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An organ pipe of length 80 cm is opened at x=0 and closed at x=80 cm. Speed of sound in the air column is 320 m/s.If standing waves are generated in the closed organ pipe,then the correct equation of standing waves is are ( here s=longitudinal displacement , P_ex=pressure excess)(Neglect the end correction)
is it correct ? \[\large \bf P_{ex}=A \sin(\frac{25 \pi}{8}x)\cos(1000\pi t)\]
@Michele_Laino and @samigupta8
U asked same doubt @mayankdevnani N yep obviously dat is d ans
yep, but i think it is incorrect
So what r u getting ?
\[\large \bf P_{ex}=Acos(\frac{25 \pi}{8}x)\sin(1000 \pi t)\] this what i get
Option me hi ni h naa shayd
yep :(
@Michele_Laino @IrishBoy123 @Vincent-Lyon.Fr
\( P(x,t)=A \sin(\dfrac{25 \pi}{8}x)\cos(1000\pi t)\) is correct for the harmonic no 5. You need a sine function since the pipe is open at x=0 (acoustic pressure is zero). Using a cosine would produce a maximum amplitude for pressure at x=0, caracteristic of a closed end.
pipe is open at x=0,then P(x,t)=0
@Vincent-Lyon.Fr can we say that both the terms can also be of sine function . In dis way ur argument wud also hold true...Is it necessary that one has to be cos n other a sine function....
If we consider the fundamental frequency, or fundamental wavelength, which is four times the length \(L\) of the pipe, then the excess of pressure \(\Delta p\), is given by the subsequent formula: \[\Large \Delta p = - \rho v_S^2\frac{{\partial s}}{{\partial x}}\] where \(v_S\) is the sound speed in the air, \(\rho\) is the density of air, furthermore, we have: \[\Large s\left( x \right) = A\sin \left\{ {2\pi \left( {\frac{{{v_S}}}{{4L}}t - \frac{x}{{4L}}} \right)} \right\}\]
but standing wave superposition for pressure variation is in the form:- \[\large \bf \triangle P=\triangle P_0(\cos kx)(\sin \omega t)\]
but answer is in the form of :- \[\large \bf \triangle P_0= \triangle P_0(\sin kx)(\cos \omega t)\] How?
Exactly @Michele_laino so v have equation of pressure variation as Po cos(wt-kx)....n when want to find stationary wave den one eq. Is dis n other wud be Po cos(wt+kx) for the wave travelling in opposite direction n we find superposition of the two then we will be having both terms in cos functions....
Whether you have a cos or a sine for the \(\omega t\) part is irrelevant. You can have \(\cos (\omega t+\phi)\) with ANY value of \(\phi\) you want. They are all solutions for your problem.
okay.What about `kx` ? coskx or sinkx ?
I already answered that question : - only sinkx is ok if x=0 is an open end (no acoustic pressure there, maximum velocity) - only coskx is ok if x=0 is an closed end (no velocity there, maximum acoustic pressure)
yes! We have to find the resulting stationary wave by means of the superposition principle first @samigupta8
Thanks....@Michele_Laino u cleared my doubt....
:)
the pressure variation is the effect and the stationary waves are the cause
So they can be in any form sine or cos....v don't have to give a damn to DAT thing...
I think that the form can be sin.. or cos.. since both type of solution type obey to the oscillatory motion. Furthermore we can get a sin.. solution starting from the cos.. form, depending on the initial conditions
Yeah...correct BT der is no other option DAT can stand for match vid harmonic frequencies ....so DAT also rules out d case
yes! More precisely we can say that sin.. or cos.. represent the same \(physical\) behaviour
Yep....
@Michele_Laino and @Vincent-Lyon.Fr is my answer correct also ?
Which one, please?
This one
No, the cosine is wrong since the question states that x=0 is an open end.
if we replace it by displacement, then is it true?
i think it would be,right ?
@Vincent-Lyon.Fr
Yes, it would be true for velocity or for displacement, but the amplitude A would be a velocity or a displacement respectively.
i got it now ! thank you
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