Answer:
The tension in the cable B is approximately 8375.227 N
Step-by-step explanation:
The given parameters are;
The orientation of one cable, B = Horizontal
The orientation of the other cable, A = 40° to the vertical
The horizontal speed with which the chair swings= 32 revolutions per minute
ω = 32×2×π/60 rad /s
The weight of the seat = 255 N
The weight of the person = 825 N
The acceleration due to gravity, g = 9.8 m/s²
Therefore, we have;
The centripetal force
, which gives;

The weight of the person and the seat W = 825 + 255 = 1080 N = The vertical force component in the system
The vertical component of the cable A = The vertical force component in the system = 1080 N
Let
represent the tension in A
The vertical component of the tension =
× cos 40° = 1080
= 1080/(cos(40°)) ≈ 1409.84 N
The horizontal component of
=
From ∑Fₓ = 0, given that the centripetal force is acting outwards and the tension in cable B and the horizontal component of
are acting inwards, we have;
The centripetal force,
= The tension in the cable B + The horizontal component of
9281.457 = The tension in the cable B + 906.23
The tension in the cable B = 9281.457 - 906.23 ≈ 8375.227 N.