Question #48970

1.
The figure above shows part of a system consisting of a block at the top of an inclined plane that rests on a
table, which is located on Earth. The block and plane are at rest when the block is released. In trial 1 there is
no friction between the block and the plane or between the plane and the table. In trial 2 the plane is fixed to
the table so it cannot move, but there is still no friction between the block and the plane.
(a) Indicate whether the speed of the block relative to the table when the block reaches the bottom of the
plane is greater in trial 1 or trial 2. Justify your answer in a clear, coherent, paragraph-length
explanation.
(b) Assuming the body has mass M and the plane has mass 3M and angle 30o, find the ratio of the speeds of
the block at the base of the plane, just before entering the curved area of the plane, in the 2 cases ( trial
1 / trial 2).
1

Expert's answer

2014-11-18T01:33:57-0500

Answer on Question #48970-Physics-Mechanics-Kinematics-Dynamics

The figure above shows part of a system consisting of a block at the top of an inclined plane that rests on a table, which is located on Earth. The block and plane are at rest when the block is released. In trial 1 there is no friction between the block and the plane or between the plane and the table. In trial 2 the plane is fixed to the table so it cannot move, but there is still no friction between the block and the plane.

(a) Indicate whether the speed of the block relative to the table when the block reaches the bottom of the plane is greater in trial 1 or trial 2. Justify your answer in a clear, coherent, paragraph-length explanation.

(b) Assuming the body has mass MM and the plane has mass 3M3M and angle 30o30o , find the ratio of the speeds of the block at the base of the plane, just before entering the curved area of the plane, in the 2 cases (trial 1 / trial 2).

Solution


Assume the body has mass mm and the plane has mass MM , the angle be α\alpha .

(a) In trial 1 the weight of the body has parallel and perpendicular components to a plane;


W=Wcosα,W=Wsinα.W _ {\perp} = W \cos \alpha , W _ {\parallel} = W \sin \alpha .


A plane is moving to the left by the force Wsinα=WsinαcosαW_{\perp}\sin \alpha = W\sin \alpha \cos \alpha

The acceleration of plane is


ap=WsinαcosαM.a _ {p} = \frac {W \sin \alpha \cos \alpha}{M}.


Vertical acceleration of the body is


ay=Wsinαm=Wsin2αm.a _ {y} = \frac {W _ {\parallel} \sin \alpha}{m} = \frac {W \sin^ {2} \alpha}{m}.


But the horizontal acceleration of the body relative to the table is


ax=WsinαcosαmWsinαcosαM.a _ {x} = \frac {W \sin \alpha \cos \alpha}{m} - \frac {W \sin \alpha \cos \alpha}{M}.


The magnitude of acceleration of the body relative to the table is


a1=ax2+ay2=Wmsin4α+sin2αcos2α(1mM)2=Wsinαmsin2α+cos2α(1mM)2.a _ {1} = \sqrt {a _ {x} ^ {2} + a _ {y} ^ {2}} = \frac {W}{m} \sqrt {\sin^ {4} \alpha + \sin^ {2} \alpha \cos^ {2} \alpha \left(1 - \frac {m}{M}\right) ^ {2}} = \frac {W \sin \alpha}{m} \sqrt {\sin^ {2} \alpha + \cos^ {2} \alpha \left(1 - \frac {m}{M}\right) ^ {2}}.


The speed of the block relative to the table when the block reaches the bottom of the plane is


v1=a1t,v _ {1} = a _ {1} t,


where t=2iat = \sqrt{\frac{2i}{a_{\parallel}}}, a=Wsinαma_{\parallel} = \frac{W \sin \alpha}{m}.

In trial 2 the weight of the body has parallel and perpendicular components to a plane;


W=Wcosα,W=Wsinα.W_{\perp} = W \cos \alpha, W_{\parallel} = W \sin \alpha.


The magnitude of acceleration of the body relative to the table is


a=Wsinαm.a_{\parallel} = \frac{W \sin \alpha}{m}.


The speed of the block relative to the table when the block reaches the bottom of the plane is


v2=at,v_{2} = a_{\parallel} t,


where t=2iat = \sqrt{\frac{2i}{a_{\parallel}}}.

The ratio of the speeds of the block at the base of the plane is


v2v1=ata1t=WsinαmWsinαmsin2α+cos2α(1mM)2=1sin2α+cos2α(1mM)2>1.\frac{v_{2}}{v_{1}} = \frac{a_{\parallel} t}{a_{1} t} = \frac{\frac{W_{\parallel} \sin \alpha}{m}}{\frac{W \sin \alpha}{m} \sqrt{\sin^{2} \alpha + \cos^{2} \alpha \left(1 - \frac{m}{M}\right)^{2}}} = \frac{1}{\sqrt{\sin^{2} \alpha + \cos^{2} \alpha \left(1 - \frac{m}{M}\right)^{2}}} > 1.


Because


sin2α+cos2α(1mM)2<sin2α+cos2α=1=1.\sqrt{\sin^{2} \alpha + \cos^{2} \alpha \left(1 - \frac{m}{M}\right)^{2}} < \sqrt{\sin^{2} \alpha + \cos^{2} \alpha} = \sqrt{1} = 1.


So, the speed of the block relative to the table when the block reaches the bottom of the plane is greater in trial 2.

(b)


v1v2=sin2α+cos2α(1mM)2=sin230+cos230(1M3M)2=14+34(23)2=14+13=712.\frac{v_{1}}{v_{2}} = \sqrt{\sin^{2} \alpha + \cos^{2} \alpha \left(1 - \frac{m}{M}\right)^{2}} = \sqrt{\sin^{2} 30 + \cos^{2} 30 \left(1 - \frac{M}{3M}\right)^{2}} = \sqrt{\frac{1}{4} + \frac{3}{4} \left(\frac{2}{3}\right)^{2}} = \sqrt{\frac{1}{4} + \frac{1}{3}} = \sqrt{\frac{7}{12}}.


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