Lecture 3: Motion in two and three dimensions (chap 4 in Halliday)

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Lecture 3: Motion in two and three dimensions (chap 4 in Halliday)

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To increasing the dimension is straightforward. Just add more ... Projectile motion (????): a special case of two dimensional motion. Vertical and horizontal ... –

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Title: Lecture 3: Motion in two and three dimensions (chap 4 in Halliday)


1
Lecture 3 Motion in two and three dimensions
(chap 4 in Halliday)
To increasing the dimension is straightforward.
Just add more components on the vectors.
Position
Displacement
2
Similarly, average velocity and instantaneous
velocity are defined as
Or simply
where
Same for acceleration
3
Projectile motion (????) a special case of two
dimensional motion.
  1. Vertical and horizontal motion are independent.
  2. The horizontal motion has no acceleration, i.e.
    constant velocity.
  3. Vertical motion is simply a linear motion (free
    fall) with constant acceleration discussed in
    lecture 1.

4
  1. 3,2,1
  2. 1,2,3
  3. Same
  4. 6,5,4

5
The gravity doesnt affect the result.
6
Horizontal motion
Vertical motion
From the above, one has the equation of path
(trajectory)
x0 and y0 0
Horizontal range (R)
7
Horizontal
Vertical
8
  • vertical direction
  • horizontal direction

eliminate t
9
Uniform circular motion (????)
  • The magnitude v of the velocity does not change,
    but the direction changes continuously.
  • there is an acceleration

(?????)
  • a always pointing towards to the center of the
    circle.
  • the period is given by

10
The magnitude of v is
5s
Since v1-v2, means that it completes half
circumference from 2s to 5s, therefore
2s
Average acceleration
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