How do you integrate #int y/(e^(2y))# by integration by parts method?

Answer 1

#I = c -(ye^(-2y))/2 - e^(-2y)/4#

We have

#I = int y/e^(2y)dy#
With some simple rewriting, based on the properties of exponentials #1/a^(x) = a^(-x)#
#I = int ye^(-2y)dy#

If we say

#u = y# so #du = dy# #dv = e^(-2y)dy# so #v = -e^(-2y)/2#

By the integration by parts formula

#int udv = uv - int vdu#
#I = -(ye^(-2y))/2 - int-e^(-2y)/2dy#

Putting the constants outside of the integral

#I = -(ye^(-2y))/2 +1/2int e^(-2y)dy# #I = c -(ye^(-2y))/2 - e^(-2y)/4#
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Answer 2

To integrate ( \int \frac{y}{e^{2y}} ) using integration by parts, let ( u = y ) and ( dv = \frac{1}{e^{2y}} dy ). Then, differentiate ( u ) to get ( du = dy ) and integrate ( dv ) to get ( v = -\frac{1}{2e^{2y}} ).

Now, apply the integration by parts formula:

[ \int u , dv = uv - \int v , du ]

Substitute the values of ( u ), ( dv ), ( v ), and ( du ) into the formula:

[ \int \frac{y}{e^{2y}} , dy = -\frac{y}{2e^{2y}} - \int -\frac{1}{2e^{2y}} , dy ]

[ = -\frac{y}{2e^{2y}} + \frac{1}{4} \int e^{-2y} , dy ]

Now, integrate ( \int e^{-2y} ) to get:

[ = -\frac{y}{2e^{2y}} + \frac{1}{4} \left( -\frac{1}{2} e^{-2y} \right) + C ]

Where ( C ) is the constant of integration.

Therefore, the integral ( \int \frac{y}{e^{2y}} , dy ) is:

[ = -\frac{y}{2e^{2y}} - \frac{1}{8e^{2y}} + C ]

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Answer from HIX Tutor

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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