Opus_723 said:
I just started working through Halliday and Resnick, and I'm going through the kinematic equations for constant acceleration. I don't need help with the work, but I noticed that the book never addresses non-constant acceleration. I was expecting more Calculus in this book (the kinematic equations were derived using algebra), and was wondering where I could find learning material for kinematics with non-constant acceleration. I also wanted to know if I got the right book? I see bits of Calculus throughout, but I'm worried that the majority of the book will deal with special cases and assumptions like the constant acceleration in this chapter. It seems kind of useless to keep looking at special cases like that.
It all comes from the definitions of position and velocity:
a = dv/dt and v = dx/dt. It's more useful to write in differential form:
dv = adt
dx = vdt
For constant acceleration you can integrate the first equation to get:
v = at + const.
Plugging in t = 0 gives you the constant vo.
v = vo + at.
You can then plug this into the dx equation and integrate to get:
x = vot + 1/2 at^2 + const. (The constant is x0.)
You follow the same procedure for non-constant acceleration. If a is a function of time you simply integrate. If a is a function of x you can use the chain rule and integrate.
a(x) = dv/dt = dv/dx dx/dt = dv/dx v
Writing in differential form,
a(x) dx = v dv
or 1/2 v^2 = Int (a(x) dx)
Assuming you can integrate the function, you can find a relation for v as a function of x. You can then integrate v to find x as a function of time. Another important case is when the acceleration is a function of v.
a(v) = dv/dt -> dt = dv/a(v)
If you integrate, you will have time as a function of velocity. You may or may not be able to solve for v as a function of t.
Surprisingly, it's hard to find an introductory physics book that really uses calculus from the beginning. HRK is pretty good overall. I like their style and they covers a lot of material.
(Sorry I don't know how to make nice equations.)