Timelike geodesic curves for two-dimensional metric

In summary, the study of timelike geodesic curves in a two-dimensional metric explores the paths that particles follow in spacetime under the influence of gravity. These curves are determined by the metric's properties, which define the geometry of the space. The analysis involves deriving the equations of motion for particles, examining the conditions under which these curves are parametrized, and understanding their implications for the behavior of matter and energy in a two-dimensional universe. The results provide insights into the fundamental structure of spacetime and the nature of gravitational interactions in lower-dimensional theories.
  • #1
Fisherlam
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Homework Statement
For the two-dimensional metric ##ds^2 = [dx^2 + c^2dt^2] /(\alpha t^{-2})##, with ##\alpha## being a constant of appropriate dimensions, show that $$\frac{dx/dt}{\sqrt{1-(dx/dt)^2}}$$ is constant and hence, or otherwise, find all timelike geodesic curves.
Relevant Equations
$$L=g_{ab}\dot{x}^a\dot{x}^b $$ $$\frac{\partial L}{\partial x}=\frac{\partial }{\partial u}\left(\frac{\partial L}{\partial \dot{x}}\right) $$
Using EL equation, $$L=\left(\frac{t^2}{\alpha}\dot{x}^2-\frac{c^2t^2}{\alpha}\dot{t}^2\right)^{0.5} \Longrightarrow \mathrm{constant} =\left(\dot{x}^2 -c^2 \dot{t}^2\right)^{-0.5} \left(\frac{t^2}{\alpha}\right)^{0.5} \dot{x}$$.

Get another equation from the metric: $$ds^2=-\frac{c^2t^2}\alpha dt^2+\frac{t^2}\alpha dx^2=c^2d\tau^2\quad\Longrightarrow\quad-\frac{c^2t^2}\alpha t^2+\frac{t^2}\alpha\dot{x}^2=c^2\quad\Longrightarrow\quad\frac{t^2}\alpha=\frac{c^2}{\dot{x}^2-c^2\dot{t}^2}$$

Substitution and set ##c=1##: $$\mathrm{constant}=\left(\dot{x}^2-c^2\dot{t}^2\right)^{-0.5}\left(\frac{t^2}\alpha\right)^{0.5}\dot{x}=\frac{c\dot{x}}{\dot{x}^2-c^2\dot{t}^2}=\frac{\dot{x}}{\dot{x}^2-\dot{t}^2}=\cdots?$$

I think I am close but clearly missing something...
 
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  • #3
I've done some digging and if this comes from the Cambridge Part II Physics 2021 past paper, then this is actually a typo. They actually wanted you to find the first conserved quantity which you've obtained from the E-L equations.
 

FAQ: Timelike geodesic curves for two-dimensional metric

What is a timelike geodesic curve?

A timelike geodesic curve is a path in spacetime that represents the trajectory of a particle moving slower than the speed of light. In general relativity, these curves are the shortest paths between two points in a curved spacetime, and they correspond to the motion of particles with mass. In a two-dimensional metric, these curves can be analyzed using the properties of the metric tensor to understand how they behave in the given spacetime geometry.

How do you determine if a curve is timelike in a two-dimensional metric?

To determine if a curve is timelike in a two-dimensional metric, one must compute the metric tensor for the spacetime and evaluate the curve's tangent vector at each point along the curve. If the inner product of the tangent vector with itself, using the metric tensor, is negative (in a signature convention where time is negative), then the curve is classified as timelike. This indicates that the curve can be traversed by a particle moving at subluminal speeds.

What is the significance of geodesics in general relativity?

Geodesics are significant in general relativity because they describe the motion of free-falling particles in curved spacetime. They represent the paths that particles follow when no external forces act upon them, essentially indicating how gravity influences motion. Understanding geodesics helps physicists predict the behavior of objects in gravitational fields, such as planets orbiting stars or light bending around massive objects.

Can timelike geodesics intersect each other?

In general relativity, timelike geodesics cannot intersect each other in a globally consistent manner. If two timelike geodesics were to intersect, it would imply the existence of two different worldlines for the same particle, which violates the principle of uniqueness of particle trajectories. However, different particles can follow their own distinct timelike geodesics that may come close to or cross paths without violating this principle.

What are the properties of timelike geodesics in a two-dimensional spacetime?

In a two-dimensional spacetime, timelike geodesics exhibit several important properties. They are characterized by having a constant proper time along the curve, meaning that an observer moving along the geodesic experiences a consistent passage of time. Additionally, timelike geodesics are locally the shortest paths between two points in spacetime, and they can be described mathematically using the geodesic equation derived from the metric. The curvature of the spacetime affects the shape and behavior of these geodesics, leading to phenomena such as gravitational time dilation.

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