Source: Principles of Physics
Problem
A cord is used to vertically lower an initially stationary block of mass M at a constant downward acceleration of g/4. When the block has fallen a distance d, find
- the work done by the cord's force on the block,
- the work done by the gravitational force on the block,
- the kinetic energy of the block, and
- the speed of the block.
[Q1] $W_T = -(3/4)Mgd$ [Q2] $W_g = Mgd$ [Q3] $K_f = (1/4)Mgd$ [Q4] $v = \sqrt{gd/2}$
Let T be the tension in the cord and the downward direction be positive. Apply Newton's second law to the block:
$$F_{net} = Mg - T = Ma$$Given the acceleration $a = g/4$:
$$Mg - T = M(g/4)$$ $$T = Mg - Mg/4 = \frac{3}{4}Mg$$[Q1] The cord's force (tension) is directed upward, opposite to the downward displacement $d$. The work done by the cord, $W_T$, is:
$$W_T = -Td = -\frac{3}{4}Mgd$$[Q2] The gravitational force $Mg$ is in the same direction as the displacement $d$. The work done by gravity, $W_g$, is:
$$W_g = Mgd$$[Q3] The net work done on the block equals the change in its kinetic energy (Work-Energy Theorem), $W_{net} = \Delta K$. The block starts from rest, so its initial kinetic energy $K_i=0$.
$$K_f = W_{net} = W_g + W_T$$ $$K_f = Mgd - \frac{3}{4}Mgd = \frac{1}{4}Mgd$$[Q4] The kinetic energy is also given by $K_f = \frac{1}{2}Mv^2$. We can solve for the speed $v$:
$$\frac{1}{2}Mv^2 = \frac{1}{4}Mgd$$ $$v^2 = \frac{gd}{2}$$ $$v = \sqrt{\frac{gd}{2}}$$