Solving Sound Interference: Find Diff. Freq. Destructive Interference

  • Thread starter Thread starter kahless2005
  • Start date Start date
  • Tags Tags
    Interference Sound
AI Thread Summary
The discussion focuses on solving a problem involving destructive interference between two sound waves emitted from a speaker, with frequencies f(1) and f(2). The user has derived the wave equations for both frequencies and is seeking guidance on demonstrating that destructive interference occurs at a specific distance x. A hint suggests looking for a point where the waves are out of phase by pi radians, indicating the need to add the wave functions to find the cancellation time. The distinction between time-dependent and location-dependent cancellation is emphasized, highlighting the importance of analyzing the waveforms. The conversation aims to clarify the conditions for achieving destructive interference in this context.
kahless2005
Messages
44
Reaction score
0
Given for the problem:
A speaker sends out two sound waves with equal Amplitudes but the frequencies are f(1) and f(2) respectively. The motion of sound as w = A * cos(k*x - t*(Omega)). The wave number's and the angular frequency's definition are the same for light.

Find for the problem:
Show that at a distance x directly in front of the speaker, there is destructive interference between the waves with a frequency f(1) - f(2).

My solution so far:
w(1) = A * cos((2PI/(Lambda(1))) * x - (2PI * f(1) * t)
w(2) = A * cos((2PI/(Lambda(2))) * x - (2PI * f(2) * t)

I assume that the final equation will be in the form of:
dt = (x / v) - t
where v is the speed of sound

A little advice please!
 
Physics news on Phys.org
I hope i put this in the right section... It is a Sophmre level physics class... :blushing:
 
kahless2005 said:
Given for the problem:
A speaker sends out two sound waves with equal Amplitudes but the frequencies are f(1) and f(2) respectively. The motion of sound as w = A * cos(k*x - t*(Omega)). The wave number's and the angular frequency's definition are the same for light.

Find for the problem:
Show that at a distance x directly in front of the speaker, there is destructive interference between the waves with a frequency f(1) - f(2).

My solution so far:
w(1) = A * cos((2PI/(Lambda(1))) * x - (2PI * f(1) * t)
w(2) = A * cos((2PI/(Lambda(2))) * x - (2PI * f(2) * t)

I assume that the final equation will be in the form of:
dt = (x / v) - t
where v is the speed of sound

A little advice please!

Hint: You are looking for a point, x, where the two waves are out of phase by pi radians.

-Dan
 
"Destructive Interference" in this case is time-dependent cancellation of the total amplitude (that means add the wave functions), at any location.
This is in contrast to location-dependent cancellation of the total amplitude
(an interference pattern) at all time.

Choose an x-value, and add the wave forms ; see when (time) they cancel.
 
TL;DR Summary: I came across this question from a Sri Lankan A-level textbook. Question - An ice cube with a length of 10 cm is immersed in water at 0 °C. An observer observes the ice cube from the water, and it seems to be 7.75 cm long. If the refractive index of water is 4/3, find the height of the ice cube immersed in the water. I could not understand how the apparent height of the ice cube in the water depends on the height of the ice cube immersed in the water. Does anyone have an...
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
Back
Top