Rotational work and energy involve the motion of objects that are rotating or spinning. In this scenario, the tennis ball is initially at rest and then rolls down the hill, gaining rotational kinetic energy as it moves. When it becomes airborne, it has both translational and rotational kinetic energy.
To determine the range x, we can use the principle of conservation of energy. This states that the total energy of a system remains constant, as long as no external forces act on it. In this case, we can assume that there are no external forces acting on the ball, so the total energy is conserved.
The initial energy of the ball is purely potential energy due to its position at the top of the hill. As it rolls down, this potential energy is converted into both translational and rotational kinetic energy. At the point where it becomes airborne, all of its potential energy has been converted into kinetic energy.
To find the range x, we can use the equations for translational and rotational kinetic energy. The translational kinetic energy is given by 1/2mv^2, where m is the mass of the ball and v is its velocity. The rotational kinetic energy is given by 1/2Iω^2, where I is the moment of inertia and ω is the angular velocity.
We can calculate the translational velocity by using the conservation of energy equation:
mgh = 1/2mv^2 + 1/2Iω^2
Where m is the mass of the ball, g is the acceleration due to gravity, and h is the height of the hill. We can rearrange this equation to solve for v:
v = √(2gh - Iω^2/m)
To find the range x, we need to know the time the ball spends in the air. We can use the equation x = vt, where t is the time. To find t, we can use the equation for projectile motion:
y = y0 + v0yt - 1/2gt^2
Where y is the height of the ball at a given time, y0 is the initial height, v0y is the initial vertical velocity, and g is the acceleration due to gravity. We can rearrange this equation to solve for t:
t = √(2(y-y0)/g)
Substituting this value of t into the equation for range, we get:
x = √(2gh - I