/licenses/by-nc/4.0/
- Full license: https://creativecommons.org/licenses/by-nc/4.0/legalcode
- Hugging Face dataset: https://huggingface.co/datasets/ai4bharat/NPTEL
This processed dataset follows the same license. For any usage not covered by this license, please contact the dataset authors and cite the BhasaAnuvaad paper.
Citation
If you use GAPS in your research, please cite:
GAPS (this dataset)
@article{gaps2026,
title = {GAPS: Golden-Aligned Parallel Speech Corpus for Accent Conversion and Anonymization},
author = {TBD},
journal = {TBD},
year = {2026}
}
(Placeholder — update once the paper is public.)
NPTEL / BhasaAnuvaad
@article{jain2024bhasaanuvaad,
title = {BhasaAnuvaad: A Speech Translation Dataset for 14 Indian Languages},
author = {Jain, Sparsh and Sankar, Ashwin and Choudhary, Devilal and Suman, Dhairya and Narasimhan, Nikhil and Khan, Mohammed Safi Ur Rahman and Kunchukuttan, Anoop and Khapra, Mitesh M and Dabre, Raj},
journal = {arXiv preprint arXiv:2411.04699},
year = {2024}
}
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