A container filled with liquid moves down a rough fixed inclined plane with constant acceleration as shown in figure above.
The angle of incline is cos − 1 5 3 and the liquid surface makes an angle of cos − 1 5 4 with the horizontal.
If the coefficient of friction can be written as b a where a , b are coprime positive integers, find a + b .
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The exact solution of the problem is tan 1 6 ∘ ≈ 0 . 2 8 7 , which cannot be written as the fraction of integers. You want us to assume that tan 5 3 = 4 / 3 , but that is not obvious.
I have a much shorter solution for you, but because I could not solve the problem, I cannot post it as a regular solution.
Anyway, here it is: First, I work with the local inertial frame of reference of the container, so that the force of gravity can be ignored. I choose the x-axis parallel to the incline. The angle between the liquid surface and the horizontal is now 53 - 37 = 16 degrees. This angle is due to the contact force on the container (normal force and friction).
The normal force is m g cos 5 3 ∘ in the y-direction, and the friction force is μ m g cos 5 3 ∘ in the x-direction. The resultant force is perpendicular to the liquid surface, and therefore makes a 16 degree angle with the vertical. This gives tan 1 6 ∘ = F y F x = μ . The friction coefficient is therefore μ = tan 1 6 ∘ ≈ 0 . 2 8 7 .
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I did it the same way but yes, I approximated the value of t a n 5 3 to be 3 4 and value of t a n 3 7 to be 4 3 then use t a n ( A − B ) to calculate t a n 1 6 . (all angles are in degrees)
However, It should be mentioned in the question to take t a n 5 3 = 3 4 and t a n 3 7 = 4 3 and the incline is fixed.
Don't tell me u dint assume it to be 3/5 nd 4/5 ... lol
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No I didn't... Because it is only an approximation.
Why force of gravity can be ignored?
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I chose a coordinate system in free fall. Relative to that coordinate system, there is no gravitational force, and the container is accelerated upward by the normal force from the incline.
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@Arjen Vreugdenhil – oh.. fine.. nice one bro!
Thanks. I have edited the problem for clarity.
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Thanks. 8 months ago I was not aware of the Reporting feature, but now I am :) In fact, nowadays I'd even do the edit myself
Consider Any Small Point Mass On The Surface Of Liquid . Since A Liquid Cannot Sustain Shear Stress
Therefore The Mass Must Be In Equilibrium Along The Surface Of Liquid. We Work From The Frame Of
Beaker . Resolving Pseudo Force And Weight Of Mass Along the surface of liquid and equating them We Get
4-3x = 3/cos16
For Finding value of cos16 we use trigonometric identity cos(53-37)
On Solving We Get x = 7/24
Although It Should Have Been Mentioned But We Here Use
cos53 = 3/5
cos37 = 4/5
Because Mostly Indian Students Will Know This Approximation .
@Prakhar Bindal - I didn't get why did u took cos16.can u explain plz
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