Fellows,
I have been wondering about calculus on manifolds. We know, gradient vector $\mbox{grad}(\phi)$ on flat $\mathbb{R}^n$ space is basically the partial derivative respective to each variable, right!? Let me ask about submanifolds: I have a potential map $\phi$ defined everywhere on manifold $(g, \mathcal{M})$. A submanifold $(h, \mathcal{S})$ has its tangent field $T_p \mathcal{S} \subseteq T_p \mathcal{M}$ on point $p \in \mathcal{S} \subseteq \mathcal{M}$. I have not enough knowledge to understand how to calculate the entries of such vector. I think, it might be easier if manifold $\mathcal{M}$ is rather n real space $\mathbb{R}^n$, which makes metric $g_{ij}$ equal to Dirac entries $\delta_{ij}$.
Let me add an example: we have a classic potential gravitational map defined on attached coordinate frame $\frac{\alpha}{r^2}$, such that constant $\alpha \in \mathbb{R}_+$ corresponds to quantity $GM$, the gravitational constant $G$ and planet mass $M$. It has the formula $\frac{\alpha}{x^2+y^2+z^2}$ in cartesian coordinates. At other hand, we have planet surface $\mathcal{S}$ defined by chart map $\varphi$ given by formula $\rho(\theta, \lambda) \begin{bmatrix} \sin{\lambda} \cos{\theta} \\ \sin{\lambda} \sin{\theta} \\ \cos{\lambda} \end{bmatrix}$. In this case, what would be the gradient $\mbox{grad}_{\mathcal{S}}\phi$ at point $p = \varphi(u, v)$? It is clear: the potential quantity at point $p$ is $\frac{\alpha}{\rho(u, v)^2}$, but is $\mbox{grad}_p \mathcal{S}$ given by vector below?
$$ -2 \, \frac{\alpha}{\rho(u, v)^3} \, \left(\frac{\partial \rho}{\partial u} \, X_u + \frac{\partial \rho}{\partial v} \, X_v \right) $$