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5 Questions around this concept.
Two bodies of masses $\mathrm{m}_1=5 \mathrm{~kg}$ and $\mathrm{m}_2=3 \mathrm{~kg}$ are connected by a light string going over a smooth light pulley on a smooth inclined plane as shown in the figure. The system is at rest. The force exerted by the inclined plane on the body of mass $\mathrm{m}_1$ will be : [Take $\mathrm{g}=10 \mathrm{~ms}^{-2}$ ]
Here m1 is connected to one end of the string and m2 is connected to another end of the string. And mass m2 hung from the string connected by the pulley,
Case 1:-
When a mass m1 placed on a rough horizontal plane
So the tension (T) produced in the string will try to start the motion of mass m1:
For liming condition
$\begin{aligned} & T=F_l \\ & m_2 g=\mu R \\ & m_2 g=\mu m_1 g \\ & m_2=\mu m_{1=\text { minimum value of } m_2 \text { to start the motion }} \\ & \qquad \begin{array}{l}\mu=\frac{m_2}{m_1} \\ \text { So }\end{array} \\ & \text { where } \mathrm{T}=\text { Tension in a string } \\ & F_l=\text { Limiting friction } \\ & \mu=\text { Coefficient of friction }\end{aligned}$
Case 2:-
When a mass m1 placed on a rough inclined plane
So the tension (T) produced in the string will try to start the motion of mass m1:
For limiting condition
For $\mathrm{m}_2 \quad T=m_2 g$
For $\mathrm{m}_1 \quad T=m_1 g \sin \theta+F$
$$
T=m_1 g \sin \theta+\mu m_1 \cos \theta
$$
Use (i) \& (ii)
$m_2=m_1[\sin \theta+\mu \cos \theta]=$ minimum value of $m_2$ to start the motion
where $T=$ tension
$\mathrm{m}_2 \mathrm{~g}=$ weigh of mass $\mathrm{m}_2$
$\mathrm{F}=$ limiting friction
Here $\mu=\left[\frac{m_2}{m_1 \cos \theta}-\tan \theta\right]$
$\mu={ }_{\text {coefficient of friction }}$
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