Context: Deriving the maximally symmetric- isotropic and homogenous- spatial metric
I've seen a fair few sources state that the Rienamm tensor associated with the metric should take the form:
* ##R_{abcd}=K(g_{ac}g_{bd}-g_{ad}g_{bc})##
The arguing being that a maximally symmetric space has...
In schwarzschild metric:
$$ds^2 = e^{v}dt^2 - e^{u}dr^2 - r^2(d\theta^2 +sin^2\theta d\phi^2)$$
where v and u are functions of r only
when we calculate the Ricci tensor $R_{\mu\nu}$ the non vanishing ones will only be $$R_{tt}$$,$$R_{rr}$$, $$R_{\theta\theta}$$,$$R_{\phi\phi}$$
But when u and v...
When working with light-propagation in the FRW metric
$$ds^2 = - dt^2 + a^2 ( d\chi^2 + S_k(\chi) d\Omega^2)$$
most texts just set $$ds^2 = 0$$ and obtain the equation
$$\frac{d\chi}{dt} = - \frac{1}{a}$$
for a light-ray moving from the emitter to the observer.
Question1: Do we not strictly...
Hello everyone, I already know that the solution to this question is obvious but I can't find it.
Consider an expanding universe following the FRW metric ds^2=-dt^2-a^2(t)dx^2 (1 space dimension for simplicity). We know that the physical spatial distance x_p is related to the comoving spatial...
In a paper published in Reviews of Modern Physics in 1949, http://journals.aps.org/rmp/pdf/10.1103/RevModPhys.21.378 , H.P. Robertson provided an analysis of the physical implications of the Michelson/Morley, Kennedy and Thorndike, and Ives and Stilwell experiments which seems definitive with...
I have been recently working with Schwarzschild's solution:
ds2= - (1- (2GM/rc2))c2dt2 + dr2/(1-2GM/rc2) + r2(dθ2 + sin2(θ)d∅2)
Now, when deriving the various general relativistic tensors for this metric such as the Ricci tensor, I found the calculations to be painfully tedious and monstrous...
I have a doubt since I see the next equation and the corresponding matrix:
$$ ds^2 = \Bigg( \frac{1-\frac{r_s}{4\rho}}{1+\frac{r_s}{4\rho}}\Bigg)^2 dt^2 - \Big(1+\frac{r_s}{4\rho}\Big)^4 (d\rho^2 + p^2 d\Omega_2^2) $$$$ g_{\mu\nu} =
\left( \begin{array}{ccc}
\Bigg(...
Hello,
this is the metric I am talking about:
$$ ds^2= (dt - A_idx^i)^2 - a^2(t)\delta_{ij}dx^idx^j $$
I never see one like this. How the metric tensor matrix would be?
Is there any book or reference perhaps on string theory or superstring theory or even advanced general relativity that treats the Israel Wilson Perjes metric using the tetrad formalism in details, i.e, 1-forms and so? (Not spinors methos) I have ran across many papers that just place the spin...
In SRT, the line element is ##c^2ds^2 = c^2dt^2 - dx^2 -dy^2-dz^2## and ##g_{00} = 1## (or ##-1## depending on sign conventions). In the Schwarzschild metric we have
g_{00}=(c^2-\frac{2 GM}{r}) .
So in the first example, ##g_{00}## is constant, in the second it depends on another coordinate...
Hey! :o
In a space of finite measure, if $f$ and $g$ are measurable we set $\rho (f,g)=\int \frac{|f-g|}{1+|f-g|}d \mu$.
Show that $\rho$ is metric and that $f_n \rightarrow f$ as for $\rho$ if and only if $\forall c>0$ we have that $\mu(\{|f_n-f|>c\})\rightarrow 0$.What does "$f_n \rightarrow...
1. "William Tell is said to have shot an apple off his son's head with an arrow. If the arrow was shot with an initial speed of 55m/s and the boy was 15m away, at what launch angle did Bill aim the Arrow? (Assume that the arrow and the apple are initially at the same height above the...
Suppose, I know the metric tensor of a 2D space. for example, the metric tensor of a sphere of radius R,
gij = ##\begin{pmatrix} R^2 & 0 \\ 0 & R^2\cdot sin^2\theta \end{pmatrix}##
,and I just know the metric tensor, but don't know that it is of a sphere.
Now I want to draw a 2D space(surface)...
How does one get time dilation, length contraction, and E=mc^2 from the spacetime metric?
Suppose all that you are given is x12 + x22 + x32 - c2t2 = s2
How do you derive time dilation, length contraction, and E=mc^2 from this?
What is the most direct way to do this?
I've never seen a satisfactory explanation of the metrics used in a calculation of distance in Minkowski space. In Euclidean space, the distance is:
ds^2 = dx^2 + dy^2 + dz^2
But in Minkowski space, the distance is
ds^2 = (dt * c)^2 - dx^2 - dy^2 - dz^2
Why are the signs reversed? This implies...
This is a question inspired by the "Golf Ball" thread, which is no longer open for comments, I guess.
For a black hole of constant mass, the metric external to the black hole can be written in Schwarzschild metric, which is characterized by the constant M, and the corresponding radius 2 M...
A metric space is considered complete if all Cauchy sequences converge within the metric space. I was just curious if you could have a case of a metric space that doesn't have any Cauchy sequences in it. Wouldn't it be complete by default?
When trying to think of a space with no cauchy...
Hello,
I have a simple question about deriving $$g_{ij}
\frac{\partial x^i}{\partial t}\frac{\partial x^j}{\partial t}$$
with respect to time t.
I have noticed that the first term after derivation turns out to be$$ \frac{\partial g_{ij}}{\partial x^k} \frac{\partial x^k}{\partial...
First of all, the metric I am referring to is this one:
ds2= -c2dt2 + dl2 + (k2 + l2)(dᶿ2 + sin2(ᶿ)dø2)
where k is the radius of the throat of the wormhole. (sorry for the small Greek letters)
Now I have two questions about this solution to Einstein's equations:
1. What does the coordinate l...
OK. A problem is simple and probably very stupid... In many (most of) maths books things like Euclidean metric, norm, scalar product etc. are defined in Cartesian coordinate system (that is one which is orthonormal). But what would happen if one were to define all these quantities in...
Homework Statement
I am confused if there is any standard way to check what should be the line element $$ds^{2}$$ when the dimensions are more than three ( since we don't have the option to draw things as we usually do in case of 3d or less dimensional cases. I am following Hobson's book. I am...
What is the most general method of obtaining the event-horizon from the given black hole metric.
Let us consider Kerr black hole in Kerr coordinates given by
ds^2 = -\frac{\Delta-a^2sin^2\theta}{\Sigma}dv^2+2dvdr -\frac{2asin^2\theta(r^2+a^2-\Delta)}{\Sigma}dvd\chi-2asin^2\theta d\chi dr +...
As you may know, the metric tensor for 3D spherical coordinates is as follows:
g11= 1
g22= r2
g33= r2sin2(θ)
Now, the Minkowski metric tensor for spherical coordinates is this:
g00= -1
g11= 1
g22= r2
g33= r2sin2(θ)
In both of these metric tensors, all other elements are 0.
Now...
I am attempting to read my first book in QFT, and got stuck.
A Lorentz transformation that preserves the Minkowski metric \eta_{\mu \nu} is given by x^{\mu} \rightarrow {x'}^{\mu} = {\Lambda}^\mu_\nu x^\nu . This means \eta_{\mu \nu} x^\mu x^\nu = \eta_{\mu \nu}x'^\mu x'^\nu for all x...
After my recent studies of the curvature of the 2- sphere, I would like to move on to Minkowski space. However, I can not seem to find the metric tensor of the 4 sphere on line, nor can I seem to think of the vector of transformation properties that I would use to derive the metric tensor of the...
I have one question, which I don't know if I should post here again, but I found it in GR...
When you have a metric tensor with components:
g_{\mu \nu} = \eta _{\mu \nu} + h_{\mu \nu}, ~~ |h|<<1 (weak field approximation).
Then the inverse is:
g^{\mu \nu} = \eta^{\mu \nu} - h^{\mu \nu}...
Homework Statement
Consider the Schwarschield Metric in four dimensional spacetime (M is a constant):
ds2 = -(1-(2M/r))dt2 + dr2/(1-(2M/r)) + r2(dθ2 + sin2(θ)dø2)
a.) Write down the non zero components of the metric tensor, and find the inverse metric tensor.
b.) find all the...
I was recently trying to test something out with the Riemann tensor. I used only 2 dimensions for simplicity sake. As I was deriving the Riemann tensor, I noticed that it looked as if all of the elements were going to come out to be 0 (which they all did). Therefore, this coordinate system is...
Can the above logic be applied to Schw. Metric as well?
Suppose I have an object moving with a radial velocity v=const, then can I do the same to derive the Schwarchild time dilation as in the Minkowski?
dr = v ~ dt
ds^{2} = [K - \frac{v^2}{K} ] dt^2
So \gamma ^{-1} = \sqrt{K} [1 -...
Hello,
I am trying to understand Kaluza Klein theory on the five dimensional unification. It was mentioned over there:
" Of the 15 components of gαβ, five had to get a new physical interpretation, i.e. gα5 and g55; the components gik, i,k = 1,...,4, were to describe the gravitational field...
The Schwarzschild Metric has a form:
##ds^2 = Kdt^2 - 1/K dr^2 - r^2dO^2##
where: K = 1 - a/r;
There is a time scaled by K, but a space radially by 1/K.
This is a typical time dilation and a space contraction, which is known from SR,
but the Schwarzschild metrics is spherically...
Hello,
I'm wondering what the exact definition of a local conformal transformation is, in the context of General Relativity (/Shape Dynamics)
To be more precise:
1. Are local conformal transformations coordinate transformations or scalar transformations of the metric?
2. If they are...
Alright, so I was reading up on tensors and such with non-Cartesian coordinate systems all day but now I'm a bit tired an confused so you'll have to forgive me if it's a stupid question. So to express the dot product in some coordinate system, it's:
g(\vec{A}\,,\vec{B})=A^aB^bg_{ab}
And, if...
I think this will be a quick question...
If the Schw's metric is a solution of the vacuum, then what does the mass M_0 in the metric correspond to? I thought it was the mass of the star... but if that's true then why is it a vacuum solution?
Or is it vacuum because it describes the regions...
In the Wiki article about the Vaidya metric :
http://en.wikipedia.org/wiki/Vaidya_metric
there is mention of a "further generalisation" called the Kinnersley metric, without giving any details or even a reference. Is this a generalisation of the Vaidya metric to include angular momentum (...
Error below [/color]
For a couple of years now, I have been attempting to solve for the values in GR of the time dilation z and the radial and tangent length contractions, L and L_t respectively, which form the metric
c^2 dτ^2 = c^2 z^2 dt^2 - dr^2 / L^2 - d_θ^2 r^2 / L_t^2 (along a plane)...
if we know
K^{a b}= (∇^a*ζ^b -∇^b*ζ^a)/2,
ζ is a killing vector,
under the variation of metric g_{a b}→g_{a b}+δ(g_{a b}) which preserves the Killing vector δ(ζ^a)=0,
h_{a b} = δ(g_{a b}) = ∇^a*ζ^b +∇^b*ζ^a,
how to prove
δ(K^{a b})= ζ_c*∇^a*h^{b c} - h^{c a}*∇_c*ζ^b - (...
The killing form can be defined as the two-form ##K(X,Y) = \text{Tr} ad(X) \circ ad(Y)## and it has matrix components ##K_{ab} = c^{c}_{\ \ ad} c^{d}_{\ \ bc}##. I have often seen it stated that for a compact simple group we can normalize this metric by
##K_{ab} = k \delta_{ab}## for some...
The action for Yang-Mill's theory is often written as
$$ S= \int \frac{1}{4}\text{Tr} (F^{\mu \nu} F_{\mu \nu})d^4 x = \int d^4 x\frac{1}{4} F^{k \mu \nu} F_{k \mu \nu}$$
where latin indices are indicies in the lie algebra, and the trace is taken with respect to the inner product...
[SIZE="4"]Definition/Summary
The metric tensor g_{\mu\nu} is a 4x4 matrix that is determined by the curvature and coordinate system of the spacetime
[SIZE="4"]Equations
The proper time is given by the equation
d\tau^2=dx^{\mu}dx^{\nu}g_{\mu\nu}
using the Einstein summation convention...
Hello. I am new to engineering and to imperial units, and currently learning by doing some exercises. I'm stuck on the following conversion:
0.04 g / min x m^3 -> lbm / hr x ft^3
I figured it like this:
0.04 g / min x m^3 x (60min/1hr) x (1m/35,314)^3 x (1 lbm / 454g) =
1,49x10^-4 lbm...
The killing form on a lie algebra is defined as
$$B(X,Y) = \text{Tr}ad_X \circ ad_Y$$
where ##ad_X: \mathfrak{g} \to \mathfrak{g}## is given by ##ad_X(Y) = [X,Y]##, where the latter is the lie bracket between X and Y in ##\mathfrak{g}##. Expressed in terms of components on a basis on...
Dear all,
As I was reading my book. It said that the line element of a particular coordinate system (spherical) in R^{3} is so and so. Then it said that the metric is flat. I don't get how the metric is flat in spherical coordinate. Could someone shed some light on this please?
Thanks
Dear all,
In my journey through learning General relativity. I have stumbled upon this problem. I have to calculate the geodesic equation for R^{3} in cylindrical polars. I am not sure how to use the metric connection. The indices confuse me. I would appreciate it if someone could shade some...
I have recently been studying the tensors on the left side of the Einstein field equations, but I have been studying and deriving them in 3-D. I would now like to move on to adding time into the mixture.
I have some questions regarding the Minkowski metric \eta\mu\nu.
First, I know that...
I recently derived a matrix which I believe to be the metric tensor in spherical polar coordinates in 3-D. Here were the components of the tensor that I derived. I will show my work afterwards:
g11 = sin2(ø) + cos2(θ)
g12 = -rsin(θ)cos(θ)
g13 = rsin(ø)cos(ø)
g21 = -rsin(θ)cos(θ)...
Under a change of variables:
x^{\mu} \rightarrow x^{\mu}+ \delta x^{\mu}
How can I see how the determinant of the metric changes?
\sqrt{|g(x)|}?
Is it correct to see it as a function?
f(x) \rightarrow f(x+ \delta x) = f(x) + \delta x^{\mu} \partial_{\mu} f(x)
?