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Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

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Page 1: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 2: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

1

Page 3: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 4: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 5: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 6: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 7: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 8: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 9: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 10: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 11: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Course Review

Physics 3210Spring Semester 2019

Page 12: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

● Today: Course Review● Tomorrow: Final discussion session

(space-time diagrams)● By Tuesday 23rd: Take practice final!

● We’ll review answers in class

● Thursday 25th: Final Exam

Page 13: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Final Exam Details

● When: Thursday April 25th, 1:00-3:00 PM.● Where: JFB B1... here!● Allowed materials:

● Equation sheet● Pen/pencil(s)● Hand held calculator. Not the one on your phone. ● Straightedge to make neat diagrams

Page 14: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

More Details

● Coverage: All Units

● Types of problems: Short answer and workout.● Study recommendations:

● Review homework● Review prior exams and practice exams● Exercises from lectures and discussion (online)● Alles leben ist problemlösen...

Page 15: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Final Exam Topics● Section 1

● Vectors

● Kinematics (incl polar coordinates)

● Newton's Laws

● Friction and Springs

● Harmonic Oscillator

● Section 2

● Work-energy theorem

● Energy conservation, conservative forces

● Center-of-Mass, Momentum Conservation

● Lagrangian Mechanics

● Rotational Dynamics

● Section 3

● Angular Momentum Vector

● Fictitious Forces

● Central Forces, Planetary Motion

● Damped Oscillator

● Special Relativity

Not yet covered in exam!!!

Page 16: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

2D Kinematics: Projectile Motion

● Independent horizontal and vertical motion

● Horizontal: constant velocity

● Vertical: constant acceleration

Page 17: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 18: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Newton's Laws

1) An object subject to no net external force is at rest or moving at a constant velocity when viewed from an inertial reference frame.

2) a = Fnet

/m

3) For every action there is an equal and opposite reaction F

AB = -F

BA

Page 19: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 20: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Forces and Free-Body Diagrams

● FBD: Tool for generating equations

for dynamic systems

● Each object in the system is drawn isolated from all but the forces

acting on it.

b) what is the acceleration (magnitude and direction) of m

2?

c) what is the amount by which the spring is stretched from equilibrium?

Page 21: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Simple Pendulum/Harmonic Motion

The simple pendulum shown - consisting of a massless string of length L = 1.0 m and a bob of mass 0.1 kg - is given an initial velocity v

0 = 3.0 m/s to the right,

at an initial displacement q0 = 0. Find:

The position of the pendulum at t = 8 seconds.

The tension in the string at t = 8 seconds.

q

Mass m

Length L

Page 22: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 23: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Final Exam Topics● Section 1

● Vectors

● Kinematics (incl polar coordinates)

● Newton's Laws

● Friction and Springs

● Harmonic Oscillator

● Section 2

● Work-energy theorem

● Energy conservation, conservative forces

● Center-of-Mass, Momentum Conservation

● Lagrangian Mechanics

● Rotational Dynamics

● Section 3

● Angular Momentum Vector

● Fictitious Forces

● Central Forces, Planetary Motion

● Damped Oscillator

● Special Relativity

Not yet covered in exam!!!

Page 24: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Work-Kinetic Energy Theorem

The net work done on a body is equal to the change in kinetic energy of the body

Formal definition of work(“Force times distance” generalized)

Formal definition of kinetic energy

Page 25: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 26: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 27: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Generalize mechanical energy conservation to conservative systems including springs:

Spring P.E. K.E.

Gravitational P.E.

Page 28: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Work-Energy Theorem

b) If the force f is such that the block will move with constant speed v = 0.1 m/s down the ramp, calculate the work done by the force F if the block travels the length of the ramp.c) Suppose that, while traveling at v = 0.1 m/s down the ramp, at d = 3 meters from the end of the ramp the rope breaks. Use the work-kinetic energy theorem to calculate the speed of the crate when it reaches the bottom of the ramp.

Page 29: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Lagrangian Mechanics

Basic program:

L = T – V

Apply Euler-

Lagrange eqns

Page 30: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

You will be given I for basic shapes.

Page 31: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Spring PE

RotationalKE

GravitationalPE

TranslationalKE

I = S mir

i

2

= “moment of inertia”

Page 32: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Rotational Dynamics

Page 33: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Similarity to 1D motion

Mechanics Lecture 15, Slide 33

Page 34: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 35: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Final Exam Topics● Section 1

● Vectors

● Kinematics (incl polar coordinates)

● Newton's Laws

● Friction and Springs

● Harmonic Oscillator

● Section 2

● Work-energy theorem

● Energy conservation, conservative forces

● Center-of-Mass, Momentum Conservation

● Lagrangian Mechanics

● Rotational Dynamics

● Section 3

● Angular Momentum Vector

● Fictitious Forces

● Central Forces, Planetary Motion

● Damped Oscillator

● Special Relativity

Not yet covered in exam!!!

Page 36: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics
Page 37: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Fictitious Forces

Page 38: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

(b) If Annie walks to the center of the carousel (and Bob stays where he is), what is the final rate of spin of the carousel?

(c) What is the direction of the Coriolis force on Annie as she walks?

(d) What is the direction fo the azimuthal force on Bob as Annie walks?

Page 39: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Potentials, Central Forces

● For conservative forces, the force is the spatial derivative of a potential function.

● e.g. F(x) = - dU(x)/dr

● Orbital motion may be described by an effective potential

● Ueff

= L2/2mr2 + U(r)

Page 40: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Special Relativity

● Origins● Michelson-Morley expt● What problem did SR solve?

● The invariant interval● ds2 = -c2dt2 + dx2

● Time dilation and length contraction

● Expect: Workout with space-time diagram.

Page 41: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Special Relativity

● Origins● Michelson-Morley expt● What problem did SR solve?

● The invariant interval● ds2 = -c2dt2 + dx2

● Time dilation and length contraction

● Expect: Workout with space-time diagram.

Page 42: Welcome to Physics 211!belz/phys3210/final_rev.pdf · Section 2 Work-energy theorem Energy conservation, conservative forces Center-of-Mass, Momentum Conservation Lagrangian Mechanics

Final Exam Topics● Section 1

● Vectors

● Kinematics (incl polar coordinates)

● Newton's Laws

● Friction and Springs

● Harmonic Oscillator

● Section 2

● Work-energy theorem

● Energy conservation, conservative forces

● Center-of-Mass, Momentum Conservation

● Lagrangian Mechanics

● Rotational Dynamics

● Section 3

● Angular Momentum Vector

● Fictitious Forces

● Central Forces, Planetary Motion

● Damped Oscillator

● Special Relativity

Not yet covered in exam!!!