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Laws of Motion question

2021 · 1 Sep · Shift 2 · Q69
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  5. /2021 · 1 Sep · Shift 2 · Q69

Laws of Motion question

2021 · 1 Sep · Shift 2 · Q69

JEE MainPhysicsLaws of MotionNumerical+4 / −1
When a body slides down from rest along a smooth inclined plane making an angle of 30 ∘^\circ∘ with the horizontal, it takes time T. When the same body slides down from the rest along a rough inclined plane making the same angle and through the same distance, it takes time α\alphaα T, where α\alphaα is a constant greater than 1. The co-efficient of friction between the body and the rough plane is 1x(α2−1α2){1 \over {\sqrt x }}\left( {{{{\alpha ^2} - 1} \over {{\alpha ^2}}}} \right)x​1​(α2α2−1​) where x = ‾\underline{\hspace{2cm}}​.
Numerical answer
View written solutionFree

Correct answer: 3

  1. Motion on the smooth incline

Let the length of the incline be sss and angle be θ=30∘\theta = 30^\circθ=30∘.

For the smooth plane, acceleration is a1=gsin⁡30∘=g2a_1 = g\sin 30^\circ = \frac{g}{2}a1​=gsin30∘=2g​

Since the body starts from rest, s=12a1T2s = \frac{1}{2} a_1 T^2s=21​a1​T2 s=12⋅g2⋅T2=gT24s = \frac{1}{2}\cdot \frac{g}{2} \cdot T^2 = \frac{gT^2}{4}s=21​⋅2g​⋅T2=4gT2​

  1. Motion on the rough incline

Let the acceleration on the rough plane be a2a_2a2​.

Given that time taken is αT\alpha TαT, and distance is the same sss. So, s=12a2(αT)2s = \frac{1}{2} a_2 (\alpha T)^2s=21​a2​(αT)2 s=12a2α2T2s = \frac{1}{2} a_2 \alpha^2 T^2s=21​a2​α2T2

But from the smooth case, s=gT24s = \frac{gT^2}{4}s=4gT2​

Hence, 12a2α2T2=gT24\frac{1}{2} a_2 \alpha^2 T^2 = \frac{gT^2}{4}21​a2​α2T2=4gT2​

Cancelling T2T^2T2, 12a2α2=g4\frac{1}{2} a_2 \alpha^2 = \frac{g}{4}21​a2​α2=4g​ a2α2=g2a_2 \alpha^2 = \frac{g}{2}a2​α2=2g​ a2=g2α2a_2 = \frac{g}{2\alpha^2}a2​=2α2g​

  1. Acceleration on rough incline using friction

Along the incline, a2=g(sin⁡30∘−μcos⁡30∘)a_2 = g(\sin 30^\circ - \mu \cos 30^\circ)a2​=g(sin30∘−μcos30∘) a2=g(12−μ⋅32)a_2 = g\left(\frac{1}{2} - \mu \cdot \frac{\sqrt{3}}{2}\right)a2​=g(21​−μ⋅23​​)

Equating with the value found above: g(12−μ32)=g2α2g\left(\frac{1}{2} - \frac{\mu \sqrt{3}}{2}\right) = \frac{g}{2\alpha^2}g(21​−2μ3​​)=2α2g​

Cancel ggg and multiply by 2: 1−μ3=1α21 - \mu \sqrt{3} = \frac{1}{\alpha^2}1−μ3​=α21​

So, μ3=1−1α2=α2−1α2\mu \sqrt{3} = 1 - \frac{1}{\alpha^2} = \frac{\alpha^2 - 1}{\alpha^2}μ3​=1−α21​=α2α2−1​

Thus, μ=13(α2−1α2)\mu = \frac{1}{\sqrt{3}}\left(\frac{\alpha^2 - 1}{\alpha^2}\right)μ=3​1​(α2α2−1​)

  1. Compare with the given form

Given, μ=1x(α2−1α2)\mu = \frac{1}{\sqrt{x}}\left(\frac{\alpha^2 - 1}{\alpha^2}\right)μ=x​1​(α2α2−1​)

Comparing, 1x=13\frac{1}{\sqrt{x}} = \frac{1}{\sqrt{3}}x​1​=3​1​

Therefore, x=3x = 3x=3

  1. Comparison with stored answer

Derived answer is 333, which matches the stored correct answer.

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