Two blocks each of mass m lie on a smooth table. They are attached to two other masses as shown in the figure. The pulleys and strings are light. An object O is kept at rest on the table. The sides AB & CD of the two blocks are made reflecting. The acceleration of two images formed (of the object O) in those two reflecting surfaces with respect to each other is :
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Could you please explain in brief why you multiplied your answer by 2.
Thanks!
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If the distance between a plane mirror and an object is given by Δ s ( t ) , then the distance between the object and its reflexion is given by 2 Δ s ( t ) . Using this, we know that the distance between the reflected images will be 2 Δ s R ( t ) + 2 Δ s L ( t ) . As we know that the acceleration is the second derivative of space in respect to time, then a ( t ) = d t 2 d 2 [ 2 Δ s R ( t ) + 2 Δ s L ( t ) ] = 2 d t 2 d 2 Δ s R ( t ) + 2 d t 2 d 2 Δ s L ( t ) = 2 a R ( t ) + 2 a L ( t ) . .
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I still don't understood....😥😥
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@Abhimanyu Gehlot – Which part you didn't understand? Did you understand why the distance is doubled?
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@Plinio Sd – So relieved! My book did not multiply by 2 and gave the final answer as 17g/12. I was so worried. Huh!
Listen the distance of object form mirror is x then its Image distance form mirror is also x so the distance btwn Image and object is 2x
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So if distance is increasing by 2 acceleration should also increase by two
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Using the second Newton's law, F = m a , we can find that the acceleration of the right-side system is given by 2 m g = ( m + 2 m ) a R ⇒ a R = 3 2 g . Analogously, for the left-side system, we find a L = 4 3 g . Note that when an image is reflected, if the distance between the mirror and the object is Δ s , then the distance between the reflected image and the object is 2 Δ s , which implies that the acceleration is multiplied by 2 too. Then, the two reflected images separates themselves with an acceleration of 2 a R + 2 a L = 6 1 7 g .