Q152 / 170 · Manipal (MET) 2015 · Physics
A block of mass $m$ is lying on the edge having inclination angle $\alpha=\tan ^{-1}\left(\frac{1}{5}\right)$. Wedge is moving with a constant acceleration, $a=2 \mathrm{~ms}^{-2}$. The minimum value of coefficient of friction $\mu$, so that $m$ remains stationary with respect to wedge is


- A$\frac{2}{a}$
- Correct answerB$\frac{5}{12}$
- C$\frac{1}{5}$
- D$\frac{2}{5}$
Solution
FBD of $m$ in frame of wedge

$N=m g \cos (\alpha)-m a \sin (\alpha)$ Now, $f=\mu N=m a \cos \alpha+m g \sin \alpha$ $\begin{aligned} & \Rightarrow \quad \mu=\frac{a \cos \alpha+g \sin \alpha}{g \cos \alpha-a \sin \alpha} \\ & \Rightarrow \quad \mu=\frac{a+g \tan \alpha}{g-a \tan \alpha}=\frac{5}{12} \Rightarrow \mu=\frac{5}{12}\end{aligned}$

$N=m g \cos (\alpha)-m a \sin (\alpha)$ Now, $f=\mu N=m a \cos \alpha+m g \sin \alpha$ $\begin{aligned} & \Rightarrow \quad \mu=\frac{a \cos \alpha+g \sin \alpha}{g \cos \alpha-a \sin \alpha} \\ & \Rightarrow \quad \mu=\frac{a+g \tan \alpha}{g-a \tan \alpha}=\frac{5}{12} \Rightarrow \mu=\frac{5}{12}\end{aligned}$
Hence, the correct answer is option: 'B'.