How do you integrate #int e^xcos(2x)# by parts?
We integrate the resulting integral by parts again:
So if we name:
we get the following equation:
so that:
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To integrate ( \int e^x \cos(2x) ) by parts, we use the integration by parts formula, which states:
[ \int u , dv = uv - \int v , du ]
Let ( u = e^x ) and ( dv = \cos(2x) , dx ). Then, ( du = e^x , dx ) and ( v = \frac{1}{2} \sin(2x) ).
Now, we apply the integration by parts formula:
[ \int e^x \cos(2x) , dx = e^x \cdot \frac{1}{2} \sin(2x) - \int \frac{1}{2} \sin(2x) \cdot e^x , dx ]
The integral on the right-hand side is similar to the original integral but with ( e^x ) as ( u ) and ( \sin(2x) , dx ) as ( dv ).
So, we repeat the integration by parts:
[ u = e^x, \quad dv = \sin(2x) , dx ] [ du = e^x , dx, \quad v = -\frac{1}{2} \cos(2x) ]
Now, we plug these into the formula:
[ \int e^x \cos(2x) , dx = e^x \cdot \frac{1}{2} \sin(2x) - \left( -\frac{1}{2} e^x \cos(2x) - \int -\frac{1}{2} \cos(2x) \cdot e^x , dx \right) ]
Simplify:
[ \int e^x \cos(2x) , dx = \frac{1}{2} e^x \sin(2x) + \frac{1}{2} \int e^x \cos(2x) , dx ]
Now, we can isolate the integral term:
[ \frac{1}{2} \int e^x \cos(2x) , dx = \frac{1}{2} e^x \sin(2x) ]
Multiply both sides by ( 2 ):
[ \int e^x \cos(2x) , dx = e^x \sin(2x) + C ]
Where ( C ) is the constant of integration. This is the final result of integrating ( \int e^x \cos(2x) ) by parts.
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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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