Find Fundamental Frequency & Tension of Oscillating Wire in Tube

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The discussion revolves around calculating the fundamental frequency and tension of a wire oscillating in a tube closed at one end. The tube's length is 1.03 m, and the wire is 0.37 m long with a mass of 8.2 g. The fundamental frequency is determined using the formula f = v/λ, where λ is calculated as 4L/(2n+1) for n = 0, indicating a quarter wavelength fits in the tube. The challenge arises in finding the correct value for n, as participants note that a negative n value is obtained, which is incorrect. The key points emphasize understanding the relationship between the tube's closed end and the wire's oscillation to derive the correct frequency and tension.
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Homework Statement


A tube 1.03 m long is closed at one end. A stretched wire is placed near the open end. The wire is 0.37 m long and has a mass of 8.2 g. It is fixed at both ends and oscillates in its fundamental mode. By resonance, it sets the air column in the tube into oscillation at that column's fundamental frequency. Find (a) that frequency and (b) the tension in the wire. (Take the speed of sound in air to be 343 m/s.)


Homework Equations


well in this particular question i think you have to use the formula f=\frac{v}{\lambda}
in which case lamda is equal to 4L/2n+1 and then you find the derivative of that set it equal to zero and find your n
plug that back in and i think you mite get frequency but i keep getting a negative n value


The Attempt at a Solution


i guess u read above
 
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The wavelength of the fundamental resonance tone of the tube forms with n = 0. That is a quarter of a wavelength of the oscillation will fit into the tube. The stationary point is at the closed end and the maximum displacement of the air molecules is at the open end.
 
so the frequency would be zero?
 
No, you said that

"... in which case lamda is equal to 4L/2n+1 ..."

that is the requirement for uneven amount of quarter wavelengths to fit into the tube. Why uneven quarters? A node forms at the closed end and an antinode at the open end.
 

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