Daniel B. answered 01/24/21
A retired computer professional to teach math, physics
Let
m = 0.5 kg be the mass of the ball,
L = 1.5 m be the length of the string,
θ = 30° is the angle the string makes with the vertical,
g = 9.81 m/s² be gravitational acceleration,
r (unknown) be the radius of the circle,
v (unknown) be the velocity of the ball.
(a)
There are three forces acting on the ball:
G: downward force of gravity,
T: upward force of tension along the string,
F: horizontal centripetal force toward the center of rotation.
It is important in the free-body diagram that
F = G + T,
which is vector addition of the forces.
It says that G and T are responsible for the centripetal force needed for the circular motion.
(b)
F = mv²/r (1)
(c)
Use equation (1).
To calculate r:
r = Lsin(θ)
To calculate F:
From the free-body diagram in (a) showing F = G + T,
F = Gtan(θ) = mgtan(θ)
Substituting into (1):
mgtan(θ) = mv²/(Lsin(θ)) (2)
v = √(gLtan(θ)sin(θ)) (3)
Substituting actual numbers
v = √(9.81 × 1.5 × tan(30°) × sin(30°)) = 2.061 m/s
(d)
New given: v = 4 m/s
New unknown: θ
Rearranging equation (2)
tan(θ)sin(θ) = v²/gL
Let's denote
U = v²/gL = 4²/(9.81×1.5) = 1.08732585
Then we need to solve
tan(θ)sin(θ) = U
Rewriting in terms of cos(θ) and then solving a quadratic equation over cos(θ):
(sin(θ)/cos(θ)) sin(θ) = U
sin²(θ) = Ucos(θ)
1 - cos²(θ) = Ucos(θ)
cos²(θ) + Ucos(θ) - 1 = 0
cos(θ) = (-U ± √(U² + 4))/2
Approximating U = 1
cos(θ) = (-1 ± √(1² + 4))/2 = (-1 ± √5)/2
Only cos(θ) = (-1 + √5)/2 gives a solution within the range [-1,+1] of cos(θ).
cos(θ) = 0.618
θ = 51.8°
(e)
New given: T = 9.8 N
New unknown: v
From the free-body diagram
cos(θ) = G/T
Substituting actual numbers to get θ:
cos(θ) = mg/T = 0.5 × 9.8 / 9.81 = 0.5
θ = 60°
To calculate v use equation (3)
v = √(gLtan(θ)sin(θ))
= √(9.81 × 1.5 × tan(60°) × sin(60°)) = 4.7 m/s