As the ball goes through one revolution, it moves a distance
that is equal to the circumference of the horizontal circle.
Circumference = 2 * π * r
If you look at the diagram, you will see a right triangle that
contains the radius of the circle, the angle, and the length of the
cord. Let’s use following equation to determine the radius.
r = L * sin β, r = L * sin β
Let’s use this for r in the circumference equation.
Circumference = 2 * π * L * sin β = 2 * π *L* sin β
To determine the velocity of the ball, divide by T seconds
v = 2 * π * L*sin β / T
Let’s determine the vertical and horizontal component of the
tension
Vertical = F * cos β, Horizontal = F * sin β
The vertical component of the tension is equal to the weight of the
ball. The horizontal component of the tension is equal to the
centripetal force.
F * cos β = m * g
F * sin β = m * v^2/r
Divide the second equation by the first equation.
F^2 = (mg)^2 +( mv^2/R)^2
on substituting and solving. we get
F = m*4*pi^2*L/T^2
We have
F * cos β = m * g
cos β = mg/F = mg/ [ m*4*pi^2*L/T^2]
cos β = [g*T^2 / 4 *pi^2*L]
β = cos-1 [g*T^2 / 4 *pi^2*L]
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A ball of mass 1.25 kg is attached by a 1.4 meter long massless rope to the top of a vertical pole. The ball swings in a horizontal circle at a constant rate of ? rad/s...
Please show work, so i can
practice.
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