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and the y will be the y derivative.
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That's not obvious,
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but in other words it's clear it's sufficient
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but it's also necessary.
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So, every conservative force
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is the derivative of some potential, in this fashion.
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Finally, I said if someone comes and gives you a force
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and says, "Is it conservative or not?"
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Either you can think in your head
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and try to guess that function U,
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of which this F is the derivative,
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in this fashion.