Interestingly, it is not only rotating rigid objects that have angular momentum. Any object with translational momentum also has angular momentum, as long as it is moving perpendicular to some axis!
One especially critical feature of angular momentum (along with many other angular quantities) for a point particle is that it depends on your choice of axis. Interestingly, the angular momentum of a rotating rigid object does not depend on your choice of axis (because it is actually rotating around a fixed axis!).
Suppose a friend of yours wrote down the following equation for something they call the “total momentum”: \(\vec{p} + \vec{L}\text{.}\) How could you convince your friend that this equation is incorrect, and that there cannot be such a thing as total momentum?