In order to understand the generalization of Newtonian mechanics to two and three dimensions, we first need to understand a new type of derivative called the partial derivative.
To motivate the discussion, let us use the chain rule to take the
ordinary derivative of
where
is some function
of
, say
:
| (9.20) |
Notice that the partial derivative is actually simpler to evaluate than an ordinary derivative, because only the explicit dependence of the function on the differentiating variable need be considered -- all other variables are taken to be constant.
David Raymond 2006-04-07