A Jacobi field $J$ with initial conditions $J(0)=0$ and $J‘(0)=w$ along the geodesic $\gamma(t)=exp_p(tv)$ can explicitly be written as
\begin{equation}
J(t)=(d exp_p)_{tv}(tw).
\end{equation}
For small enough $t$ the differential of the exponential map at $tv$ is bijective. So for any $\nu \in T_{\gamma(t)}M$ there is some $u \in T_pM$ with
\begin{equation}
(d exp_p)_{tv}(u)=\nu.
\end{equation}
Then the Jacobi field with initial condition $J(0)=0$ and $J‘(0)=\frac{u}{t}$ is the one you‘re looking for.
A Jacobi field $J$ with initial conditions $J(0)=0$ and $J‘(0)=w$ along the geodesic $\gamma(t)=exp_p(tv)$ can explicitly be written as \begin{equation} J(t)=(d exp_p)_{tv}(tw). \end{equation} For small enough $t$ the differential of the exponential map at $tv$ is bijective. So for any $\nu \in T_{\gamma(t)}M$ there is some $u \in T_pM$ with \begin{equation} (d exp_p)_{tv}(u)=\nu. \end{equation} Then the Jacobi field with initial condition $J(0)=0$ and $J‘(0)=\frac{u}{t}$ is the one you‘re looking for.