Let:
M be the mass of the large sphere,
m be the mass of the plumb bob,
G be the gravitational constant,
g be the acceleration due to gravity,
r be the density of the material of the large sphere,
T be the tension in the string,
a be the inclination to vertical of the plumb line,
s be the required distance
L be the length of the plumb line.
Then:
M = (4pi/3) R^3 r
= (4pi/3)(3 * 10^3)^3 (2.6 * 10^3)
= 2.94 * 10^14 kg.
Resolving horizontally and vertically for the plumb line:
T cos(a) = mg ...(1)
T sin(a) = GMm / (3R)^2 ...(2)
s = L sin(a)
As a is very small, approximation is justified, and it is reasonable to replace sin(a) by tan(a):
s = L tan(a) ...(3)
Dividing (2) by (1):
tan(a) = GM / 9R^2 g
From (3):
s = LGM / 9R^2g
= (0.5)(6.67 * 10^(-11))(2.94 * 10^14) / 9(3 * 10^3)^2 (9.81)
= 1.23 * 10^-5 m
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