I have some signals which I add up to a larger signal, where each signal is located in a different frequency region.
Now, I perform the FFT operation on the big signal with FFTW and cut the concrete FFT bins (where the signals are located) out.
For example: The big signal is FFT transformed with 1024 points,
the sample rate of the signal is fs=200000.
I calculate the concrete bin positions for given start and stop frequencies in the following way:
tIndex.iStartPos = (int64_t) ((tFreqs.i64fstart) / (mSampleRate / uFFTLen));
and e.g. I get for the first signal to be cut out 16 bins.
Now I do the IFFT transformation again with FFTW and get the 16 complex values back (because I reserved the vector for 16 bins).
But when I compare the extracted signal with the original small signal in MATLAB, then I can see that the original signal (is a wav-File) has xxxxx data and my signal (which I saved as raw binary file) has only 16 complex values.
So how do I obtain the length of the IFFT operation to be correctly transformed? What is wrong here?
EDIT
The logic itself is split over 3 programs, each line is in a multithreaded environment. For that reason I post here some pseudo-code:
ReadWavFile(); //returns the signal data and the RIFF/FMT header information
CalculateFFT_using_CUFFTW(); //calculates FFT with user given parameters, like FFT length, polyphase factor, and applies polyphased window to reduce leakage effect
GetFFTData(); //copy/get FFT data from CUDA device
SendDataToSignalDetector(); //detects signals and returns center frequency and bandwith for each sigal
Freq2Index(); // calculates positions with the returned data from the signal detector
CutConcreteBins(position);
AddPaddingZeroToConcreteBins(); // adds zeros till next power of 2
ApplyPolyphaseAndWindow(); //appends the signal itself polyphase-factor times and applies polyphased window
PerformIFFT_using_FFTW();
NormalizeFFTData();
Save2BinaryFile();
-->Then analyse data in MATLAB (is at the moment in work).
If you have a real signal consisting of 1024 samples, the contribution from the 16 frequency bins of interest could be obtained by multiplying the frequency spectrum by a rectangular window then taking the IFFT. This essentially amounts to:
filling a buffer with zeros before and after the frequency bins of interest
copying the frequency bins of interest at the same locations in that buffer
if using a full-spectrum representation (if you are using fftw_plan_dft_1d(..., FFTW_BACKWARD,... for the inverse transform), computing the Hermitian symmetry for the upper half of the spectrum (or simply use a half-spectrum representation and perform the inverse transform through fftw_plan_dft_c2r_1d).
That said, you would get a better frequency decomposition by using specially designed filters instead of just using a rectangular window in the frequency domain.
The output length of the FT is equal to the input length. I don't know how you got to 16 bins; the FT of 1024 inputs is 1024 bins. Now for a real input (not complex) the 1024 bins will be mirrorwise identical around 512/513, so your FFT library may return only the lower 512 bins for a real input. Still, that's more than 16 bins.
You'll probably need to fill all 1024 bins when doing the IFFT, as it generally doesn't assume that its output will become a real signal. But that's just a matter of mirroring the lower 512 bins then.
Related
I have a signal of frequency 10 MHz sampled at 100 MS/sec. How to compute FFT in matlab in terms of frequency when my signal is in rawData (length of this rawData is 100000), also
what should be the optimum length of NFFT.(i.e., on what factor does NFFT depend)
why does my Amplitude (Y axis) change with NFFT
whats difference between NFFT, N and L. How to compute length of a signal
How to separate Noise and signal from a single signal (which is in rawData)
Here is my code,
t=(1:40);
f=10e6;
fs=100e6;
NFFT=1024;
y=abs(rawData(:1000,2));
X=abs(fft(y,NFFT));
f=[-fs/2:fs/NFFT:(fs/2-fs/NFFT)];
subplot(1,1,1);
semilogy(f(513:1024),X(513:1024));
axis([0 10e6 0 10]);
As you can find the corresponding frequencies in another post, I will just answer your other questions:
Including all your data is most of the time the best option. fft just truncates your input data to the requested length, which is probably not what you want. If you known the period of your input single, you can truncate it to include a whole number of periods. If you don't know it, a window (ex. Hanning) may be interesting.
If you change NFFT, you use more data in your fft calculation, which may change the amplitude for a given frequency slightly. You also calculate the amplitude at more frequencies between 0 and Fs/2 (half of the sampling frequency).
Question is not clear, please provide the definition of N and L.
It depends on your application. If the noise is at the same frequency as your signal, you are not able to separate it. Otherwise, you can a filter (ex. bandpass) to extract the frequencies of interest.
In working on a project I came across the need to generate various waves, accurately. I thought that a simple sine wave would be the easiest to begin with, but it appears that I am mistaken. I made a simple program that generates a vector of samples and then plays those samples back so that the user hears the wave, as a test. Here is the relevant code:
vector<short> genSineWaveSample(int nsamples, float freq, float amp) {
vector<short> samples;
for(float i = 0; i <= nsamples; i++) {
samples.push_back(amp * sinx15(freq*i));
}
return samples;
}
I'm not sure what the issue with this is. I understand that there could be some issue with the vector being made of shorts, but that's what my audio framework wants, and I am inexperienced with that kind of library and so do not know what to expect.
The symptoms are as follows:
frequency not correct
ie: given freq=440, A4 is not the note played back
strange distortion
Most frequencies do not generate a clean wave. 220, 440, 880 are all clean, most others are distorted
Most frequencies are shifted upwards considerably
Can anyone give advice as to what I may be doing wrong?
Here's what I've tried so far:
Making my own sine function, for greater accuracy.
I used a 15th degree Taylor Series expansion for sin(x)
Changed the sample rate, anything from 256 to 44100, no change can be heard given the above errors, the waves are simply more distorted.
Thank you. If there is any information that can help you, I'd be obliged to provide it.
I suspect that you are passing incorrect values to your sin15x function. If you are familiar with the basics of signal processing the Nyquist frequency is the minimum frequency at which you can faithful reconstruct (or in your case construct) a sampled signal. The is defined as 2x the highest frequency component present in the signal.
What this means for your program is that you need at last 2 values per cycle of the highest frequency you want to reproduce. At 20Khz you'd need 40,000 samples per second. It looks like you are just packing a vector with values and letting the playback program sort out the timing.
We will assume you use 44.1Khz as your playback sampling frequency. This means that a snipet of code producing one second of a 1kHz wave would look like
DataStructure wave = new DataStructure(44100) // creates some data structure of 44100 in length
for(int i = 0; i < 44100; i++)
{
wave[i] = sin(2*pi * i * (frequency / 44100) + pi / 2) // sin is in radians, frequency in Hz
}
You need to divide by the frequency, not multiply. To see this, take the case of a 22,050 Hz frequency value is passed. For i = 0, you get sin(0) = 1. For i = 1, sin(3pi/2) = -1 and so on are so forth. This gives you a repeating sequence of 1, -1, 1, -1... which is the correct representation of a 22,050Hz wave sampled at 44.1Khz. This works as you go down in frequency but you get more and more samples per cycle. Interestingly though this does not make a difference. A sinewave sampled at 2 samples per cycle is just as accurately recreated as one that is sampled 1000 times per second. This doesn't take into account noise but for most purposes works well enough.
I would suggest looking into the basics of digital signal processing as it a very interesting field and very useful to understand.
Edit: This assumes all of those parameters are evaluated as floating point numbers.
Fundamentally, you're missing a piece of information. You don't specify the amount of time over which you want your samples taken. This could also be thought of as the rate at which the samples will be played by your system. Something roughly in this direction will get you closer, for now, though.
samples.push_back(amp * std::sin(M_PI / freq *i));
How can I draw an spectrum for an given audio file with Bass library?
I mean the chart similar to what Audacity generates:
I know that I can get the FFT data for given time t (when I play the audio) with:
float fft[1024];
BASS_ChannelGetData(chan, fft, BASS_DATA_FFT2048); // get the FFT data
That way I get 1024 values in array for each time t. Am I right that the values in that array are signal amplitudes (dB)? If so, how the frequency (Hz) is associated with those values? By the index?
I am an programmer, but I am not experienced with audio processing at all. So I don't know what to do, with the data I have, to plot the needed spectrum.
I am working with C++ version, but examples in other languages are just fine (I can convert them).
From the documentation, that flag will cause the FFT magnitude to be computed, and from the sounds of it, it is the linear magnitude.
dB = 10 * log10(intensity);
dB = 20 * log10(pressure);
(I'm not sure whether audio file samples are a measurement of intensity or pressure. What's a microphone output linearly related to?)
Also, it indicates the length of the input and the length of the FFT match, but half the FFT (corresponding to negative frequencies) is discarded. Therefore the highest FFT frequency will be one-half the sampling frequency. This occurs at N/2. The docs actually say
For example, with a 2048 sample FFT, there will be 1024 floating-point values returned. If the BASS_DATA_FIXED flag is used, then the FFT values will be in 8.24 fixed-point form rather than floating-point. Each value, or "bin", ranges from 0 to 1 (can actually go higher if the sample data is floating-point and not clipped). The 1st bin contains the DC component, the 2nd contains the amplitude at 1/2048 of the channel's sample rate, followed by the amplitude at 2/2048, 3/2048, etc.
That seems pretty clear.
I am trying to compute a fast fourier transform of a large chunk of data imported from a text file which is around 16 gB in size. I was trying to think of a way to compute its fft in matlab, but due to my computer memory (8gB) it is giving me an out of memory error. I tried using memmap, textscan, but was not able to apply to get FFT of the combined data.
Can anyone kindly guide me as to how should I approach to get the fourier transform? I am also trying to get the fourier transform (using definition) using C++ code on a remote server, but it's taking a long time to execute. Can anyone give me a proper insight as to how should I handle this large data?
It depends on the resolution of the FFT that you require. If you only need an FFT of, say, 1024 points, then you can reshape your data to, or sequentially read it as N x 1024 blocks. Once you have it in this format, you can then add the output of each FFT result to a 1024 point complex accumulator.
If you need the same resolution after the FFT, then you need more memory, or a special fft routine that is not included in Matlab (but I'm not sure if it is even mathematically possible to do a partial FFT by buffering small chunks through for full resolution).
It may be better you implement FFT with your own code.
The FFT algorithm has a "butterfly" operation. Hence you can split the whole step into smaller blocks.
The file size is too large for a typical pc to handle. But FFT doesn't need all data at once. It can always start with 2-point (maybe 8-point is better) FFT, and you can build up by cascading the stages. It means you can read only a few points at a time, do some calculation, and save your data to disk. Next time you doing another iteration, you can read the saved data from disk.
Depending on how you build the data structure, you can either store all the data in one single file, and read/save it with pointers (in Matlab it's merely a number); or you can store every single point in one individual file, generating billions of files and distinguishing them by file names.
The idea is you can dump your calculation to disk, instead of memory. Of course it requires such amount of disk space, which is more feasible.
I can show you a piece of pseudo-code. Depending on the data structure of your original data (that 16GB txt file), the implementation will be different, but you can easily operate as you own the file. I will start with 2-point FFT and do with the 8-point sample in this wikipedia picture.
1.Do 2-point FFT on x, generating y, the 3rd column of white circles from left.
read x[0], x[4] from file 'origin'
y[0] = x[0] + x[4]*W(N,0);
y[1] = x[0] - x[4]*W(N,0);
save y[0], y[1] to file 'temp'
remove x[0], x[4], y[0], y[1] from memory
read x[2], x[6] from file 'origin'
y[2] = x[2] + x[6]*W(N,0);
y[3] = x[2] - x[6]*W(N,0);
save y[2], y[3] to file 'temp'
remove x[2], x[6], y[2], y[3] from memory
....
2.Do 2-point FFT on y, generating z, the 5th column of white circles.
3.Do 2-point FFT on z, generating final result, X.
Basically the Cooley–Tukey FFT algorithm is designed to enable you cut up the data and calculate piece by piece, so it's possible to handle large-amount data. I know it's not a regular way but if you can take a look at the Chinese version of that Wikipedia page, you may find a number of pictures that may help you understand how it splits up the points.
I've encountered this same problem. I ended up finding a solution in a paper:
Extending sizes of effective convolution algorithms. It essentially involves loading shorter chunks, multiplying by a phase factor and FFT-ing, then loading the next chunk in the series. This gives a sampled of the total FFT of the full signal. The process is then repeated with a number of times with different phase factors to fill in the remaining points. I will attempt to summarize here (adapted from Table II in the paper):
For a total signal f(j) of length N, decide on a number m or shorter chunks each of length N/m that you can store in memory (if needed, zero-pad the signal such that N is a multiple of m)
For beta = 0, 1, 2, ... ,m - 1 do the following:
Divide the new series into m subintervals of N/m successive points.
For each subinterval, multiply each jth element by exp(i*2*pi*j*beta/N). Here, j is indexed according to the position of the point relative to the first in the whole data stream.
Sum the first elements of each subinterval to produce a single number, sum the second elements, and so forth. This can be done as points are read from file, so there is no need to have the full set of N points in memory.
Fourier transform the resultant series, which contains N/m points.
This will give F(k) for k = ml + beta, for l = 0, ..., N/m-1. Save these values to disk.
Go to 2, and proceed with the next value of beta.
I am trying to do a 2D Real To Complex FFT using CUFFT.
I realize that I will do this and get W/2+1 complex values back (W being the "width" of my H*W matrix).
The question is - what if I want to build out a full H*W version of this matrix after the transform - how do I go about copying some values from the H*(w/2+1) result matrix back to a full size matrix to get both parts and the DC value in the right place
Thanks
I'm not familiar with CUDA, so take that into consideration when reading my response. I am familiar with FFTs and signal processing in general, though.
It sounds like you start out with an H (rows) x W (cols) matrix, and that you are doing a 2D FFT that essentially does an FFT on each row, and you end up with an H x W/2+1 matrix. A W-wide FFT returns W values, but the CUDA function only returns W/2+1 because real data is even in the frequency domain, so the negative frequency data is redundant.
So, if you want to reproduce the missing W/2-1 points, simply mirror the positive frequency. For instance, if one of the rows is as follows:
Index Data
0 12 + i
1 5 + 2i
2 6
3 2 - 3i
...
The 0 index is your DC power, the 1 index is the lowest positive frequency bin, and so forth. You would thus make your closest-to-DC negative frequency bin 5+2i, the next closest 6, and so on. Where you put those values in the array is up to you. I would do it the way Matlab does it, with the negative frequency data after the positive frequency data.
I hope that makes sense.
There are two ways this can be acheived. You will have to write your own kernel to acheive either of this.
1) You will need to perform conjugate on the (half) data you get to find the other half.
2) Since you want full results anyway, it would be best if you convert the input data from real to complex (by padding with 0 imaginary) and performing the complex to complex transform.
From practice I have noticed that there is not much of a difference in speed either way.
I actually searched the nVidia forums and found a kernel that someone had written that did just what I was asking. That is what I used. if you search the cuda forum for "redundant results fft" or similar you will find it.