Viotar/Quantifying the signal: Difference between revisions

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A measurement will be done for the low E-string and the high e-string, on the open string and the 1st, 12th and 13th fret. The 1st and 2nd is needed to "shift" the signal in the frequency domain. Everything that shifts up according to the fret change is part of the vibration we want to measure, the rest is noise. The 12th and 13th fret are done so that the same can be done for a much higher position (one octave up), because there will probably be a somewhat different spectrum apart from the higher note.


A measurement will be done for the low E-string and the high e-string, on the open string and the 1st, 12th and 13th fret. The 1st and 2nd is needed to "shift" the signal in the frequency domain. Everything that shifts up according to the fret change is part of the vibration we want to measure, the rest is noise. The 12th and 13th fret are done so that the same can be done for a much higher position (one octave up), because there will probably be a somewhat different spectrum apart from the higher note.
==Analysing the results==
 
Probaby, Helmholtz is the only harmonic vibration that you can get from a string when you bow it. With a bow you can never get a normal standing wave as when you would pluck the string. Because of this, it is not necessary to quantify "how much" the measured vibration is the specific Helmholtz waveform. It may suffit to merely quantify how harmonic the measured vibration is. This can be done by detecting the fundamental frequency in the fft of the signal, and looking looking how many multiplications of this frequency are still in the signal. The more overtones, the sharper the Helmholtz, and therefore the better the tone.

Revision as of 13:29, 1 November 2010

The signal that we want from the string, somehow will have to be read out by the instrument. No matter how this is done, some sensor will provide a signal, in which the vibration we want from the string should be recognised. This recognising has to be done on a reliable, quantitative basis. More specifically, there has to be some kind of scalar quantity that gives us how far we really are from the ideal trajectory in the bow speed-force space, so a feedback loop can be made to let the system find this trajectory for itself. For this, an experiment will be done, and it's results will be analysed thoroughly.

Experiment plan

- Is the computer model of the bowed string accurate?

- Where does the "pleasant" sound come from that you hear when you stand next to the instrument when it's bowed? Is it mainly the vibration of the body that you hear? In that case it would origin mainly from the pressure variances of the string on the bridge, which translate into the body. On the other hand, it could be mainly the vibration of the string that you hear. In that case, the transversal wave as described by the computer model and measured by a laser sensor is dominant. The outcome of this will be important in the choice of what the capture and amplify exactly, when the instrument is done.

- What does the vibration we want (Helmholtz) look like in the transversal wave of one point of the string?

- What does the vibration we want (Helmholtz) look like in the pressure variances of the string on the piëzo element?


A measurement will be done for the low E-string and the high e-string, on the open string and the 1st, 12th and 13th fret. The 1st and 2nd is needed to "shift" the signal in the frequency domain. Everything that shifts up according to the fret change is part of the vibration we want to measure, the rest is noise. The 12th and 13th fret are done so that the same can be done for a much higher position (one octave up), because there will probably be a somewhat different spectrum apart from the higher note.

Analysing the results

Probaby, Helmholtz is the only harmonic vibration that you can get from a string when you bow it. With a bow you can never get a normal standing wave as when you would pluck the string. Because of this, it is not necessary to quantify "how much" the measured vibration is the specific Helmholtz waveform. It may suffit to merely quantify how harmonic the measured vibration is. This can be done by detecting the fundamental frequency in the fft of the signal, and looking looking how many multiplications of this frequency are still in the signal. The more overtones, the sharper the Helmholtz, and therefore the better the tone.