Where capacitance come from?
Let's imagine a metal ball. And we want to charge it. What happens?
Our charge will be acted upon by an electric force directed in the opposite direction to its movement. This means that we will be forced to counteract this force, that is, to do work, to expend energy.
What else will we notice? That each subsequent charge that we transfer to the ball will require more and more energy from us.
Also, if we repeat this experiment with a larger metal ball, we will notice that it is easier to charge (it takes less energy to charge to the same value).
It turns out that the energy we spend on charging depends on the magnitude of the charge on our metal ball. That is, we have some kind of functional relationship between the charge on a metal ball and the voltage (the energy that must be applied to transfer a unit charge).
$$ Q = f(U) $$
This functional relationship is unique for each capacitor. However, for most capacitors, this relationship is linear. Therefore, we can introduce the capacitance as:
$$ Q = CU \Rightarrow C = \frac{Q}{U} $$
However, there are nonlinear capacitors for which this functional dependence is nonlinear. In such cases, we cannot speak of capacitance. Similarly, as for nonlinear resistors, we cannot speak of their resistance. However, as for nonlinear resistors, a differential capacitance is introduced at a particular operating point.
$$ C = \frac{dQ}{dU} $$
The conclusion is that the capacitance of a capacitor is not like the capacitance of, for example, a water bottle. It is like the resistance to charge. A larger capacitance means a smaller resistance to charge. It's just that the resistance is already taken, we are using it for a different physical phenomenon, so we use a different word here.