Integration with Reduction Formula

Matty R
Messages
83
Reaction score
0
Hello :smile:

I was hoping someone could help me with this. I'm going round in circles and don't understand how to solve it.

Homework Statement



The integral I_m is defined as:

I_m = \int^{\frac{\pi}{2}} _{0} (cos^m(x))dx

where m is a positive integer.

By representing cos^m(x) by cos(x)cos^{m-1}(x), show that:

I_m = \left( \frac{m-1}{m} \right) I_{m-2}

,for m \geq 2


Homework Equations



Integration by parts

I = \int^{b}_{a} \left( u \frac{dv}{dx} \right)dx = \left[uv \right] ^{b}_{a} - \int ^{b}_{a} \left( v \frac{du}{dx} \right)dx


The Attempt at a Solution



I've tried using each of the two functions as u and dv/dx, but can't get anywhere.

I would very much appreciate any help with this.

Thanks.
 
Physics news on Phys.org
Can you show what you got when you tried dv/dx=cos(x) and u=cos^(m-1)(x) and explain where you're stuck?
 
Thanks for the reply. :smile:

Part of my problem is that I don't understand how to incorporate the limits for something like sin^{m-1}(x).

I_{m} = \int^{\frac{\pi}{2}}_{0} \left(cos(x)cos^{m-1}(x) \right)dx

Integration by parts

I_{m} = \left[sin(x)cos^{m-1}(x) \right]^{b}_{a}+\int^{b}_{a} \left(sin(x)sin^{m-1}(x) \right) dx

= \left[sin(x)cos^{m-1}(x) \right]^{b}_{a}+J

Integration by parts

J = - \left[cos(x)sin^{m-1}(x) \right]^{b}_{a} + I_{m}

I_{m} = \left[sin(x)cos^{m-1}(x) \right]^{b}_{a} - \left[cos(x)sin^{m-1}(x) \right]^{b}_{a} + I_{m}

Thats what I get to. I'm not even confident of how I've dealt with u and dv/dx, but I haven't been able to find any information about that. I also don't understand how to get to I_{m-2}

I can follow the example from my tutorials easily enough ((ln|x|)^n), but I'm completely lost with this one.

EDIT

I haven't differentiated properly. I didn't use the chain rule. I'll try again.
 
Last edited:
Yeah, when you do use the chain rule, it should work out.
 
Matty R said:
Integration by parts

I_{m} = \left[sin(x)cos^{m-1}(x) \right]^{b}_{a}+\int^{b}_{a} \left(sin(x)sin^{m-1}(x) \right) dx

= \left[sin(x)cos^{m-1}(x) \right]^{b}_{a}+J

Integration by parts

J = - \left[cos(x)sin^{m-1}(x) \right]^{b}_{a} + I_{m}
Why J = - \left[cos(x)sin^{m-1}(x) \right]^{b}_{a} + I_{m}? Where did you found sin^{m - 1}\left(x\right)?
 
LeonhardEuler said:
Yeah, when you do use the chain rule, it should work out.

Yup. I've got it now. I still had a hiccup, with (m - 1) multiplied by a couple of terms, I tried to fully expand it. I think I understand it now.

I found an example applying sin^m(x) in my lecture notes, so I'll use that for applying this integral.

Thanks for your help. :smile:

inline said:
Why J = - \left[cos(x)sin^{m-1}(x) \right]^{b}_{a} + I_{m}? Where did you found sin^{m - 1}\left(x\right)?

I think I got it from integrating cos^{m - 1}(x) incorrectly. :redface:
 
There are two things I don't understand about this problem. First, when finding the nth root of a number, there should in theory be n solutions. However, the formula produces n+1 roots. Here is how. The first root is simply ##\left(r\right)^{\left(\frac{1}{n}\right)}##. Then you multiply this first root by n additional expressions given by the formula, as you go through k=0,1,...n-1. So you end up with n+1 roots, which cannot be correct. Let me illustrate what I mean. For this...
Back
Top