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I was reading The History of Physics by Isaac Asimov, and I came across this passage.
"Imagine a body dropped first from a height of 1000 kilometers, then from 2000 kilometers, then from 3000 kilometers, and so on. The drop from 1000 kilometers would result in a velocity of impact v_{1}. If the value g were constant all the way up, then a drop from 2000 kilometers would involve a gain in the first 1000 kilometers equal to the gain in the second 1000 kilometers, so the final velocity of impact would be v_{1}+v_{1} or 2v_{1}."
I was wondering why it came to 2v_{1}. Wouldn't it be \sqrt{2}v_{1}?
Here's my thinking:
From an equation, v^{2}_{f}=v^{2}_{i}+2gs, then we have
v^{2}_{1}=2g(1000) and v^{2}_{2}=2g(2000), and thus
v_{2}=\sqrt{2}v_{1}.
"Imagine a body dropped first from a height of 1000 kilometers, then from 2000 kilometers, then from 3000 kilometers, and so on. The drop from 1000 kilometers would result in a velocity of impact v_{1}. If the value g were constant all the way up, then a drop from 2000 kilometers would involve a gain in the first 1000 kilometers equal to the gain in the second 1000 kilometers, so the final velocity of impact would be v_{1}+v_{1} or 2v_{1}."
I was wondering why it came to 2v_{1}. Wouldn't it be \sqrt{2}v_{1}?
Here's my thinking:
From an equation, v^{2}_{f}=v^{2}_{i}+2gs, then we have
v^{2}_{1}=2g(1000) and v^{2}_{2}=2g(2000), and thus
v_{2}=\sqrt{2}v_{1}.