Motion in Our Daily Llves


Centripetal Centrifugal Forces„ continued


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Centripetal Centrifugal Forces„ continued


UCSD
Physics 10
  • The car is accelerated toward the center ofthe curve by a centripetal (center seeking) force
  • 1n your reference frame of tbe car, you experience a ''fake'', or fictitious centrifuga1l'oroe""

  • - Nota real force, just inertia relative to car's acceleration

Centripetal Force
on car
velocity of car
(and the way you'd rather go)
Spring 2008
lO
UCSD
Physics 10
Pictorial ''Derivation'' of Centripetal Acceleration
a=!lv/D,.t
Top view:
a
a
a
a
\
a = v2/r (r is radius of curve)
In uniform circular motion the acceleration is constant, directed towards the center. The velocity
has constant magnitude, and is tangent to the path.

Rotating Drum Ride


UCSD
Physics 10
  • Vertical c1rum rotates, you,re pressed against wall

Real Forces:
F iction; up Centripetal; inwards Gravity (weight); down
Perceived Forces:
Centrifugal; outwards Gravity (weight); down
Perceived weight; down and out
::::=-

Works in vertical clirection too......


UCSD
Physics 10
  • Roller coaster loops:
    • Loop accelerates you downward (at top) with acceleration greater than gravity
    • You are "pulled" into the floor, train stays on track
      • it's actually the train being pulled into you!

Spring 2008
l3

Sustained vertical spinning


UCSD
Physics 10
  • Ever wonder what a bike tire feels like?
  • At constant speed, the centripetal acceleration is constant (v2/r), but the direction of gravity keeps changing!
  • Feel heavier at bottom than attop
  • This ride definitely turns your world around!

Spring 2008
14
UCSD
Physics 10
swing ropes: whar you fcel from your seat
gravity (mg)
Old-Fashioned Swings
- y- - /tie
1 . 1
/ resu tant: centnpeta
///
  • The angle of the ropes tells us

  • where the forces are:
  • Ropes and gravity pull on

  • sw1• ngers
  • If no vertical motions (Ievel swing), vertical forces cancel
  • Only thing left is horizontal component pointing toward center: centripetal force
  • Centripetal force is just mvllr

  • (F = m.a,· a = vllr)

Spring 2008
l5

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