How to calculate reflection with GNUradio? - signal-processing

I am preforming an experiment that involves a transmitter, material target, and two receivers (as a baseline). The goal is to record the RF reflectivity of the target. How can I calculate/measure this from the received signal, and can it be done in GNUradio-companion?
Any help is appreciated.
Thank You.

You can do that, in many ways. In the end, chances are you'll send some predefined signal, e.g., precomputed white pseudorandom noise from a "vector source", record that (e.g. using a "file sink" or a "vector sink") and build a correlation estimator that processes that data offline.
Of course, a correlation is just convolution with the (conjugate) time-inverse, so you can also (conjugate if complex and) time-reverse your reference signal, and use it as filter taps.
Note that in general, SDR devices are nice and linear, but not calibrated – you can only compare received signal powers, but you cannot attribute an absolute power to them – unless you know the strength of some reference reception.

Related

How to remove sidelobes while computing frequency from fft?

I am currently operating in vhf band AND trying to detect frequencies using Fast Fourier transform thresholding method.
While detection of multiple frequencies , i received spurs(May not appropriate word) in addition with original frequencies, Such as
in case of f1,f2 that are incoming frequencies i also receive their sum f1+f2 and difference f1-f2.
i am trying to eliminate these using thresholding method but i can't differentiate them with real frequency magnitudes.
Please suggest me some method, or methodology to eliminate this problem
Input frequencies F1, F2
Expected frequencies F1,F2
Receive frequencies ,F1,F2,F1-F2,F1+F2
https://imgur.com/3rYYNv2 plot link that elaborate problem
Windowing can reduce windowing artifacts and distant side lobes, but makes the main lobe wider in exchange. But a large reduction in both the main-lobe and near side-lobes normally requires using more data and a longer FFT.

How to exclude poses of a wheel based robot which place behind of the porevious pose

I am currently working on coding sensor fusion of a wheel based robot pose from GPS, Lidar, Vision and Vehicle measure. Its model is basic kinematics using EKF and no discrimination against sensors i.e. data comes in based on time stamp.
I have difficulty to fuse those sensors due to following issue;
Sometimes when the latest incoming data comes in from different sensor from a sensor gave previous state, the latest pose of the robot comes in behind previous pose. Therefore data fusion does not get so smooth and zigzag-ed as a result.
I would like discard data which plots behind/backwards of the previous data and take data which poses always forward/ahead of previous state even when sensor to provide the data changes between timestamp t and timestamp t+1. Since the data frame is global frame, it is impossible to rely on its x coordinate in minus to achieve this.
Please let me know if you had some idea on this. Thank you so much in advance.
Best,
Preliminary warning
Let me slip here a warning before suggesting posible solutions to your problem: be careful with discarding data based on your current estimate, since you never know if last measure is "pulling pose back" or previous one was wrong and caused your estimate to move forward too much.
Posible solutions
In a Kalman-like filter, observations are assumed to provide independent, uncorrelated information about state vector variables. These observations are assumed to have a random error distributed as a zero mean gaussian variable. Real life is harder, though :-(
Sometimes, measures are affected by a "bias" (a fixed term, similar to the gaussian error having a non-zero mean). e.g. tropospheric perturbations are known to introduce a position error in GPS fixes that drifts slowly over time.
If you take several sensors observing the same variable, as GPS and Lidar for for position, but they have different biases, your estimation will be jumping back and forth. Scaling problems can have a similar effect.
I will assume this is the root of your problem. If not, please refine your question.
How can you mitigate this problem? I see several alternatives:
Introduce a bias/scale correction term in your state vector to compensate sensor bias/drift. This is a very common trick in EKFs for inertial sensor fusion (gyro/accelerometer), that can work nice when tuned properly.
Apply some preprocessing to sensory inputs to correct known problems. It can be difficult to tune a filter for estimating state vector and sensor parameters at the same time.
Change how observations are interpreted. For example, use difference between consecutive position observations so that you are creating a fake odometer sensor. This greatly reduces the drift problem.
Post-process your output. Instead of discarding observations, integrate them and keep the "jumping" state vector internally, but smooth the output vector to eliminate the jumps. This is done in some UAV autopilots because such jumps affect the performance of PID controllers.
Finally, the most obvious and simple approach: discard observations based on some statistical test. A chi-square test of the residual can be used to determine if an observation is too far from expected values and must be discarded. Be careful with this options, though: observation rejection schemes must be completed with a state vector reinitialization logic to resutl in a stable behavior.
Almost all these solutions require knowning the source of each observation, so you would no longer be able to treat them indistinctly.

How can I find process noise and measurement noise in a Kalman filter if I have a set of RSSI readings?

im have RSSI readings but no idea how to find measurement and process noise. What is the way to find those values?
Not at all. RSSI stands for "Received Signal Strength Indicator" and says absolutely nothing about the signal-to-noise ratio related to your Kalman filter. RSSI is not a "well-defined" things; it can mean a million things:
Defining the "strength" of a signal is a tricky thing. Imagine you're sitting in a car with an FM radio. What does the RSSI bars on that radio's display mean? Maybe:
The amount of Energy passing through the antenna port (including noise, because at this point no one knows what noise and signal are)?
The amount of Energy passing through the selected bandpass for the whole ultra shortwave band (78-108 MHz, depending on region) (incl. noise)?
Energy coming out of the preamplifier (incl. Noise and noise generated by the amplifier)?
Energy passing through the IF filter, which selects your individual station (is that already the signal strength as you want to define it?)?
RMS of the voltage observed by the ADC (the ADC probably samples much higher than your channel bandwidth) (is that the signal strength as you want to define it?)?
RMS of the digital values after a digital channel selection filter (i.t.t.s.s.a.y.w.t.d.i?)?
RMS of the digital values after FM demodulation (i.t.t.s.s.a.y.w.t.d.i?)?
RMS of the digital values after FM demodulation and audio frequency filtering for a mono mix (i.t.t.s.s.a.y.w.t.d.i?)?
RMS of digital values in a stereo audio signal (i.t.t.s.s.a.y.w.t.d.i?) ?
...
as you can imagine, for systems like FM radios, this is still relatively easy. For things like mobile phones, multichannel GPS receivers, WiFi cards, digital beamforming radars etc., RSSI really can mean everything or nothing at all.
You will have to mathematically define away to describe what your noise is. And then you will need to find the formula that describes your exact implementation of what "RSSI" is, and then you can deduct whether knowing RSSI says anything about process noise.
A Kalman Filter is a mathematical construct for computing the expected state of a system that is changing over time, given an initial state and noisy measurements of that system. The key to the "process noise" component of this is the fact that the system is changing. The way that the system changes is the process.
Your state might change due to manual control or due to the nature of the system. For example, if you have a car on a hill, it can roll down the hill naturally (described by the state transition matrix), or you might drive it down the hill manually (described by the control input matrix). Any noise that might affect these inputs - wind, bumps, twitches - can be described with the process noise.
You can measure the process noise the way you would measure variance in any system - take the expected dynamics and compare them with the true dynamics to generate a covariance matrix.

Wavelet packet decomposition vs bandpass filters

If I am right, Wavelet packet decomposition (WPT) breaks a signal into various filter banks.
The same thing can be done using many band pass filters.
My aim is to find the energy content of a signal with a large sapmling rate ((2000 hz) in various frequency bands like 1-200, 200-400, 400-600.
What are the advantages and disadvantages of using a WPT of band pass filters?
with wpt (or dwt indeed) you have quadrature mirror filters that will ensure that if you add up all the reconstructed signals in the last level (the leaves) of the wpt tree you get exactly the original signal except for the math processor finite word length aproximations. The algorithm is pretty fast.
Moreover if your signal is non-stationary you can gain the time-frequency localization although this will drastically decrease as you go down on the tree (inverted).
The other aspect is that if yoy are lucky to get a wavelet that correlates well with the non stationary components of your signal the transform will map this components more efficiently.
For you application firstly see how many levels you have to go down in the wpt tree to go from your sampling frequency to the desired freq intervals, you may not get excately 200-400, 400-600 etc,the downer you go in the tree the more accurate are the feq limits, and you may have to join nodes to get your bands.

Phase difference between two signals?

I'm working on this embedded project where I have to resonate the transducer by calculating the phase difference between its Voltage and Current waveform and making it zero by changing its frequency. Where I(current) & V(Voltage) are the same frequency signals at any instant but not the fixed frequency signals approx.(47Khz - 52kHz). All I have to do is to calculate phase difference between these two signals. Which method will be most effective.
FFT of Two signals and then phase difference between the specific components
Or cross-correlation of two signals?
Or another if any ? Which method will give me most accurate result ? and with what resolution? Does sampling rate affects phase difference's resolution (minimum phase difference which can be sensed) ?
I'm new to Digital signal processing, in case of any mistake, correct me.
ADDITIONAL DETAILS:-
Noise In my system can be white/Gaussian Noise(Not significant) & Harmonics of Fundamental (Which might be significant one in resonant mismatch case).
Yes 4046 can be a good alternative with switching regulators. I'm working with (NCO/DDS) where I can scale/ reshape sinusoidal on ongoing basis.
Implementation of Analog filter will be very complex as I will require higher order filter with high roll-off rate for harmonic removal , so I'm choosing DSP based filter and its easy to work with MATLAB DSP Processors.
What sampling rate would you suggest for a ~50 KHz (47Khz-52KHz) system for achieving result in FFT or Goertzel with phase resolution of preferably =<0.1 degrees or less and frequency steps will vary from as small as ~1 to 2Hz . to 50 Hz-200Hz.
My frequency is variable 45KHz - 55Khz ... But will be known to my system... Knowing phase error for the last fed frequency is more desirable. After FFT AND DIGITAL FILTERING , IFFT can be performed for more noise free samples which can be used for further processing. So i guess FFT do both the tasks ...
But I'm wondering about the Phase difference accuracy cause thats the crucial part.
The Goertzel algorithm http://www.embedded.com/design/configurable-systems/4024443/The-Goertzel-Algorithm is a fairly efficient tone detection method that resolves the signal into real and imaginary components. I'll assume you can do the numeric to get the phase difference or just polarity, as you require.
Resolution versus time constant is a design tradeoff which this article highlights issues. http://www.mstarlabs.com/dsp/goertzel/goertzel.html
Additional
"What accuracy can be obtained?"
It depends...upon what you are faced with (i.e., signal levels, external noise, etc.), what hardware you have (i.e., adc, processor, etc.), and how you implement your solution (sample rate, numerical precision, etc.). Without the complete picture, I'll be guessing what you could achieve as the Goertzel approach is far from easy.
But I imagine for a high school project with good signal levels and low noise, an easier method of using the phase comparator (2 as it locks at zero degrees) of a 4046 PLL www.nxp.com/documents/data_sheet/HEF4046B.pdf will likely get you down to a few degrees.
One other issue if you have a high Q transducer is generating a high-resolution frequency. There is a method but that's another avenue.
Yet more
"Harmonics of Fundamental (Which might be significant)"... hmm hence the digital filtering;
but if the sampling rate is too low then there might be a problem with aliasing. Also, mismatched anti-aliasing filters are likely to take your whole error budget. A rule of thumb of ten times sampling frequency seems a bit low, and it being higher it will make the filter design easier.
Spatial windowing addresses off-frequency issues along with higher roll-off and attenuation and is described in this article. Sliding Spectrum Analysis by Eric Jacobsen and Richard Lyons in Streamlining Digital Signal Processing http://www.amazon.com/Streamlining-Digital-Signal-Processing-Guidebook/dp/1118278380
In my previous project after detecting either carrier, I then was interested in the timing of the frequency changes in immense noise. With carrier phase generation inconstancies, the phase error was never quiescent to be quantified, so I can't guess better than you what you might get with your project conditions.
Not to detract from chip's answer (I upvoted it!) but some other options are:
Cross correlation. Off the top of my head, I am not sure what the performance difference between that and the Goertzel algorithm will be, but both should be doable on an embedded system.
Ad-hoc methods. For example, I would try something like this: bandpass the signals to eliminate noise, find the peaks and measure the time difference between the peaks. This will probably be more efficient, and, provided you do a reasonable job throwing out outliers and handling wrap-around, should be extremely robust. The bandpass filters will, themselves, alter the phase, so you'll have to make sure you apply exactly the same filter to both signals.
If the input signal-to-noise ratios are not too bad, a computually efficient solution can be built based on zero crossing detection. Also, have a look at http://www.metrology.pg.gda.pl/full/2005/M&MS_2005_427.pdf for a nice comparison of phase difference detection algorithms, including zero-crossing ones.
Computing 1-bin of a DFT (or using the similar complex Goertzel block filter) will work if the signal frequency is accurately known. (Set the DFT bin or the Goertzel to exactly that frequency).
If the frequency isn't exactly known, you could try using an FFT with an FFTshift to interpolate the frequency magnitude peak, and then interpolate the phase at that frequency for each of the two signals. An FFT will also allow you to window the data, which may improve phase estimation accuracy if the frequency isn't exactly bin centered (or exactly the Goertzel filter frequency). Different windows may improve the phase estimation accuracy for frequencies "between bins". A Blackman-Nutall window will be better than a rectangular window, but there may be better window choices.
The phase measurement accuracy will depend on the S/N ratio, the length of time one samples the two (assumed stationary) signals, and possibly the window used.
If you have a Phase Locked Loop (PLL) that tracks each input, then you can subtract the phase coefficients (of the generator components) to determine offset between the phases. This would also be robust against noise.

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