Consider a rope with length l , mass per unit length ? , experiencing a gravitat
ID: 2280098 • Letter: C
Question
Consider a rope with length l, mass per unit length ?, experiencing a gravitational acceleration g and hanging vertically as shown. (Figure 1) Let y refer to the height of a point P above the bottom of the rope.
Explanation / Answer
Let:
dy be the length of an infinitesimal portion of the rope at height y from the lower end of the rope,
T1 be the tension at a point immediately below,
T2 be the tension at a point immediately above,
g be the acceleration due to gravity.
The downward forces on the portion are T1 and its own weight lambda * g * dy
= T1 + lambda * g * dy
The upward force is T2.
Equating the two for equilibrium of the portion:
T2 = T1 + lambda * g * dy.
T2 - T1 = lambda * g * dy ...(1)
T2 - T1 is the increase in tension as you move up the rope a distance dy.
Therefore (1) can be written:
dT = lambda * g * dy.
Integrating:
int ( 0 to y) [ dT ] = lambda * g * int(0 to y) [ dy ]
T_P = lambda * y * g.