Let \begin{align*} V\colon \mathbb R & \to \mathbb R \\ x & \longmapsto V(x). \end{align*} and \begin{align*} w\colon \mathbb R^3 & \to \mathbb R \\ (a,b,c) & \longmapsto w(a,b,c). \end{align*} I thought that using the chain rule we have $\dfrac{dV(w)}{dw(a,b,c)} = \dfrac{dV}{da} \dfrac{\partial a}{\partial w} + \dfrac{dV}{db} \dfrac{\partial b}{\partial w}+ \dfrac{dV}{dc} \dfrac{\partial c}{\partial w}$?
Numerically, I am finding that $\dfrac{dV(w)}{dw(a,b,c)} = \dfrac{1}{3}\cdot\left(\dfrac{dV}{da} \dfrac{\partial a}{\partial w} + \dfrac{dV}{db} \dfrac{\partial b}{\partial w}+ \dfrac{dV}{dc} \dfrac{\partial c}{\partial w}\right)$.
Which is correct? Why do I need multiply by $\dfrac{1}{3}$?
Let $f:A\longrightarrow B$. We denote the Jacobian of $f$ at $x\in A$ by $J_f(x)$. The chain rule for the Jacobian is
$$J_{f\circ g}(x) = J_f\big(g(x)\big)\cdot J_g(x).$$
Applying this to your case we have
$$J_{V\circ w}(a,b,c) = J_V\big(w(a,b,c)\big)\cdot J_w(a,b,c).$$
Now, $V$ is a single variable function and hence $J_V\big(w(a,b,c)\big) = V'\big(w(a,b,c)\big)$, where $V'$ is the usual derivative.
On the other hand, $w:\mathbb R^3\longrightarrow \mathbb R$, so $J_w(a,b,c)$ is just the transpose of $\nabla w(a,b,c)$. Therefore:
$$J_{V\circ w}(a,b,c) = V'\big(w(a,b,c)\big)\cdot \left( \frac{\partial w}{\partial a}(a,b,c), \frac{\partial w}{\partial b}(a,b,c), \frac{\partial w}{\partial c}(a,b,c) \right)$$