Is velocity field extendible to a vector field on the whole manifold?












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In DoCarmo’s Riemannian Geometry book, an affine connection $nabla$ on a smooth manifold $M$ is defined to be a mapping :$Xi(M)times Xi(M)rightarrow Xi(M)$, where $Xi(M)$ is the set of all smooth vector fields on $M$.



Now DoCarmo wants to clarify this definition with a theorem containing the following fact: ... c) if $V$ is a vector field along the curve $c$, and if $V$ is induced by a vector field $Yin Xi(M)$, then the covariant derivative of $V$ along $c$ denoted by $frac{DV}{dt}$ equals $nabla(frac{dc}{dt},Y)$, where $frac{dc}{dt}$ is the velocity field of the curve $c$.



But the domain of $nabla$ does not include $(frac{dc}{dt},Y)$, since $frac{dc}{dt}$ does not belong to $Xi(M)$. What is the justification?










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  • You can extend $frac{dc}{dt}$ to a smooth vector field on the manifold, and the value of the directional derivative along $c$ is independent of that choice.
    – Charlie Frohman
    Nov 23 at 13:05










  • DoCarmo immediately after defining $frac{dc}{dt}$ states that vector fields along a curve do not necessarily extend to the whole manifold @CharlieFrohman
    – User12239
    Nov 23 at 13:09










  • math.stackexchange.com/questions/1865661/…. According to this, the velocity field is generally not a vector field on the whole manifold
    – User12239
    Nov 23 at 13:14










  • The connection is defined globally on sections of the tangent bundle. Then one can show that the value of the covariant derivative $nabla_XY$ at a point $p$ actually only depends on the value $X_p$ and $Y$ in a neighborhood of $p$. This allows for the $frac{D}{dt}$ to be well-defined.
    – Matt
    Nov 23 at 14:02










  • Thanks, I got it completely now @CharlieFrohman and Matt
    – User12239
    Nov 23 at 15:17
















0














In DoCarmo’s Riemannian Geometry book, an affine connection $nabla$ on a smooth manifold $M$ is defined to be a mapping :$Xi(M)times Xi(M)rightarrow Xi(M)$, where $Xi(M)$ is the set of all smooth vector fields on $M$.



Now DoCarmo wants to clarify this definition with a theorem containing the following fact: ... c) if $V$ is a vector field along the curve $c$, and if $V$ is induced by a vector field $Yin Xi(M)$, then the covariant derivative of $V$ along $c$ denoted by $frac{DV}{dt}$ equals $nabla(frac{dc}{dt},Y)$, where $frac{dc}{dt}$ is the velocity field of the curve $c$.



But the domain of $nabla$ does not include $(frac{dc}{dt},Y)$, since $frac{dc}{dt}$ does not belong to $Xi(M)$. What is the justification?










share|cite|improve this question
























  • You can extend $frac{dc}{dt}$ to a smooth vector field on the manifold, and the value of the directional derivative along $c$ is independent of that choice.
    – Charlie Frohman
    Nov 23 at 13:05










  • DoCarmo immediately after defining $frac{dc}{dt}$ states that vector fields along a curve do not necessarily extend to the whole manifold @CharlieFrohman
    – User12239
    Nov 23 at 13:09










  • math.stackexchange.com/questions/1865661/…. According to this, the velocity field is generally not a vector field on the whole manifold
    – User12239
    Nov 23 at 13:14










  • The connection is defined globally on sections of the tangent bundle. Then one can show that the value of the covariant derivative $nabla_XY$ at a point $p$ actually only depends on the value $X_p$ and $Y$ in a neighborhood of $p$. This allows for the $frac{D}{dt}$ to be well-defined.
    – Matt
    Nov 23 at 14:02










  • Thanks, I got it completely now @CharlieFrohman and Matt
    – User12239
    Nov 23 at 15:17














0












0








0







In DoCarmo’s Riemannian Geometry book, an affine connection $nabla$ on a smooth manifold $M$ is defined to be a mapping :$Xi(M)times Xi(M)rightarrow Xi(M)$, where $Xi(M)$ is the set of all smooth vector fields on $M$.



Now DoCarmo wants to clarify this definition with a theorem containing the following fact: ... c) if $V$ is a vector field along the curve $c$, and if $V$ is induced by a vector field $Yin Xi(M)$, then the covariant derivative of $V$ along $c$ denoted by $frac{DV}{dt}$ equals $nabla(frac{dc}{dt},Y)$, where $frac{dc}{dt}$ is the velocity field of the curve $c$.



But the domain of $nabla$ does not include $(frac{dc}{dt},Y)$, since $frac{dc}{dt}$ does not belong to $Xi(M)$. What is the justification?










share|cite|improve this question















In DoCarmo’s Riemannian Geometry book, an affine connection $nabla$ on a smooth manifold $M$ is defined to be a mapping :$Xi(M)times Xi(M)rightarrow Xi(M)$, where $Xi(M)$ is the set of all smooth vector fields on $M$.



Now DoCarmo wants to clarify this definition with a theorem containing the following fact: ... c) if $V$ is a vector field along the curve $c$, and if $V$ is induced by a vector field $Yin Xi(M)$, then the covariant derivative of $V$ along $c$ denoted by $frac{DV}{dt}$ equals $nabla(frac{dc}{dt},Y)$, where $frac{dc}{dt}$ is the velocity field of the curve $c$.



But the domain of $nabla$ does not include $(frac{dc}{dt},Y)$, since $frac{dc}{dt}$ does not belong to $Xi(M)$. What is the justification?







differential-geometry riemannian-geometry smooth-manifolds vector-fields






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share|cite|improve this question













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edited Nov 23 at 13:50

























asked Nov 23 at 12:56









User12239

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  • You can extend $frac{dc}{dt}$ to a smooth vector field on the manifold, and the value of the directional derivative along $c$ is independent of that choice.
    – Charlie Frohman
    Nov 23 at 13:05










  • DoCarmo immediately after defining $frac{dc}{dt}$ states that vector fields along a curve do not necessarily extend to the whole manifold @CharlieFrohman
    – User12239
    Nov 23 at 13:09










  • math.stackexchange.com/questions/1865661/…. According to this, the velocity field is generally not a vector field on the whole manifold
    – User12239
    Nov 23 at 13:14










  • The connection is defined globally on sections of the tangent bundle. Then one can show that the value of the covariant derivative $nabla_XY$ at a point $p$ actually only depends on the value $X_p$ and $Y$ in a neighborhood of $p$. This allows for the $frac{D}{dt}$ to be well-defined.
    – Matt
    Nov 23 at 14:02










  • Thanks, I got it completely now @CharlieFrohman and Matt
    – User12239
    Nov 23 at 15:17


















  • You can extend $frac{dc}{dt}$ to a smooth vector field on the manifold, and the value of the directional derivative along $c$ is independent of that choice.
    – Charlie Frohman
    Nov 23 at 13:05










  • DoCarmo immediately after defining $frac{dc}{dt}$ states that vector fields along a curve do not necessarily extend to the whole manifold @CharlieFrohman
    – User12239
    Nov 23 at 13:09










  • math.stackexchange.com/questions/1865661/…. According to this, the velocity field is generally not a vector field on the whole manifold
    – User12239
    Nov 23 at 13:14










  • The connection is defined globally on sections of the tangent bundle. Then one can show that the value of the covariant derivative $nabla_XY$ at a point $p$ actually only depends on the value $X_p$ and $Y$ in a neighborhood of $p$. This allows for the $frac{D}{dt}$ to be well-defined.
    – Matt
    Nov 23 at 14:02










  • Thanks, I got it completely now @CharlieFrohman and Matt
    – User12239
    Nov 23 at 15:17
















You can extend $frac{dc}{dt}$ to a smooth vector field on the manifold, and the value of the directional derivative along $c$ is independent of that choice.
– Charlie Frohman
Nov 23 at 13:05




You can extend $frac{dc}{dt}$ to a smooth vector field on the manifold, and the value of the directional derivative along $c$ is independent of that choice.
– Charlie Frohman
Nov 23 at 13:05












DoCarmo immediately after defining $frac{dc}{dt}$ states that vector fields along a curve do not necessarily extend to the whole manifold @CharlieFrohman
– User12239
Nov 23 at 13:09




DoCarmo immediately after defining $frac{dc}{dt}$ states that vector fields along a curve do not necessarily extend to the whole manifold @CharlieFrohman
– User12239
Nov 23 at 13:09












math.stackexchange.com/questions/1865661/…. According to this, the velocity field is generally not a vector field on the whole manifold
– User12239
Nov 23 at 13:14




math.stackexchange.com/questions/1865661/…. According to this, the velocity field is generally not a vector field on the whole manifold
– User12239
Nov 23 at 13:14












The connection is defined globally on sections of the tangent bundle. Then one can show that the value of the covariant derivative $nabla_XY$ at a point $p$ actually only depends on the value $X_p$ and $Y$ in a neighborhood of $p$. This allows for the $frac{D}{dt}$ to be well-defined.
– Matt
Nov 23 at 14:02




The connection is defined globally on sections of the tangent bundle. Then one can show that the value of the covariant derivative $nabla_XY$ at a point $p$ actually only depends on the value $X_p$ and $Y$ in a neighborhood of $p$. This allows for the $frac{D}{dt}$ to be well-defined.
– Matt
Nov 23 at 14:02












Thanks, I got it completely now @CharlieFrohman and Matt
– User12239
Nov 23 at 15:17




Thanks, I got it completely now @CharlieFrohman and Matt
– User12239
Nov 23 at 15:17















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