erik-the-red
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The frequency of the note {\rm F}_4 is f_F.
1. If an organ pipe is open at one end and closed at the other, what length must it have for its fundamental mode to produce this note at a temperature of T? The speed of sound is v_s.
I used the equation f_n = \frac{nv}{4L}. Plugging in known values resulted in L = \frac{1}{4}\frac{v_s}{f_F}. This is correct.
2. At what air temperature will the frequency be f? (Ignore the change in length of the pipe due to the temperature change.)
I have no idea how to start this.
The frequency of the note {\rm F}_4 is f_F.
1. If an organ pipe is open at one end and closed at the other, what length must it have for its fundamental mode to produce this note at a temperature of T? The speed of sound is v_s.
I used the equation f_n = \frac{nv}{4L}. Plugging in known values resulted in L = \frac{1}{4}\frac{v_s}{f_F}. This is correct.
2. At what air temperature will the frequency be f? (Ignore the change in length of the pipe due to the temperature change.)
I have no idea how to start this.