Step 1: Understanding the Question:
The problem tracks a gas molecule colliding periodically against a flat container boundary. We are given the molecule's mass ($m$), its speed ($v$), and the collision rate ($f = 5\text{ collisions/second}$). We need to find the total momentum transferred to the wall per second.
Step 2: Key Formula or Approach:
For a perfectly elastic collision against a rigid wall, the molecule rebounds with the exact same speed but in the opposite direction.
The change in momentum of a single molecule ($\Delta p_{\text{molecule}}$) along the normal axis is:
$$\Delta p_{\text{molecule}} = p_{\text{final}} - p_{\text{initial}} = (-mv) - (mv) = -2mv$$
By Newton's Third Law (Action-Reaction), the momentum transferred to the wall per collision is equal in magnitude and opposite in sign:
$$\Delta p_{\text{wall}} = +2mv$$
The total change in momentum per second is the momentum from one collision multiplied by the number of collisions per second.
Step 3: Detailed Explanation:
Calculate the momentum change for the wall during a single collision event:
$$\Delta p_{\text{single}} = 2mv$$
Since the molecule undergoes exactly 5 independent collisions every second, multiply the single-collision transfer by 5:
$$\Delta p_{\text{total}} = 5 \times \Delta p_{\text{single}}$$
$$\Delta p_{\text{total}} = 5 \times (2mv) = 10\ mv$$
This matches the value in option (A).
Step 4: Final Answer:
The total momentum transferred to the wall per second is $10\ mv$, which corresponds to option (A).