In kinematics, the multivariate chain rule is very useful. Especially in deriving accelerations from velocities.
Consider the position of a particle attached to a pendulum riding on a cart. The cart position $x$ and the pendulum angle $\theta$ (as well as the constant $\ell$) describe the position of the particle as follows:
$$ \vec{\rm pos}(x,\theta) = \pmatrix{x+\ell \sin \theta \\ -\ell\cos \theta \\ 0} $$
To find the velocity at any time using the chain rule
$$ \begin{aligned}
\vec{\rm vel}(x,\theta,\dot{x},\dot{\theta}) & = \left( \frac{\partial}{\partial x} \vec{\rm pos}(x,\theta) \right) \dot{x} + \left( \frac{\partial}{\partial \theta} \vec{\rm pos}(x,\theta) \right) \dot{\theta} \\
& = \pmatrix{1\\0\\0} \dot{x} + \pmatrix{\ell \cos \theta \\ \ell \sin \theta \\ 0} \dot{\theta} = \pmatrix{\dot{x} + \dot{\theta} (\ell \cos \theta) \\ \dot{\theta} (\ell \sin \theta) \\ 0}
\end{aligned} $$
and again the find the accelleration
$$ \begin{aligned}
\vec{\rm acc}(x,\theta,\dot{x},\dot{\theta},\ddot{x},\ddot{\theta}) & = \left( \frac{\partial}{\partial x} \vec{\rm vel}(x,\theta,\dot{x},\dot{\theta}) \right) \dot{x} + \left( \frac{\partial}{\partial \theta} \vec{\rm vel}(x,\theta,\dot{x},\dot{\theta}) \right) \dot{\theta} + \\ & + \left( \frac{\partial}{\partial \dot{x}} \vec{\rm vel}(x,\theta,\dot{x},\dot{\theta}) \right) \ddot{x} + \left( \frac{\partial}{\partial \dot{\theta}} \vec{\rm vel}(x,\theta,\dot{x},\dot{\theta}) \right) \ddot{\theta} \\
& = \pmatrix{0\\0\\0} \dot{x} + \pmatrix{-\dot{\theta} \ell \sin \theta \\ \dot{\theta} \ell \cos \theta \\ 0} \dot{\theta} + \pmatrix{1\\0\\0} \ddot{x} + \pmatrix{\ell \cos \theta \\ \ell \sin \theta \\ 0} \ddot{\theta} \\
& = \pmatrix{\ddot{x} + \ddot{\theta} \ell \cos \theta - \dot{\theta}^2 \ell \sin \theta \\ \ddot{\theta} \ell \sin \theta + \dot{\theta}^2 \ell \cos \theta \\ 0 }
\end{aligned} $$
And you have introduced the students to the wonderful world of dynamics (kinematics actually here) by application of calculus.
Any particle constrained to some motion with one or more parameters will do here, even as simple as circular motion as the acceleration will always feature a partial derivative to position and a partial to velocity.