u'Impulse
J produced from time
x to
y is defined as the integral from
x to
y dt of the resultant force
F over the period [
x,
y].
From Newton\'s second law, force is related to momentum
p by
F =
dp/dtTherefore, impulse is defined as the integral from
x to
y of
dp/dt times
dt. As the time differentials cancel, this is just the integral from
x to
y of
dp. This gives us \u0394
p, the change in linear momentum from time
x to
y. This is often called the impulse-momentum theorem.
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