Evaluate the integral? : # int_1^e x^5 (lnx)^2 dx #
# int_1^e \ x^5 \ (lnx)^2 \ dx = (13e^6 -1)/108 #
We want to find:
We can use integration by Parts
Then plugging into the IBP formula:
gives us
So now let us look at this next integral:
Again we can use integration by Parts
and plugging into the IBP formula gives us
Combining these results we get:
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To evaluate the integral ∫(1 to e) x^5(lnx)^2 dx, you can use integration by parts.
Let u = (lnx)^2 and dv = x^5 dx. Then, differentiate u to get du and integrate dv to get v.
u = (lnx)^2 dv = x^5 dx
Differentiating u: du = 2(lnx)(1/x) dx du = (2/x)lnx dx
Integrating dv: v = (1/6)x^6
Now, apply the integration by parts formula:
∫ u dv = uv - ∫ v du
∫(1 to e) x^5(lnx)^2 dx = [(1/6)x^6(lnx)^2] from 1 to e - ∫(1 to e) (1/6)x^6 (2/x)lnx dx
Evaluate the integral from 1 to e:
= [(1/6)e^6(ln(e))^2 - (1/6)(1)^6(ln(1))^2] - ∫(1 to e) (1/6)x^5(2lnx) dx
= [(1/6)e^6(1)^2 - (1/6)(0)^2] - ∫(1 to e) (1/3)x^5(lnx) dx
= (1/6)e^6 - 0 - (1/3)∫(1 to e) x^5(lnx) dx
Now, you can integrate ∫ x^5(lnx) dx using integration by parts again or by recognizing it as a tabulated integral. The final result will be:
= (1/6)e^6 - (1/3)[(1/6)e^6 - (1/3)∫(1 to e) x^4 dx]
= (1/6)e^6 - (1/3)[(1/6)e^6 - (1/3)(1/5)e^5 - (1/3)(1/5)]
= (1/6)e^6 - (1/3)[(1/6)e^6 - (1/15)e^5 - (1/15)]
= (1/6)e^6 - (1/18)e^6 + (1/45)e^5 + (1/45)
= (4/9)e^6 + (1/45)e^5 + (1/45)
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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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