A raindrop of mass \( m_{1}=66.4 \mathrm{mg} \) (that is milli-gram) falls in quiet air (no wind). Due to the air resistance force, the drop has a maximum velocity called the terminal velocity of magnitude, \( v_{t}=16.5 \mathrm{~m} / \mathrm{s} \), which is reached high above ground. a) What would be the weight of the rain drop after it reaches terminal velocity and before it reaches ground? \( \dot{F}_{g}=0.000651 \mathrm{~N} \times \hat{j} \) b) What would be the weight of the rain drop before it reaches terminal velocity. \( \dot{F}_{g}=0.000651 \quad \times \hat{j} \) c) What would be the acceleration of the rain drop after it reaches terminal velocity and before it reaches ground? \( \dot{a}=0 \mathrm{~m} / \mathrm{s}^{\wedge} 2 \) d) What would be the air resistance force acting on the rain drop after it reaches terminal velocity and before it reaches ground?. \( \dot{F}_{R}=0.000651 \mathrm{~N} \)
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The Deep Dive
When a raindrop falls, it experiences two main forces: gravity pulling it down and air resistance pushing it up. Once the drop reaches terminal velocity, these forces balance each other out – this means the weight of the raindrop is effectively equal to the air resistance force at that moment. So, after reaching terminal velocity, the raindrop’s weight of \(0.000651 \, \text{N}\) exactly counters the air resistance. Before reaching terminal velocity, the raindrop is accelerating downward since the force of gravity is greater than the air resistance. As the speed increases, so does the air resistance until it eventually matches the gravitational force, resulting in no further acceleration. You can imagine it like a roller coaster building speed on the way down until it glides evenly!
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