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Question: A cylindrical tube, with its base as shown in the figure, is filled with water. It is moving down wi...

A cylindrical tube, with its base as shown in the figure, is filled with water. It is moving down with a constant acceleration a along a fixed inclined plane with angle θ\theta = 45°. P1 and P2 are pressures at points 1 and 2, respectively, located at the base of the tube. Let B= (P1-P2)/(pgd), where p is the density of water, d is the inner diameter of the tube and g is the acceleration due to gravity. Which of the following statement(s) is (are) correct?

A

B = 0 when a = g/√2

B

B > 0 when a = 9//2

C

B = √2-1 when a = 9/2

D

B = 1/√2 when a = g/2

Answer

A and B

Explanation

Solution

The pressure gradient in the fluid is given by P=ρ(gafluid)\nabla P = \rho (\vec{g} - \vec{a}_{fluid}). Assuming the fluid is in equilibrium in the accelerating frame, afluid=atube=ai^\vec{a}_{fluid} = \vec{a}_{tube} = a \hat{i}. The gravitational acceleration is g=gsinθi^gcosθj^\vec{g} = g \sin \theta \hat{i} - g \cos \theta \hat{j}. The acceleration of the tube is a=ai^\vec{a} = a \hat{i}.

The pressure gradient components are: Px=ρ(gsinθa)\frac{\partial P}{\partial x} = \rho (g \sin \theta - a) Py=ρgcosθ\frac{\partial P}{\partial y} = -\rho g \cos \theta

Points 1 and 2 are at the base of the tube, and the line connecting them is along the inclined plane, with point 1 further down the incline than point 2. The distance between them along the incline is dd. Thus, the pressure difference P1P2P_1 - P_2 is given by: P1P2=x2x1Pxdx=x2x1ρ(gsinθa)dxP_1 - P_2 = \int_{x_2}^{x_1} \frac{\partial P}{\partial x} dx = \int_{x_2}^{x_1} \rho (g \sin \theta - a) dx Since the distance along the incline is dd, and point 1 is at x1=x2+dx_1 = x_2 + d: P1P2=ρ(gsinθa)dP_1 - P_2 = \rho (g \sin \theta - a) d

We are given θ=45\theta = 45^\circ, so sinθ=12\sin \theta = \frac{1}{\sqrt{2}}. P1P2=ρ(g2a)dP_1 - P_2 = \rho \left( \frac{g}{\sqrt{2}} - a \right) d

The quantity BB is defined as B=P1P2ρgdB = \frac{P_1 - P_2}{\rho g d}. Substituting the expression for P1P2P_1 - P_2: B=ρ(g2a)dρgd=g2ag=12agB = \frac{\rho \left( \frac{g}{\sqrt{2}} - a \right) d}{\rho g d} = \frac{\frac{g}{\sqrt{2}} - a}{g} = \frac{1}{\sqrt{2}} - \frac{a}{g}

Now we evaluate the given options:

A. B=0B = 0 when a=g/2a = g/\sqrt{2}. If a=g/2a = g/\sqrt{2}, then B=12g/2g=1212=0B = \frac{1}{\sqrt{2}} - \frac{g/\sqrt{2}}{g} = \frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}} = 0. This statement is correct.

B. B>0B > 0 when a=9/2a = 9/\sqrt{2}. Assuming g>9g > 9 (which is true, as g9.8m/s2g \approx 9.8 \, m/s^2), then a=9/2<g/2a = 9/\sqrt{2} < g/\sqrt{2}. In this case, ag<12\frac{a}{g} < \frac{1}{\sqrt{2}}, so B=12ag>0B = \frac{1}{\sqrt{2}} - \frac{a}{g} > 0. This statement is correct.

C. B=21B = \sqrt{2}-1 when a=9/2a = 9/2. If a=9/2a = 9/2, then B=129/2g=1292gB = \frac{1}{\sqrt{2}} - \frac{9/2}{g} = \frac{1}{\sqrt{2}} - \frac{9}{2g}. For B=21B = \sqrt{2}-1, we would need 1292g=21\frac{1}{\sqrt{2}} - \frac{9}{2g} = \sqrt{2}-1. 92g=12(21)=112=122\frac{9}{2g} = \frac{1}{\sqrt{2}} - (\sqrt{2}-1) = 1 - \frac{1}{\sqrt{2}} = 1 - \frac{\sqrt{2}}{2}. g=92(12/2)=922=9(2+2)(22)(2+2)=9(2+2)42=9(2+2)215.36g = \frac{9}{2(1 - \sqrt{2}/2)} = \frac{9}{2-\sqrt{2}} = \frac{9(2+\sqrt{2})}{(2-\sqrt{2})(2+\sqrt{2})} = \frac{9(2+\sqrt{2})}{4-2} = \frac{9(2+\sqrt{2})}{2} \approx 15.36. This value of gg is not standard. Thus, this statement is incorrect for the usual value of gg.

D. B=1/2B = 1/\sqrt{2} when a=g/2a = g/2. If a=g/2a = g/2, then B=12g/2g=1212B = \frac{1}{\sqrt{2}} - \frac{g/2}{g} = \frac{1}{\sqrt{2}} - \frac{1}{2}. This is not equal to 1/21/\sqrt{2}. This statement is incorrect.

Therefore, statements A and B are correct.