- #1
WendysRules
- 37
- 3
Homework Statement
Given ## ds^2 = a^2cot^2 \alpha d\alpha^2 + a^2sin^2 \alpha d\phi^2## where a is some constant. Find:
a) The gaussian curvature
b) the surface area of the upper half of the tractrix
Homework Equations
Stoke theorem: ## \int_S dF = \int_{\partial S} F ##
and for curvature, we know the ## \Omega^1_2 = K\omega ## where K is the gaussian curvature, and omega is the basis.
The Attempt at a Solution
I'll start with the curvature: So to get ## \Omega^1_2 ## I need to first find ##\omega^1_2##
So, given my line element, I see that my basis is ##\{ a\cot \alpha d alpha, a \sin \alpha d\phi \}##
So, my torsion conditions are: 1) ## 0 = d\sigma^1+\omega^1_1 \wedge \sigma^1+\omega^1_2 \wedge \sigma^2 ##
2) ## 0 = d\sigma^2+ \omega^2_1 \wedge sigma^1 + \omega^2_2 \wedge sigma^2 ##
Plugging in our basis and simplifying, we see that: 1) ## 0 = 0 + 0 + \omega^1_2 \wedge a\sin\alpha d\phi## which forces ##\omega^1_2 = b d\phi## for some b.
Thus, 2 becomes : ## 0 = a\cos\alpha d\alpha \wedge d\phi + \omega^2_1 \wedge a\cot\alpha d\alpha + 0## which becomes ## 0 = a\cos\alpha d\alpha \wedge d\phi + ab\cot\alpha d\alpha \wedge d\phi ## which forces ##b= -sin\alpha##. Thus, ## \omega^1_2 = -sin\alpha d\phi ## this makes ##\Omega^1_2 = d\omega^1_2 = d(-sin\alpha d\phi) = -cos \alpha d\alpha \wedge d\phi## since ##\omega = \sigma^1 \wedge \sigma^2 ## we see that ## \Omega^2_1 = \frac{-cos\alpha}{a^2cot\alpha sin\alpha} d\alpha \wedge d\phi## which would make ## K = \frac{-1}{a^2}## giving us a constant negative curvature.
b) This one, in my opinion, is more difficult. My boundaries will be ## \alpha \in \left[0, \frac{\pi}{2} \right]## and ##\phi \in \left[0, 2\pi \right ) ## So, for my F, I know that ## F= \vec{F} \cdot d\vec {r} ## where I can either convert to Cartesian, or try to just say that ## \vec{F} = F_{\alpha} \hat {\alpha} + F_{\phi} \hat {\phi} ## and ## d\vec {r} = a \cot \alpha d\alpha \hat {\alpha} + a \sin \alpha d\phi \hat {\phi} ## making ## F = a F_{\alpha} \cot \alpha d\alpha + a F_{\phi} \sin \alpha d\phi ## which would make ## dF = \left( a \frac{\partial F_\phi}{\partial \alpha}+a F_\phi \cos \phi-a \cot \alpha \frac{\partial F_\alpha}{\partial \phi} \right) d\alpha \wedge d\phi ## using stokes tells us that our surface integral is ## \int_S \left( -a \cot \alpha \frac{\partial F_\alpha}{\partial \phi} + a \frac{\partial F_\phi}{\partial \alpha}+a F_\phi \cos \phi \right) d\alpha \wedge d\phi = \int^{\frac{\pi}{2}}_{0} F_{\alpha} a \cot \alpha d\alpha + \int^{\frac{\pi}{2}}_{0} F_{\phi} a \sin \alpha d\phi ##
which if I do it, I get
however, there is a problem with this, I don't know my functions true identities? So must I really go through converting to Cartesian? Or is there something I'm missing? I know in Cartersian that ## x = a\sin \alpha \cos \phi ## ## y = a \sin \alpha \sin \alpha ## and ## z = -a \cos \alpha - ln {\tan{\frac{\alpha}{2}}}## so I could work it out if i really had to, but I think I might be missing something obvious!