Understanding Covariant Derivatives Along a Curve

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SUMMARY

The discussion focuses on the concept of covariant derivatives along a curve, specifically the equation D_t V(t) = \nabla_{\dot{\gamma}(t)} W. Here, V represents a vector field along the curve γ, while W is an extension of V. The left-hand side, D_t V, denotes the covariant derivative at time t, yielding a tangent vector at γ(t). The right-hand side, involving the connection ∇ and the tangent vector \dot{γ}(t), raises questions about whether it can be expressed as (\nabla_X W)(γ(t)), where X is any vector field satisfying X(γ(t)) = \dot{γ}(t).

PREREQUISITES
  • Understanding of vector fields and their properties
  • Familiarity with the concept of connections in differential geometry
  • Knowledge of covariant derivatives and their applications
  • Basic grasp of curves and tangent vectors in manifold theory
NEXT STEPS
  • Study the properties of connections in differential geometry
  • Learn about the absolute derivative as discussed in Fecko's work
  • Explore the relationship between vector fields and tangent vectors along curves
  • Investigate applications of covariant derivatives in physics and engineering
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Mathematicians, physicists, and students of differential geometry who are looking to deepen their understanding of covariant derivatives and their implications in the study of curves and connections.

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I'm teaching myself about connections and came across something I am not completely sure about. The text I am using defines a connection as taking in two vector fields and outputting a vector field. However, later when discussing covariant derivatives along a curve I see this equation:

<br /> D_t V(t) = \nabla_{\dot{\gamma}(t)} W,<br />

where V is a vector field along the curve \gamma, W is an extension field of V, \nabla is the connection and D_t takes in a vector field along \gamma and gives a vector field along \gamma.

I understand that the left hand side is the value of the vector field D_t V at time t (a tangent vector at \gamma(t)). However, the right hand side is confusing me since \dot{\gamma}(t) is a tangent vector at \gamma(t) and not a vector field. Since the value of a covariant derivative at a point p depends only on the value at p of the vector field we are differentiating along, is the right hand side the same as (\nabla_X W) (\gamma(t)) where X is any vector field such that X(\gamma(t)) = \dot{\gamma}(t)?

Thanks.
 
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