| Week of | Aug 22 | Sep 5 | Oct 1 | Nov 5
| Phy 205 page |
| Aug 27 | Sep 10 | Oct 8 | Nov 12 | ||
| Sep 17 | Oct 15 | Nov 19 | |||
| Sep 24 | Oct 22 | Nov 26 | |||
| Oct 29 | Notes for Fall, 2000 |
5 Sep Velocity again. Re-write the previous development in terms of functional notation, x(t). Emphasize that this notation can be a little confusing, as it meant "x of t" not "x times t".
t2 - t1 = Δt. To find the velocity AT a point still requires that you take these average values and let the time interval approach zero.
For an example take a function x( t ) = A + Bt + Ct2. Then
Put this into the definition of average velocity and simplify. The result is
As the time interval approaches zero, this approaches B + 2 C t.
The acceleration of a car is sometimes expressed in terms of the amount of time it takes to go from zero to 60 mi/hr. This becomes a quantitative measure by taking the quotient:
To see how this compares to other accelerations I did some unit conversion to put this into a more standard form.
7 Sep
Go over a couple of homework problems in some detail.
Velocity and acceleration in still more detail. The only two basic
equations in chapter 2 of Young and Freedman are the equations (2-3) and
(2-5). These are the definitions of velocity (in one dimension) and
acceleration (in one dimension).
|
|
As a matter of notation, I am using vx for the velocity along the x-axis even though Young simply uses "v." The reason that I'm using the more extended notation is that in chapter 3 that's the notation that Young will use anyway. Why change? I went over the conceptual questions of signs that occur in the velocity and acceleration equation in the special case of falling under gravity. The sign for ax wasn't all that obvious.