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Suppose you are standing on top of a hemisphere of radius r and you kick a soccer ball horizontally such that it has velocity v. what is the minimum v that ensures the ball will not hit the hemispherical surface. in this case, how far does the ball land from the base of the hemisphere?

1 Answer

4 votes


|v| =√( G \cdot M / r), where


  • M the mass of the planet, and

  • G the universal gravitation constant.

Step-by-step explanation:

Minimizing the initial velocity of the soccer ball would minimize the amount of mechanical energy it has. It shall maintain a minimal gravitational potential possible at all time. It should therefore stay to the ground as close as possible. An elliptical trajectory would thus be unfavorable; the ball shall maintain a uniform circular motion as it orbits the planet.

Equation 1 (see below) relates net force the object experiences,
\Sigma F to its orbit velocity
v and its mass
m required for it to stay in orbit :


\Sigma F = m \cdot v^(2) / r (equation 1)

The soccer ball shall experiences a combination of gravitational pull and air resistance (if any) as it orbits the planet. Assuming negligible air resistance, the net force
\Sigma F acting on the soccer ball shall equal to its weight,
W = m \cdot g where
g the gravitational acceleration constant. Thus


\Sigma F = W = m \cdot g (equation 2)

Substitute equation 2 to the left hand side of equation 1 and solve for
v; note how the mass of the soccer ball,
m, cancels out:


m \cdot g = \Sigma F = m \cdot v^(2) / r \\ v^(2) = g \cdot r \\ |v| = √(g \cdot r) \; (|v| \ge 0) (equation 3)

Equation 4 gives the value of gravitational acceleration,
g, a point of negligible mass experiences at a distance
r from a planet of mass
M (assuming no other stellar object were present)


g = G \cdot M/ r^(2) (equation 4)

where the universal gravitation constant
G = 6.67408 * 10^(-11) \cdot \text{m}^(3) \cdot \text{kg}^(-1) \cdot \text{s}^(-2)

Thus



\begin{array}{lll}|v| &=& √(g \cdot r)\\ & =&√( G \cdot M / r)\end{array}

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