So here is were I'm at now
L = 12 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]\frac{1}{1+cos(θ)}[/itex][itex]\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex]dθ
from here I used the fact that
1 + cos(θ) = 2[itex]cos^{2}[/itex]([itex]\frac{θ}{2}[/itex])
so
[itex]\frac{sec^{2}(\frac{θ}{2})}{2}[/itex] = [itex]\frac{1}{1+cos(θ)}[/itex]
similarly
[itex]\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex] = [itex]\sqrt{1+\frac{sec^{4}(\frac{θ}{2})sin^{2}(θ)}{4}}[/itex]
So I know have the following
L = 12 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]\frac{1}{1+cos(θ)}[/itex][itex]\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex]dθ = 12 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]\frac{sec^{2}(\frac{θ}{2})}{2}[/itex] [itex]\sqrt{1+\frac{sec^{4}(\frac{θ}{2})sin^{2}(θ)}{4}}[/itex]dθ
from here I use the fact that
[itex]sin^{2}[/itex](θ)=4[itex]sin^{2}[/itex]([itex]\frac{θ}{2}[/itex])[itex]cos^{2}[/itex]([itex]\frac{θ}{2}[/itex])
wolfram alpha confirm it's true
http://www.wolframalpha.com/input/?i=sin(x)^2=4sin(x/2)^2*cos(x/2)^2
plugging this in I get
12 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]\frac{sec^{2}(\frac{θ}{2})}{2}[/itex] [itex]\sqrt{1+sec^{4}(\frac{θ}{2})sin^{2}(\frac{θ}{2})cos^{2}(\frac{θ}{2})}[/itex]dθ=6 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]sec^{2}(\frac{θ}{2})[/itex][itex]\sqrt{1+sec^{2}(\frac{θ}{2})sin^{2}(\frac{θ}{2})}[/itex]dθ, u = [itex]\frac{θ}{2}[/itex], [itex]\frac{du}{dθ}[/itex]=[itex]\frac{1}{2}[/itex],du=[itex]\frac{dθ}{2}[/itex],dθ=2du,L=12 [itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{2}(u)[/itex][itex]\sqrt{1+sec^{2}(u)sin^{2}(u)}[/itex]du=12 [itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{2}(u)[/itex][itex]\sqrt{1+tan^{2}(u)}[/itex]du
then from here I use
[itex]sin^{2}(θ)[/itex])+[itex]cos^{2}(θ)[/itex]=1
that if I divide through by [itex]cos^{2}(θ)[/itex] I get
[itex]tan^{2}(θ)[/itex])+1=[itex]sec^{2}(θ)[/itex]
L=12 [itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{2}(u)[/itex][itex]\sqrt{sec^{2}(u)}[/itex]du=12[itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{3}(u)[/itex]du
then because
∫[itex]sec^{n}(x)dx = \frac{sec^{n-2}(x)tan(x)}{n-1}+\frac{n-2}{n-1}∫sec^{n-2}(x)dx[/itex]
we got
12[itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{3}(u)du=12[\frac{sec(u)tan(u)}{2}+\frac{1}{2}∫sec(u)du]|^{θ=\frac{∏}{2}}_{θ=0}[/itex]
and because
∫sec(x)dx=ln|sec(x)+tan(x)|+c
we got
[itex]12[\frac{sec(u)tan(u)}{2}+\frac{1}{2}∫sec(u)du]|^{θ=\frac{∏}{2}}_{θ=0}=12[\frac{sec(u)tan(u)}{2}+\frac{1}{2}ln(|sec(u)+tan(u)|)]|^{θ=\frac{∏}{2}}_{θ=0}[/itex]
plugging back in
u = [itex]\frac{θ}{2}[/itex]
we got
[itex]12[\frac{sec(u)tan(u)}{2}+\frac{1}{2}ln(|sec(u)+tan(u)|)]|^{θ=\frac{∏}{2}}_{θ=0}=12[\frac{sec(\frac{θ}{2})tan(\frac{θ}{2})+ln|sec(θ/2)+tan(\frac{θ}{2})|}{2}]|^{θ=\frac{∏}{2}}_{θ=0}=12[\frac{sec(\frac{∏}{4})tan(\frac{∏}{4})+ln(|sec(∏/4)+tan(\frac{∏}{4})|)}{2}-\frac{sec(0)tan(0)+ln(|sec(0)+tan(0)|}{2})=12[\frac{\sqrt{2}+ln(|\sqrt{2}+1|)}{2}-0][/itex]=6([itex]\sqrt{2}[/itex]+ln([itex]\sqrt{2}+1)[/itex])