JEE Mains · Physics · STD 12 -Electromagnetic induction
- JEE Mains 2026
- Hard
- Numerical
A block takes \(t\) time to slide down a plane inclined at \(45°\) to the horizontal. If the surface is made smooth (frictionless), the block takes time \(\dfrac{t}{2}\) to slide down the plane. The coefficient of friction between the block and the inclined plane is \(\left(\dfrac{\alpha}{100}\right)\). The value of \(\alpha\) is __________.
Pick an option to check your answer.
Answer & Solution
Correct Answer
(B) 75
Step-by-step Solution
Detailed explanation
Let the length of the inclined plane be \(s\).
For the smooth inclined plane, the acceleration of the block is \(a_1 = g \sin \theta\).
The time taken is \(t_1 = \dfrac{t}{2}\). Using the second equation of motion \(s = ut + \dfrac{1}{2}at^2\) with \(u = 0\):
\(s = \dfrac{1}{2} (g \sin \theta) \left(\dfrac{t}{2}\right)^2 = \dfrac{1}{8} g \sin \theta t^2\)
For the rough inclined plane, the acceleration of the block is \(a_2 = g(\sin \theta - \mu \cos \theta)\).
The time taken is \(t_2 = t\). Using the equation of motion again:
\(s = \dfrac{1}{2} g(\sin \theta - \mu \cos \theta) t^2\)
Equating the two expressions for \(s\):
\(\dfrac{1}{8} g \sin \theta t^2 = \dfrac{1}{2} g(\sin \theta - \mu \cos \theta) t^2\)
\(\dfrac{1}{4} \sin \theta = \sin \theta - \mu \cos \theta\)
Given \(\theta = 45^{\circ}\), we have \(\sin 45^{\circ} = \cos 45^{\circ} = \dfrac{1}{\sqrt{2}}\). Substituting these values:
\(\dfrac{1}{4} = 1 - \mu\)
\(\mu = 1 - \dfrac{1}{4} = \dfrac{3}{4} = 0.75\)
We are given \(\mu = \dfrac{\alpha}{100}\).
\(\dfrac{\alpha}{100} = 0.75 \Rightarrow \alpha = 75\)
Answer: \(75\)
For the smooth inclined plane, the acceleration of the block is \(a_1 = g \sin \theta\).
The time taken is \(t_1 = \dfrac{t}{2}\). Using the second equation of motion \(s = ut + \dfrac{1}{2}at^2\) with \(u = 0\):
\(s = \dfrac{1}{2} (g \sin \theta) \left(\dfrac{t}{2}\right)^2 = \dfrac{1}{8} g \sin \theta t^2\)
For the rough inclined plane, the acceleration of the block is \(a_2 = g(\sin \theta - \mu \cos \theta)\).
The time taken is \(t_2 = t\). Using the equation of motion again:
\(s = \dfrac{1}{2} g(\sin \theta - \mu \cos \theta) t^2\)
Equating the two expressions for \(s\):
\(\dfrac{1}{8} g \sin \theta t^2 = \dfrac{1}{2} g(\sin \theta - \mu \cos \theta) t^2\)
\(\dfrac{1}{4} \sin \theta = \sin \theta - \mu \cos \theta\)
Given \(\theta = 45^{\circ}\), we have \(\sin 45^{\circ} = \cos 45^{\circ} = \dfrac{1}{\sqrt{2}}\). Substituting these values:
\(\dfrac{1}{4} = 1 - \mu\)
\(\mu = 1 - \dfrac{1}{4} = \dfrac{3}{4} = 0.75\)
We are given \(\mu = \dfrac{\alpha}{100}\).
\(\dfrac{\alpha}{100} = 0.75 \Rightarrow \alpha = 75\)
Answer: \(75\)
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