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Class 4: Constant acceleration motion Review d d dt dt a (m/s 2 - - PowerPoint PPT Presentation
Class 4: Constant acceleration motion Review d d dt dt a (m/s 2 - - PowerPoint PPT Presentation
Class 4: Constant acceleration motion Review d d dt dt a (m/s 2 ) x (m) v (m/s) dt dt v t graph v x (velocity) t (time) t 1 t 2 t 3 Grey area (with sign) = x 2 -x 1 dv x a slope of curve x dt t 2
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v‐t graph
vx (velocity) t (time) t3 t2 t1
curve
- f
slope dt dv a
x x
curve under Area dt v x x x
x t t 1 2
2 1
Grey area (with sign) = x2-x1
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Instantaneous acceleration (1D)
dt dv t v Lim
- n
accelerati Average Lim a
t t x
Instantaneous acceleration
In mechanics, only instantaneous acceleration is important. Average acceleration is just introduced to define its instantaneous values. So from now
- n, by acceleration, we mean instantaneous acceleration.
dt x d dt dx dt d dt dv a
2 x
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Constant acceleration motion (1D)
ax = constant
t a 2 1 t v x x t a v v
2 x i x i f x i x f x
These two equations are enough to solve any problem of this type. Five variables are involved: xf‐xi (=x), vf, vi, a, and t. So we can afford to solve for two variables as unknown with these two equations.
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Free falling is a constant acceleration motion (1D)
ay = constant = 9.8 m/s2 for any object
t a 2 1 t v y y t a v v
2 y i y i f y i y f y
` g
g = 9.8 m/s2
g g
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