How do you find the antiderivative of #e^(sinx)*cosx#?
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To find the antiderivative of ( e^{\sin(x)} \cos(x) ), you can use integration by parts. Let ( u = e^{\sin(x)} ) and ( dv = \cos(x)dx ). Then, ( du = e^{\sin(x)} \cos(x) dx ) and ( v = \sin(x) ).
Applying the integration by parts formula:
[ \int e^{\sin(x)} \cos(x) dx = e^{\sin(x)} \sin(x) - \int \sin(x) \cdot e^{\sin(x)} \cos(x) dx ]
This results in:
[ \int e^{\sin(x)} \cos(x) dx = e^{\sin(x)} \sin(x) - \int e^{\sin(x)} \cos(x) dx ]
Now, you can add ( \int e^{\sin(x)} \cos(x) dx ) to both sides and solve for it:
[ 2 \int e^{\sin(x)} \cos(x) dx = e^{\sin(x)} \sin(x) ]
[ \int e^{\sin(x)} \cos(x) dx = \frac{1}{2} e^{\sin(x)} \sin(x) + C ]
Where ( C ) is the constant of integration.
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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