Does it necessarily follow that the integral curves of $k^a$ are null geodesics?Geodesics of null surface and induced connectionIntegral curves of the gradientParameter Curves are GeodesicsA smooth function f satisfies $left|operatorname grad f right|=1$ ,then the integral curves of $operatornamegrad f$ are geodesicsIntegral curves in null hypersurfacesIntegral curves and null geodesicsIdentity in general relativity, not sure if true or not“Flow lines” of “dust” are geodesics?Integral curves of vector field are geodesicsOrthogonal geodesics to hypersurfacesWhy there are such angular coordinates?
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Does it necessarily follow that the integral curves of $k^a$ are null geodesics?
Geodesics of null surface and induced connectionIntegral curves of the gradientParameter Curves are GeodesicsA smooth function f satisfies $left|operatorname grad f right|=1$ ,then the integral curves of $operatornamegrad f$ are geodesicsIntegral curves in null hypersurfacesIntegral curves and null geodesicsIdentity in general relativity, not sure if true or not“Flow lines” of “dust” are geodesics?Integral curves of vector field are geodesicsOrthogonal geodesics to hypersurfacesWhy there are such angular coordinates?
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Let $f$ be a function on a spacetime $(M, g_ab)$ whose gradient, $k_a = nabla_a f$, ie everywhere null, i.e., $k_ak^a = 0$ throughout $M$. Does it necessarily follow that the integral curves of $k^a$ are null geodesics?
differential-geometry manifolds riemannian-geometry mathematical-physics general-relativity
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$begingroup$
Let $f$ be a function on a spacetime $(M, g_ab)$ whose gradient, $k_a = nabla_a f$, ie everywhere null, i.e., $k_ak^a = 0$ throughout $M$. Does it necessarily follow that the integral curves of $k^a$ are null geodesics?
differential-geometry manifolds riemannian-geometry mathematical-physics general-relativity
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add a comment |
$begingroup$
Let $f$ be a function on a spacetime $(M, g_ab)$ whose gradient, $k_a = nabla_a f$, ie everywhere null, i.e., $k_ak^a = 0$ throughout $M$. Does it necessarily follow that the integral curves of $k^a$ are null geodesics?
differential-geometry manifolds riemannian-geometry mathematical-physics general-relativity
$endgroup$
Let $f$ be a function on a spacetime $(M, g_ab)$ whose gradient, $k_a = nabla_a f$, ie everywhere null, i.e., $k_ak^a = 0$ throughout $M$. Does it necessarily follow that the integral curves of $k^a$ are null geodesics?
differential-geometry manifolds riemannian-geometry mathematical-physics general-relativity
differential-geometry manifolds riemannian-geometry mathematical-physics general-relativity
edited yesterday
Andrews
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asked Apr 4 '16 at 3:18
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The condition that $k$ is a gradient implies that it is curl-free; i.e. $nabla_i k_j = nabla_j k_i$. Let $gamma$ be an integral curve of $k^i$; i.e. $dot gamma^i(t) = k^i(gamma(t))$. Then replacing $dot gamma$ with $k$ in the covariant acceleration and applying the curl-free condition we get $$ddot gamma^i = dot gamma^j nabla_j dot gamma^i = k^j nabla_j k^i = k^j nabla^i k_j.$$
Now we're basically done - just recognize the RHS as $frac12 nabla^i (k^j k_j)$, at which point the fact that $k$ is null ($k^j k_j = 0$) tells us that $ddot gamma = 0$; i.e. $gamma$ is a geodesic.
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1 Answer
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$begingroup$
The condition that $k$ is a gradient implies that it is curl-free; i.e. $nabla_i k_j = nabla_j k_i$. Let $gamma$ be an integral curve of $k^i$; i.e. $dot gamma^i(t) = k^i(gamma(t))$. Then replacing $dot gamma$ with $k$ in the covariant acceleration and applying the curl-free condition we get $$ddot gamma^i = dot gamma^j nabla_j dot gamma^i = k^j nabla_j k^i = k^j nabla^i k_j.$$
Now we're basically done - just recognize the RHS as $frac12 nabla^i (k^j k_j)$, at which point the fact that $k$ is null ($k^j k_j = 0$) tells us that $ddot gamma = 0$; i.e. $gamma$ is a geodesic.
$endgroup$
add a comment |
$begingroup$
The condition that $k$ is a gradient implies that it is curl-free; i.e. $nabla_i k_j = nabla_j k_i$. Let $gamma$ be an integral curve of $k^i$; i.e. $dot gamma^i(t) = k^i(gamma(t))$. Then replacing $dot gamma$ with $k$ in the covariant acceleration and applying the curl-free condition we get $$ddot gamma^i = dot gamma^j nabla_j dot gamma^i = k^j nabla_j k^i = k^j nabla^i k_j.$$
Now we're basically done - just recognize the RHS as $frac12 nabla^i (k^j k_j)$, at which point the fact that $k$ is null ($k^j k_j = 0$) tells us that $ddot gamma = 0$; i.e. $gamma$ is a geodesic.
$endgroup$
add a comment |
$begingroup$
The condition that $k$ is a gradient implies that it is curl-free; i.e. $nabla_i k_j = nabla_j k_i$. Let $gamma$ be an integral curve of $k^i$; i.e. $dot gamma^i(t) = k^i(gamma(t))$. Then replacing $dot gamma$ with $k$ in the covariant acceleration and applying the curl-free condition we get $$ddot gamma^i = dot gamma^j nabla_j dot gamma^i = k^j nabla_j k^i = k^j nabla^i k_j.$$
Now we're basically done - just recognize the RHS as $frac12 nabla^i (k^j k_j)$, at which point the fact that $k$ is null ($k^j k_j = 0$) tells us that $ddot gamma = 0$; i.e. $gamma$ is a geodesic.
$endgroup$
The condition that $k$ is a gradient implies that it is curl-free; i.e. $nabla_i k_j = nabla_j k_i$. Let $gamma$ be an integral curve of $k^i$; i.e. $dot gamma^i(t) = k^i(gamma(t))$. Then replacing $dot gamma$ with $k$ in the covariant acceleration and applying the curl-free condition we get $$ddot gamma^i = dot gamma^j nabla_j dot gamma^i = k^j nabla_j k^i = k^j nabla^i k_j.$$
Now we're basically done - just recognize the RHS as $frac12 nabla^i (k^j k_j)$, at which point the fact that $k$ is null ($k^j k_j = 0$) tells us that $ddot gamma = 0$; i.e. $gamma$ is a geodesic.
answered Apr 4 '16 at 12:13
Anthony CarapetisAnthony Carapetis
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