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11:00 PM
And answer my context question. It looks like you're using the expression for the Riemannian metric in normal polar coordinates. Warning: Because of the virus, I am not home, so I have neither my computer nor my library.
 
The context is that I have a 2D metric in the following general form $g=t(dt)^{2}+G(t,x)(dx)^{2}$ and I want to figure out how the metric component( function of (t,x)) $G(t,x)$ has to look like to avoid a curvature singularity (re Gauss curvature).
 
How badly hit is the area of the US you live in? @Ted
 
Not too bad yet, Alessandro. I've been essentially indoors for about two weeks.
 
@TedShifrin Here is the question again:

I have calculated the Gauss curvature for $g=t(dt)^{2}+G(t,x)(dx)^{2}$:

$K=-\frac{1}{2}\frac{\frac{\partial^{2}G}{\partial t^{2}}}{tG}+\frac{1}{4}\left(\frac{\frac{\partial G}{\partial t}}{t^{2}G}+\frac{(\frac{\partial G}{\partial t})^{2}}{tG^{2}}\right)=-\frac{2Gt\cdot\frac{\partial^{2}G}{\partial t^{2}}-\frac{\partial G}{\partial t}(\frac{\partial G}{\partial t}\cdot t+G)}{4G^{2}t^{2}}$, and apparently it diverges for $G^{2}t^{2}=0$. I am trying to figure out how $G:=G(t,x)$ (which is defined for all $t,x\in\mathbb{R}$) has to look like in order t
 
@eigenvalue: i'm troubled by the $t$ coefficient. So we're on $t\ge 0$ only.
 
11:04 PM
Good, I hope you remain safe and healthy
 
You wrote $t\in\Bbb R$.
Me too, Alessandro. I went to a doctor more than 2 wks ago who, it turned out, subsequently tested positive. But no symptoms for me.
 
It's a signature changing metric again. so it's valid vor all t. The Gauss curvature diverges at t=0 (= hyper surface of signature change)
 
Oh, right. I never do that stuff :)
But we have a singular metric when $t=0$.
 
I am actually trying to figure out how G should look like to avoid the divergence. How can I use the Taylor expansion to figure that out?
@TedShifrin You tested positive? Did the doctor tell you whether you are immune now (for this and future outbreaks)?
 
I would have to compute myself, using moving frames.
No, the doctor tested positive. With no symptoms I can't be tested (yet).
 
11:09 PM
Of what use is the Taylor series in this context? I have heard that it could be useful but don't see how or why?
Oh, I see. It's a shame that getting tested is such a problem. There should be at home test kits for everyone.
 
You don't know the zero in the denominator isn't canceled by the numerator without computing Taylor expansion (in $t$), yes.
I will do my own computation. Give me a few minutes.
 
Thanks! :-)
I am so happy to be able to talk with someone about this. Nothing worse that being stuck at home with nobody around to discuss your stuff with
 
Is the metric with $G$ or $G^2$?
 
The metric is: $g=t(dt)^{2}+G(t,x)(dx)^{2}$
 
OK, I agree with your formula.
Are we expecting $G\ne 0$ at dt=0$?
 
11:23 PM
You mean the formula for the Taylor series?
 
No, I worked out $K$.
 
I assume $G(t,x)\geq0$ for all $t$.
Because only the two metric signs (-,+) and (+,+) occur, I only need to consider the non-negative case $G(t,x)\geq0$.
But looking at the formula $K=-\frac{2Gt\cdot\frac{\partial^{2}G}{\partial t^{2}}-\frac{\partial G}{\partial t}(\frac{\partial G}{\partial t}\cdot t+G)}{4G^{2}t^{2}}$ I thought that we have to have $t^{2}G^{2}(t,x)\neq0$ to avoid a curvature singularity at $t=0$
 
Write $G = G_0 + tG_1+ t^2G_2+ \dots$. Assume $G_0 >0$. If $G_0=0$, then your sign condition says $G_1=0$ too, so factor out the $t^2$ and proceed similarly.
I would write partials as subscripts for convenience.
No, you're wrong. Obviously it vanishes at $t=0$. You have to figure out how to cancel with the numerator and get a removable singularity.
The $G_i$ in my notation are functions of $x$, so computing $t$ derivatives is easy.
 
ok, so in your notation the $G = G_0 + tG_1+ t^2G_2+ \dots$ is the Taylor series. ... - I see, that's why the Taylor series becomes useful?
... It makes more sense now. I am going to work on that now.... and allow myself to bug you again if I get suck somewhere... hope that's fine with you?
 
Sure. I'm not around as much as usual because I'm not at home with my computer. But sure.
 
11:34 PM
Sounds good!
Make sure you stay healthy (or as healthy as you can) and be safe!!
 
Of course :) You too.
 
Legit my math courses have gone online and I practically come here for advice.
 
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