Download Radial (Centripetal) Acceleration – ar or ac

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Woodward effect wikipedia , lookup

Lorentz force wikipedia , lookup

Torque wikipedia , lookup

Gravity wikipedia , lookup

Free fall wikipedia , lookup

Inertia wikipedia , lookup

Mechanics of planar particle motion wikipedia , lookup

Centrifugal force wikipedia , lookup

Coriolis force wikipedia , lookup

Pioneer anomaly wikipedia , lookup

Relativistic angular momentum wikipedia , lookup

Modified Newtonian dynamics wikipedia , lookup

Artificial gravity wikipedia , lookup

Weightlessness wikipedia , lookup

Fictitious force wikipedia , lookup

G-force wikipedia , lookup

Centripetal force wikipedia , lookup

Transcript
Radial (Centripetal) Acceleration – ar or ac
I. Uniform Circular Motion
‘uniform’ means ‘constant’ - In this case, it refers to constant speed (v) or constant
angular speed (  , omega). A particle moves in circular motion with constant speed.
dv
Recall that in one dimension, (linear) acceleration was defined by: a  . In two
dt
dimensions, this linear acceleration is called ‘tangential acceleration’ and denoted by ‘a t’
or ‘a||’ (parallel symbol because the tangential acceleration vector is parallel to the
tangential velocity vector). Since the derivative of a constant is zero, at = 0 m/s2.
d
Recall that for circular motion, angular acceleration was defined by:  
. This
dt
 (alpha) was called ‘angular acceleration’ and since angular speed  is constant and the
derivative of a constant is zero,  = 0 rad/s2.
Furthermore, since at = R , uniform circular motion means both tangential
acceleration and angular acceleration are zero.
II. Centripetal (Radial) Acceleration
‘ac’ or ‘ar’ or ‘ a ’ - perpendicular symbol because the centripetal acceleration
vector points perpendicular to the velocity vector (and inward toward the circle’s center).
So if speed is not changing, how can there be any kind of nonzero ‘acceleration’?
Speed is not changing, true, but the direction of the velocity vector is changing. The
centripetal force (Fc) causing this change should be thought of as a ‘turning force’, a force
‘radially inward’. Centripetal (inward) force is not to be confused with the ‘fictitious’
centrifugal (outward) force.
v2
v2
III. Centripetal Acceleration Magnitude – ac 
(What’s going on here?)
or aR 
R
R
Centripetal acceleration direction is radially inward toward the center of the circle.
(1) Notice the similar isosceles triangles.
(2) Using sides (magnitudes), vi
vi
r
v r
vf
we get


v
r
vf
v
ri
(3) Recall:
ri
rf
v

rf
a

t
v v r
=
 
t r t
v dv
r
(4) lim

 a and lim
v
t 0 t
t 0 t
dt
v2
v r
(5) So a = lim 
 ac or ac 
t 0 r t
r