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Circular Motion Uniform and Non-Uniform
22

Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Jan 03, 2016

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Roxanne Adams
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Page 1: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Circular MotionUniform and Non-Uniform

Page 2: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

ReviewEquations for Motion Along One

Dimension

dt

dx

t

xv

t

xv

t

ave

0lim

dt

dv

t

va

t

va

t

ave

0lim

Page 3: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

ReviewMotion Equations for Constant

Acceleration

•1.

•2.

•3.

•4.

atvv 0

221

00 attvxx

20vv

vave

xavv 220

2

Page 4: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

ReviewAcceleration in Uniform Circular

Motion

Velocity is always tangent to the pathAcceleration is always perpendicular

to velocityAcceleration is center seeking

(Centripetal)

R

va

2

Page 5: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Review3 Laws of MotionIf in Equilibrium

If not in equilibriumChange in Motion is Due to Force

Force causes a change in acceleration!

0F

maF

Page 6: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Acceleration on a Curve

0t

0v

2t

2v

0a

r

va

2

2a

Page 7: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Acceleration on a Curve

0t

0v

2t

2v

0a

Car is always accelerating

There must be a force acting on the car!

r

va

2

Page 8: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Force on a Curve

Centripetal Force

0t

0v

2t

2v

0a

r

va

amF2

r

vmF

2

0F

Page 9: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Note: On Centrifugal ForceThere is no such thing as

centrifugal forceIt is merely the action reaction

pair of centripetal force.

Page 10: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Centrifugal Force

Centrifugal force you feel in a turning car is just a result of your inertia trying to maintain a straight line of motion.

Page 11: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Example: Car on a curveA 1,500 kg car is rounding a

curve with radius 35.0 m. If the coefficient of friction is 0.500 find the maximum speed the car can have without slipping.

Page 12: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Example: Car on a curveMax velocity is related to max

acceleration is related to Centripetal force

No slipping means Centripetal Force= Force of

frictionr

vmF

2

Nf

Page 13: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Example: Car on a curve

smv

v

grv

m

mgrv

mgr

vm

Nr

vm

1.13

)80.9)(500.0)(0.35(

2

2

2

Page 14: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Example: Car on a banked curveA civil engineer wishes to design

a curved ramp in such a way that a car will not have to rely on friction to round the curve without skidding (in case of rain or ice). This is done by banking the curve (tilted towards one side). If the speed of the ramp is supposed to be 13.4 m/s, and the radius is 50.0m at what angle should the curve be banked?

Page 15: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Example: Car on a banked curve

Page 16: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Example: Car on a banked curve

r

vmNF

2

sin

cos

cos

mgN

mgN

Page 17: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Example: Car on a banked curve

1.20)50)(8.9(

4.13tantan

tan

tan

tan

21

21

2

2

2

gr

v

gr

v

r

vg

r

vmmg

Page 18: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Giancoli 5-22A 1200 kg car rounds a curve of

radius 67m banked at 12o. If the car is travelling at 95 kph will a friction force be required? If so, how much and in what direction?

Page 19: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Vertical Uniform Circular Motion

A passenger on a Ferris wheel weighs 750N. The wheel has a radius of 100 m and moves at constant speed of 10.5m/s. Find the apparent weight of the passenger at the top and at the bottom of the wheel.

Page 20: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Vertical Uniform Circular Motion

At top At BottommaF

)(2

2

2

r

vgmN

r

vmmgN

r

vmwNF

)(2

2

2

r

vgmN

r

vmmgN

r

vmwNF

Page 21: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Non- Uniform Circular MotionRadial acceleration – causes

change in directionTangential acceleration – causes

change in speed

Page 22: Circular Motion Uniform and Non-Uniform. Review Equations for Motion Along One Dimension.

Artificial Gravity