Since the body is initially at equilibrium under the action of the four forces, the net force on the body is zero.
This gives us the equation for equilibrium: \[ F_1 + F_2 + F_3 + F_4 = 0 \] When \( F_1 \) is removed, the remaining forces acting on the body are \( F_2, F_3, \) and \( F_4 \).
The net force on the body is now: \[ F_{{net}} = F_2 + F_3 + F_4 \] From the equilibrium condition, we know that \( F_1 = -(F_2 + F_3 + F_4) \).
Therefore, when \( F_1 \) is removed, the remaining net force is: \[ F_{{net}} = F_1 \] Thus, the acceleration \( a \) of the body is given by Newton's second law: \[ a = \frac{F_{{net}}}{M} = \frac{F_1}{M} \]
Therefore, the body moves with an acceleration of \( \frac{F_1}{M} \) after \( F_1 \) is removed.
Thus, the correct answer is: \[ \boxed{\frac{F_1}{M}} \]
A block of mass 1 kg is pushed up a surface inclined to horizontal at an angle of \( 60^\circ \) by a force of 10 N parallel to the inclined surface. When the block is pushed up by 10 m along the inclined surface, the work done against frictional force is:
[Given: \( g = 10 \) m/s\( ^2 \), \( \mu_s = 0.1 \)]
A gas can be taken from A to B via two different processes ACB and ADB. When path ACB is used, \( 60 J \) of heat flows into the system and \( 30 J \) of work is done by the system. If path ADB is used, the work done by the system is \( 10 J \). The heat flow into the system in path ADB is: