Covariant derivative of a tensor field

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Let $F$ be a tensor field of type $(0,2)$ on a Riemannian manifold (like a Riemannian metric). Let $\gamma$ be a geodesic on $M$ and let $e(t)$ be a parallel transport along $\gamma$. I want to find a formula for $\frac{d}{dt} F_{\gamma(t)}(e(t),\gamma'(t))$. How can I derivate this quantity. I understand calculcations when $F$ is the Riemanian metric (this is zero using compatibility between the metric and Levi Civita connection). But I don't see how to do for general $F$. Thanks in advance for your help.

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I'm not sure I understand precisely what you want, but the covariant derivative of $F$ along $\gamma$ is given by

$$ \frac{DF}{dt}(e(t),\dot{\gamma}(t)) = \frac{d}{dt} F(e(t),\dot{\gamma}(t)) - F \left( \frac{De}{dt}(t), \dot{\gamma}(t) \right) - F \left( e(t), \frac{D \dot{\gamma}}{dt}(t) \right) = \frac{d}{dt} F(e(t),\dot{\gamma}(t)) $$

since $e(t), \dot{\gamma}(t)$ are parallel along $\gamma$. The expression $F(e(t),\dot{\gamma}(t))$ is a scalar depending on $t$ so you can differentiate it just like you differentiate a regular function. If $e_i(t)$ is a frame alone $\gamma$ and you expand

$$ e(t) = a^i(t) e_i(t), \,\, \dot{\gamma}(t) = \gamma^i(t)e_i(t), \,\, F(e_i(t),e_j(t)) = f_{ij}(t)$$

then

$$ F(e(t), \dot{\gamma}(t)) = F(a^i(t)e_i(t), \gamma^j(t)e_j(t)) = a^i(t)\gamma^j(t) f_{ij}(t) $$

and so

$$ \frac{d}{dt} F(e(t), \dot{\gamma}(t)) = \dot{a}^{i}(t)\gamma^j(t)f_{ij}(t) + a^i(t)\dot{\gamma}^j(t)f_{ij}(t) + a^i(t)\gamma^j(t)\dot{f_{ij}}(t).$$