A stretched string, tube or wireless antenna has a resonance fixed by the velocity of the wave (sound in air, metal, electrical wave etc.) and the length of the object. The fundamental occurs when a standing wave is anchored between points of mechanical or electrical constraint, such as the ends of the wire or tube.

If I were to move one of the fixed supports (an end of the string) such that it moves as if it were a point a few cm from the end of a standing wave of lower frequency, would it still resonate?

I think that it wouldn't, but I don't understand why. Do I need a more complex motion that also stretches the wire at 90 degrees phase shift from the movement?


If I understand you correctly, you want to know what happens when you move one end of a string. Actually this is usually the way you get your standing wave in the first place. Mathematically, you can get the behavior by assuming a time dependent boudary condition at one end, e.g. a $\vec A_0\sin{\omega t}$ time dependence of the amplitude in a certain direction. Then, for transverse $\vec A_0$, you will get resonances (standing waves) for angular frequencies corresponding to integer multiples of a half wavelength + a quarter wavelength fitting into the length of the string. For longitudinal $\vec A_0$, you will get resonances for angular frequencies corresponding to integer multiples of a half wavelength.

If you have a string oscillating in a standing wave you can quench the oscillation by starting a (longitudinal) sinusoid oscillation with the standing wave frequency at an end point in anti-phase.

  • $\begingroup$ I wasn't completely clear when I said 'move one of the fixed supports'. Imagine a guitar string, plucked and oscillating. Consider a point 1cm from the bridge. It's oscillating in phase with the midpoint of the string, but with less amplitude. Now move the bridge 1cm so the tension is the same but the vibrating length is 1cm longer and the fundamental a little lower. If I physically move the same point as before in the same manner as it naturally oscillated, I wouldn't expect to excite a resonance because the fundamental is now a lower frequency. $\endgroup$ – artag Oct 28 '16 at 18:51
  • $\begingroup$ But, how does the longer part of the string 'know' that ? Why doesn't it oscillate at the original frequency, given that it has the same tension and some point on it is moving in the same way as the original measurement ? $\endgroup$ – artag Oct 28 '16 at 18:51
  • $\begingroup$ I shouldn't have said 'move the end'. I should have said 'shorten the string, but constrain the movement at the new end to be the same as it was for that point on the original length' $\endgroup$ – artag Oct 28 '16 at 18:53
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    $\begingroup$ @sammy gerbil : thanks for the links. in this instance I am looking at forced oscillation. But parametric oscillation (probably by changing tension) is another option and I thank you for clarifying the distinction for me. $\endgroup$ – artag Oct 28 '16 at 18:55
  • $\begingroup$ @artag - This is, of course, very different to how I understood your question. $\endgroup$ – freecharly Oct 28 '16 at 19:06

This additional answer assumes that the question is about shortening the length of a vibrating string during vibration.

If you are shortening the length of a string that is already vibrating in its fundamental mode, you are moving the resonant frequency to higher values corresponding to the changed length of the string. This is a well-known phenomenon in violins, where during shortening/lengthening the vibrating string length by continuously moving the pressure point on the finger board, a tone with increasing/decreasing pitch is produced.


Revised Answer (for earlier version click on "edited ... ago")

Reading your question as well as your comments it is still not quite clear what you mean.

I presume that the string of length $L$ with fixed ends A and B is set vibrating, as in the 1st figure below. The tension and mass per unit length determine the speed $v$ of travelling waves. The fundamental frequency is $f=\frac{2v}{L}$ (which comes from speed = wavelength x frequency).

P is a point on the string close to end B. It vibrates with frequency $f$. Note that if we force P to vibrate with frequency $f$ then it does not matter whether or not the section PB of the string exists : we could remove it without destroying the standing wave.

enter image description here

With the string at rest end B is then unfixed and forced to vibrate with the same motion that point P had in the 1st diagram. We now have the situation in the 2nd diagram.

If the moving end B has the same frequency $f$ as P, then a standing wave will not be formed on the string. The forcing frequency corresponds to a string of shorter length $L$, but the effective length $L'$ is now somewhat longer than $L$. (How much longer is difficult to say; see the discussion below.) The forcing frequency $f'$ should be correspondingly lower. The tension in the string and its mass per unit length are the same; the speed $v$ of waves on the string is the same. So :
$v = fL/2 = f'L'/2$.

The amplitude of B is not important. Any amplitude will work, but the frequency is crucial.

How much lower than $f$ does $f'$ need to be? I think this cannot be answered exactly. If $L'$ is only slightly greater than $L$, the section BB' will be very steep. This will require the midpoint of the string to have a very large amplitude. A real string may not have enough elasticity to extend so much. To maintain the same amplitude the increase should be approximately proportional :

If P were the midpoint of AB, then $L'=2L$ and $f'=\frac12 f$.

  • $\begingroup$ I wasn't completely clear when I said 'move one of the fixed supports'. Imagine a guitar string, plucked and oscillating. $\endgroup$ – artag Oct 28 '16 at 18:44
  • $\begingroup$ Sorry - my fault - I did not read your question carefully. $\endgroup$ – sammy gerbil Oct 28 '16 at 22:47

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