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can be represented by a graph, x versus t.
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At any point on the graph
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you can take the derivative,
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which will be tangent to the curve at each point,
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and its numerical value will be
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what you can call the instantaneous velocity of that point
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and you can take the derivative over the derivative
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and call it the acceleration.
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So, we are going to specialize to a very limited class of problems
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in the rest of this class.
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A limited class of problems is
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one in which the acceleration is just a constant.