Fundamental Frequency of Helium-Filled Pipe

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The discussion revolves around calculating the fundamental frequency of a pipe filled with helium compared to when it is filled with air. To find the new frequency, the participants derive relationships using the speed of sound equations and the properties of the gases involved, specifically their molar masses and heat capacities. The key formula derived is f_He = f * sqrt((γ_He * M_air) / (γ_air * M_He)), which relates the frequencies based on the gas properties. Clarifications were made regarding the notation used, specifically the meaning of 'e' as the density of the gas. The conversation highlights the importance of understanding gas dynamics in acoustic applications.
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A certain pipe produces a fundamental frequency f in air.

If the pipe is filled with helium at the same temperature, what fundamental frequency does it produce? (Take the molar mass of air to be M_air, and the molar mass of helium to be M_He). The ratio γ of heat capacities for air (7/5) and for Helium (5/3).

I'm not sure how to approach this question.

Any help would be great.

Thanks.
 
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First, you have to find the Length of the pipe. Remember,
c=f \lambda

and c= \sqrt\frac{\gamma P}{e}

also, PV=nRT
=> PV=(m/M)RT
=> P/e=(RT)/M

In both the cases, the length of the pipe is same. Find the relation between the wavelength and the length of the pipe. You should now be able to calculate the fundamental frequency in the second case
 
Probably a stupid question, but what is e? We never learned this equation.
 
In siddharth's notation, e denotes the density of the gas. That is, e = \frac{m}{V}.
 
Okay, here is my approach. Let me know if you think it makes sense.

We have c = f\lambda and c = \sqrt{(\gamma RT)/M}. In the fundamendal mode, \lambda = 2L. So

2f_\mathrm{He}L = \sqrt{(\gamma_\mathrm{He}RT)/M_\mathrm{He}} (1)

and

2fL = \sqrt{(\gamma_\mathrm{air}RT)/M_\mathrm{air}} (2)

Dividing (1) by (2),

f_\mathrm{He}/f = \sqrt{(\gamma_\mathrm{He}M_\mathrm{air})/(\gamma_\mathrm{air}M_\mathrm{He})}

so

f_\mathrm{He} = f\sqrt{(\gamma_\mathrm{He}M_\mathrm{air})/(\gamma_\mathrm{air}M_\mathrm{He})}
 
Yep, that does make sense when you go through it like that. I've just never approached c = sqrt(γP/e). Thanks for your help.
 

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