2015: Problems 19-20

Topic: Oscillatory Motion
Concepts: Newton’s laws, Simple harmonic motion


Solution:

Suppose we displace the water so that the right side moves up by distance xx and the left side moves down by distance xx. Then the extra weight on the right side is

F=ρVextrag=ρA(2x)gF=\rho V_{\text{extra}}g=\rho A(2x)g

where AA is the cross-sectional area of the U-tube. This force accelerates all the water so by Newton’s 2nd law,

ma=F=2ρAxgma=-F=-2\rho Axg

where the minus sign accounts for the fact that the force is restoring. Since m=ρV=ρALm=\rho V=\rho AL, we have

ρALa=2ρAxg\rho ALa=-2\rho Axg
a=x¨=2gLxa=\ddot{x}=-\frac{2g}{L}x

This is of simple harmonic form (z¨=ω2z\ddot{z}=-\omega^2z) so we can identify the angular frequency as

ω=2gL\omega=\sqrt{\frac{2g}{L}}

Thus, the frequency is given by

f=ω2π=12π2gLf=\frac{\omega}{2\pi}=\frac{1}{2\pi}\sqrt{\frac{2g}{L}}

so the answer is A.

Topic: Fluids
Concepts: Pressure with depth


Solution:

We compute the pressure at the bottom of the U-tube in two ways: through the left side and through the right side. From the left side,

Pbot=P0+ρoilgL+ρwatergdP_{\text{bot}}=P_0+\rho_{\text{oil}}gL+\rho_{\text{water}}gd

From the right side,

Pbot=P0+ρwaterg(Ld)P_{\text{bot}}=P_0+\rho_{\text{water}}g(L-d)

Since these are equal, we have

ρoilgL+ρwatergd=ρwaterg(Ld)\rho_{\text{oil}}gL+\rho_{\text{water}}gd=\rho_{\text{water}}g(L-d)
ρoilL=ρwater(L2d)\rho_{\text{oil}}L=\rho_{\text{water}}(L-2d)

We are given ρoil=ρwater/2\rho_{\text{oil}}=\rho_{\text{water}}/2 so

L2=L2d\frac{L}{2}=L-2d
2d=L22d=\frac{L}{2}
d=L4d=\frac{L}{4}

Finally, the height difference hh between both sides is

h=(L+d)(Ld)=2d=2(L4)=L2h=(L+d)-(L-d)=2d=2\left(\frac{L}{4}\right)=\frac{L}{2}

so the answer is B.

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