What is the metric tensor on a spherical surface?

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SUMMARY

The metric tensor on a spherical surface is defined using the parametrization of the sphere of radius ρ centered at the origin, given by the function f(θ, φ) = (ρ sin(θ) cos(φ), ρ sin(θ) sin(φ), ρ cos(θ)). The components of the metric tensor are calculated using the inner products of the partial derivatives of this function, resulting in a matrix G(θ, φ) that includes g_{11}, g_{12}, g_{21}, and g_{22}. The calculation of these derivatives is essential for determining the metric tensor's values.

PREREQUISITES
  • Understanding of spherical coordinates and their parametrization
  • Knowledge of differential calculus, specifically partial derivatives
  • Familiarity with inner product notation in vector calculus
  • Basic concepts of tensor analysis
NEXT STEPS
  • Calculate the derivatives of the parametrization function f(θ, φ) to derive the metric tensor components
  • Explore the implications of the metric tensor in general relativity and differential geometry
  • Learn about the applications of the metric tensor in physics, particularly in curved spaces
  • Investigate the relationship between the metric tensor and geodesics on spherical surfaces
USEFUL FOR

Mathematicians, physicists, and students studying differential geometry or general relativity, particularly those interested in the properties of spherical surfaces and metric tensors.

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What is the metric tensor on a spherical surface?
 
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I learned this like 2 minutes ago but I believe the following is correct:

A parametrisation of the sphere of radius \rho centered on the origin is

f(\theta, \phi)=(\rho \sin(\theta) \cos(\phi) , \rho \sin(\theta)\sin(\phi),\rho \cos(\theta))

where I am using this convention for the spherical angles : http://en.wikipedia.org/wiki/Spherical_coordinates#Spherical_coordinates

The components of the metric tensor are then

g_{11}(\theta, \phi) = \langle \frac{\partial f}{\partial \theta}, \frac{\partial f}{\partial \theta} \rangle
g_{12}(\theta, \phi) = \langle \frac{\partial f}{\partial \theta}, \frac{\partial f}{\partial \phi} \rangle
g_{21}(\theta, \phi) = \langle \frac{\partial f}{\partial \phi}, \frac{\partial f}{\partial \theta} \rangle
g_{22}(\theta, \phi) = \langle \frac{\partial f}{\partial \phi}, \frac{\partial f}{\partial \phi} \rangleThe matrix form is then

G(\theta, \phi)=\left( \begin {array} {cc} g_{11}(\theta, \phi) & g_{12}(\theta, \phi) \\ g_{21}(\theta, \phi) & g_{22}(\theta, \phi) \end {array} \right)

All you got to do is calculate the derivatives. Have fun. :p
 
Last edited:

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