We will use the impulse-momentum theorem to relate the force applied to the golf ball to the change in its momentum.
Step 1: Define the variables
Step 2: Impulse-Momentum Theorem
The impulse, \(J\), is equal to the change in momentum: \[J = \Delta p = m(v - u)\] Also, the impulse is the integral of force over time: \[J = \int_{0}^{t} F(t) \, dt\]
Step 3: Force as a Function of Time
Since the force decreases linearly with time, we can express it as: \[F(t) = F_0 \left(1 - \frac{t}{T}\right)\] where \(F_0\) is the initial force (at \(t=0\)) and \(T\) is the time of contact, which is \(0.02\) s in this case.
Step 4: Calculate the Impulse
Now, we calculate the impulse by integrating the force function over time: \[J = \int_{0}^{T} F_0 \left(1 - \frac{t}{T}\right) \, dt = F_0 \int_{0}^{T} \left(1 - \frac{t}{T}\right) \, dt\] \[J = F_0 \left[t - \frac{t^2}{2T}\right]_{0}^{T} = F_0 \left(T - \frac{T^2}{2T}\right) = F_0 \left(T - \frac{T}{2}\right) = F_0 \frac{T}{2}\]
Step 5: Apply the Impulse-Momentum Theorem and Solve for \(F_0\)
Now, equating the impulse to the change in momentum: \[F_0 \frac{T}{2} = m(v - u)\] \[F_0 = \frac{2m(v - u)}{T}\]
Plugging in the given values: \[F_0 = \frac{2 \times 0.05 \text{ kg} \times (100 \text{ m/s} - 0 \text{ m/s})}{0.02 \text{ s}} = \frac{2 \times 0.05 \times 100}{0.02} = \frac{10}{0.02} = 500 \text{ N}\]
Therefore, the force at the beginning of the contact is \(500\) N.