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Consider a 2 body system as shown:2-Block System

Consider the floor to be absolutely smooth and the coefficient of friction for the contact between $m_1$ and $m_2$ to be $\mu$. Now suppose I apply a force $F$ that causes the system to move, and that force $F$ is applied on the upper block ($m_1$). Then, why does it ($m_1$) move faster than $m_2$? Why does it have a greater acceleration?

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  • $\begingroup$ isn't there a need of relation between the two masses ? Since the acceleration of both the masses will depend on the friction between them . $\endgroup$
    – Ankit
    Commented Sep 9, 2020 at 8:06

1 Answer 1

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Considering $m_1$ and $m_2$ as a system, there is a net horizontal force $F$ acting on them so their centre of mass must accelerate with acceleration

$\displaystyle a_0 = \frac F {m_1+m_2}$

This is true regardless of whether or not $m_1$ moves relative to $m_2$.

The frictional force which opposes $m_1$ moving relative to $m_2$ has a maximum value of $\mu m_1 g$. If $F - \mu m_1 g \le m_1a_0$ then $m_1$ will not move relative to $m_2$ and both blocks will accelerate with acceleration $a_0$. Substituting the expression for $a_0$ above, we see that this condition becomes

$\displaystyle F - \mu m_1 g \le F \frac {m_1} {m_1+m_2} \\ \displaystyle \Rightarrow F \frac {m_2} {m_1+m_2} \le \mu m_1 g \\ \displaystyle \Rightarrow F \le \mu g (m_1+m_2) \frac {m_1}{m_2}$

In this case, the frictional force is

$\displaystyle F \frac {m_2} {m_1+m_2}$

and we can see that (by Newton's Third Law) this acts on $m_2$ to accelerate it with acceleration $a_0$ too. In effect, the force $F$ is divided between $m_1$ and $m_2$ in proportion to their masses, so that they both have the same acceleration.

On the other hand, if

$\displaystyle F > \mu g (m_1+m_2) \frac {m_1}{m_2}$

then the net force on $m_1$ is $F - \mu m_1 g$ so $m_1$ accelerate with acceleration

$\displaystyle a_1 = \frac F {m_1} - \mu g$

and the force on $m_2$ is $\mu m_1 g$ so $m_2$ accelerates with acceleratiion

$\displaystyle a_2 = \mu g \frac {m_1}{m_2}$

and we have

$\displaystyle a_1 > \mu g \frac {m_1+m_2}{m_2} - \mu g \\ \displaystyle \Rightarrow a_1 > \mu g \frac {m_1}{m_2} \\ \displaystyle \Rightarrow a_1 > a_2$

Also note that the acceleration of the centre of mass of the system is the weighted sum of $a_1$ and $a_2$ which is

$\displaystyle \frac {m_1a_1+m_2a_2} {m_1+m_2} = \frac {(F - \mu m_1 g) + \mu m_1 g} {m_1+m_2} = \frac {F} {m_1+m_2} = a_0$

as we expect.

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