PHYSICS 231 INTRODUCTORY PHYSICS I

27
PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 10

description

PHYSICS 231 INTRODUCTORY PHYSICS I. Lecture 10. Last Lecture. Elastic Collisions: Multi-part Collision Problems (conserve E or p) Angular motion. Angular Speed. Can also be given in Revolutions/s Degrees/s. (in rad/s). Linear (tangential) Speed at r. (  in rad/s). Example 7.2. - PowerPoint PPT Presentation

Transcript of PHYSICS 231 INTRODUCTORY PHYSICS I

Page 1: PHYSICS 231 INTRODUCTORY PHYSICS I

PHYSICS 231

INTRODUCTORY PHYSICS I

Lecture 10

Page 2: PHYSICS 231 INTRODUCTORY PHYSICS I

• Elastic Collisions:

• Multi-part Collision Problems (conserve E or

p)

• Angular motion

Last Lecture

m1v1i + m2v2i = m1v1 f + m2v2 f

v1i − v2i = − v1 f − v2 f( )

s = rθ (θ in radians)

Page 3: PHYSICS 231 INTRODUCTORY PHYSICS I

Angular Speed

• Can also be given in • Revolutions/s• Degrees/s

• Linear (tangential) Speed at r

v t = ΔsΔt

= rΔθΔt

v t = rω

ω =ΔθΔt

=θ f −θ i

t f − ti

(ω in rad/s)

(in rad/s)

Page 4: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.2

A race car engine can turn at a maximum rate of 12,000 rpm. (revolutions per minute).

a) What is the angular velocity in radians per second.

b) If helicopter blades were attached to the crankshaft while it turns with this angular velocity, what is the maximum radius of a blade such that the speed of the blade tips stays below the speed of sound. DATA: The speed of sound is 343 m/sa) 1256 rad/s

b) 27 cm

Page 5: PHYSICS 231 INTRODUCTORY PHYSICS I

Angular Acceleration

• Denoted by

• ω in rad/s• rad/s²• Every point on rigid object has same

ω and

=ω f − ωi

t

Page 6: PHYSICS 231 INTRODUCTORY PHYSICS I

Rotational/Linear Correspondence:

Δθ ↔ Δxω0 ↔ v0

ω f ↔ v f

α ↔ at ↔ t

Page 7: PHYSICS 231 INTRODUCTORY PHYSICS I

Rotational/Linear Correspondence, cont’d

Rotational Motion Linear Motion

Δθ =ω0 + ω f( )

2t

Δθ =ω0t +12

α t2

ω f = ω0 + α t

ω f2

2=

ω02

2+ αΔθ

Δθ =ω f t −12

α t2

Δx =v0 + v f( )

2t

v f =v0 +t

Δx = v0t +12

at2

Δx = v f t −12

at2

v f2

2=v02

2+Δx

Constant

Constant a

Page 8: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.3A pottery wheel is accelerated uniformly from rest to a rotation speed of 10 rpm in 30 seconds. a.) What was the angular acceleration? (in rad/s2)

b.) How many revolutions did the wheel undergo during that time?a) 0.0349 rad/s2

b) 2.50 revolutions

Page 9: PHYSICS 231 INTRODUCTORY PHYSICS I

Linear movement of a rotating point

• Distance

• Speed

• Acceleration

Angles must be in radians!

Different points have different linear speeds!

at = rα€

v t = rω

Δs = rΔθ

Page 10: PHYSICS 231 INTRODUCTORY PHYSICS I

Special Case - Rolling

• Wheel (radius r) rolls without slipping• Angular motion of wheel gives linear motion of car

• Distance

• Speed

• Acceleration

x =rΔθ

v =rω

a =r

Page 11: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.4

A coin of radius 1.5 cm is initially rolling with a rotational speed of 3.0 radians per second, and comes to a rest after experiencing a slowing down of = 0.05 rad/s2.

a.) Over what angle (in radians) did the coin rotate?

b.) What linear distance did the coin move?

a) 90 radb) 135 cm

Page 12: PHYSICS 231 INTRODUCTORY PHYSICS I

Centripetal Acceleration

• Moving in circle at constant SPEED does not mean constant VELOCITY

• Centripetal acceleration results from CHANGING DIRECTION of the velocity

• Acceleration points toward center of circle

r a = Δ

r v

Δt

Page 13: PHYSICS 231 INTRODUCTORY PHYSICS I

• Similar triangles:

• Small times:

• Using or

Derivation: acent = ω2r = v2/r

a = v ΔθΔt

= vω

Δvv

= Δsr

aavg = ΔvΔt

= vr

ΔsΔt

Δs ≈ arc length = rΔθ

v = ωr

ω =v /r

acent = ω 2r =v2

r

Page 14: PHYSICS 231 INTRODUCTORY PHYSICS I

Forces Cause Centripetal Acceleration

• Newton’s Second Law

• Radial acceleration requires radial force• Examples of forces

• Spinning ball on a string• Gravity• Electric forces, e.g. atoms

rF =m r

Page 15: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.5a

a) Vector Ab) Vector Bc) Vector C

AB

CAn astronaut is in circular orbitaround the Earth.

Which vector might describe the astronaut’s velocity?

Page 16: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.5b

a) Vector Ab) Vector Bc) Vector C

AB

CAn astronaut is in circular orbitaround the Earth.

Which vector might describe the astronaut’s acceleration?

Page 17: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.5c

a) Vector Ab) Vector Bc) Vector C

AB

CAn astronaut is in circular orbitaround the Earth.

Which vector might describe the gravitational force acting on the astronaut?

Page 18: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.6a

a) Vector Ab) Vector Bc) Vector C

AB

C

Dale Earnhart drives 150 mph around a circular track at constant speed.

Neglecting air resistance, which vector best describes the frictionalforce exerted on the tires from contact with the pavement?

Page 19: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.6b

a) Vector Ab) Vector Bc) Vector C

Dale Earnhart drives 150 mph around a circular track at constant speed.

Which vector best describes the frictional force Dale Earnhart experiences from the seat?

AB

C

Page 20: PHYSICS 231 INTRODUCTORY PHYSICS I

Ball-on-String Demo

Page 21: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.7

A puck (m=.25 kg), sliding on a frictionless table, is attached to a string of length 0.5 m. The other end of the string is fixed to a point on the table and the puck is sent revolving around the fixed point. It take 2 seconds to make a complete revolution.

a) What is the acceleration of the puck?

b) What is the tension in the string?

a) 4.93 m/s2

b) 1.23 N

Page 22: PHYSICS 231 INTRODUCTORY PHYSICS I

DEMO: FLYING POKER CHIPS

Page 23: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.8

A race car speeds around a circular track.

a) If the coefficient of friction with the tires is 1.1, what is the maximum centripetal acceleration (in “g”s) that the race car can experience?

b) What is the minimum circumference of the track that would permit the race car to travel at 300 km/hr?

a) 1.1 “g”sb) 4.04 km (in real life curves are banked)

Page 24: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.9

A curve with a radius of curvature of 0.5 km on a highway is banked at an angle of 20. If the highway were frictionless, at what speed could a car drive without sliding off the road?

42.3 m/s = 94.5 mph

Page 25: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.11a

Which vector represents acceleration?

a) A b) E

c) F d) B

e) I

Page 26: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.11b

If car moves at "design" speed, which vector represents the force acting on car from contact with road

a) D b) E

c) G d) I

e) J

Page 27: PHYSICS 231 INTRODUCTORY PHYSICS I

Example 7.11c

If car moves slower than "design" speed, which vector represents frictional force acting on car from contact with road (neglect air resistance)

a) B b) C

c) E d) F

e) I