All Solutions
Page 506: Lesson Check
$f_1=dfrac{v}{2L}$
When the pipe is cut into half, the fundamental frequency is expected to double. Therefore, the fundamental frequency of each half would be greater than $200Hz$
$f_n=dfrac{nv}{4L}$
But for pipes that are open at both ends, the equation is
$f_n=dfrac{2v}{2L}$
Using this principle
$f_A=dfrac{1(343m/s)}{4(1m)}=86Hz$
$f_B=dfrac{(1)(343/s)}{2(1m)}=172;Hz$
$f_C=dfrac{2(343m/s)}{2(3m)}=114;Hz$
$f_D=dfrac{3(343m/s)}{4(3m)}=86;Hz$
Therefore, the correct arrangement is $A=D<C<B$
A=D<C<B
$$
$f_n=dfrac{nv}{4L}$
$$
f_1=dfrac{v}{4(H-h)}=dfrac{343;m/s}{4(0.260m-0.070m)}=451;Hz
$$
451;Hz
$$
$$
lambda_3=dfrac{4L}{n}=dfrac{4(2.7m)}{3}=3.6m
$$
3.6m
$$
$difference=625-375=250;Hz$
Since this fundamental frequency is twice the given fundamental frequency, we can say that
$f_1=dfrac{250;Hz}{2}=125;Hz$
Therefore, the fundamental frequency for the bottle is not 375 Hz because from the result of our calculation, it is 125 Hz. The answer is NO.
The next standing wave (second harmonic) that occurs after 625 Hz will occur at $2f_1=250Hz$ higher than 625 Hz.
Thus, the next standing wave will have a frequency
$650+250=875Hz$
875Hz
$$