Physics 131 Lecture Notes

Ohio State University Marion Campus

by Gordon Aubrecht

©copyright 1998-2003 all rights reserved

These notes sketch the topics that will be the focus of each class. You may use them to refresh your mind, and to help you structure your "lecture" notes.



Class 1

Introduction--describe Physics 131

How the days are structured; what is expected.

Grading policy explained (syllabus on paper & web)

"Gordon's forgiveness policy"

Choice for exams:

a) Small number of questions, if you miss one it can cause a big problem with your grade but mean grade is higher.

b) Large number of questions; but then low midterm and final mean grades.


Introduction to the Physical World

The particle model and other models used in physics--utility, limitations.

What is science?

Experiment as the bellwether.

What is physics? Excitement!

What are physics's limits?



Class 2

Newton's First Law:

A particle's motion will not change unless an unbalanced force acts on it.

Unbalanced forces result in a change in the motion.

Forces all act on one body.

the newton

contact vs. noncontact forces

Examples of forces in everyday life.

Simplification of the world:



Class 3

Forces in Nature

Electromagnetic plus weak becomes electroweak.

Electroweak plus strong becomes GUT (grand unified theory).

GUT plus gravitation becomes supersymmetry? the theory of everything? ??

force vs. impulse

vectors vs. scalars

weight--a vector force

surfaces exert forces on objects or bodies that touch them

free body diagrams (FBDs) and point masses



Class 4

Vectors

trigonometry

components

reference frame/coordinate system

addition

subtraction

length

meaning

Compare two and three dimensions to one dimension



Class 5

Equilibrium and Newton's Third Law

Newton's Third Law:

If body A exerts a force on body B, then body B exerts a force on body A equal in magnitude and opposite in direction.

Do Newton's Third Law examples and problems

Pairs act on different bodies.

Equilibrium:

The sum of the forces acting on a body is zero.

This is a vector relation.

Do examples.


Free Body Diagrams in detail

The force diagram compared to the free body diagram.

Identify THE body.

DRAW THE DIAGRAM!

Note that Newton's Third Law refers to two different bodies: If A exerts a force on B, B exerts an equal and oppositely directed force on A.

Do examples showing how these ideas are used.

Ropes transmit forces.



Class 6

Inertia--Operational Definition of mass

What does mass do?


Friction

static (no motion) friction: the force of static friction is just such that no motion occurs up until some maximum force is attained.

kinetic friction: bodies are moving relative to one another

Model: find force with which surfaces push together; then the frictional force is proportional to that force. The constant of proportionality is called the coefficient of kinetic friction.

The "normal" force; inclined planes

Show how to work problems--putting it all together.



Class 7

Newton's Second Law

Acceleration measures the change in motion of the object.

Newton's Seccond Law: F = ma

do examples of how to use Newton's Second Law

Weight is a force

W = mg



Class 8

Coordinate systems and their consequences

What is a coordinate system?

Components.

Distance: s

Displacement: r


Motion means change.

Intuition about speed.

What (average) speed is.

vaverage = (change in s)/(time interval involved)

The difference between speed and velocity (v and v).

vaverage = (change in r)/(time interval involved) [speed and velocity]

Instantaneous speed and velocity compared to average speed and velocity.

The m/s, the km/h.



Class 9

Defining acceleration

Acceleration means any of: increasing speed in the direction of motion, decreasing speed in the direction of motion, changing the direction of motion.

aaverage = (change in v)/(time interval involved) [acceleration]

Using average acceleration to solve for v(t); v(t) = v0 = aaverage t.

Applying this to a baseball's trajectory, Big Bertha (range 122 km), etc.



Class 10

More "realistic" motion: using finite differences

Air resistance or drag models:

Explain without air resistance

Explain how to model air resistance



Class 11

Finite differences

What does "finite difference" mean?

Using a spreadsheet to calculate (write the "program" in class).



Class 12

Reference frames

Galilean relativity

v1-compared-to-3 = v1-compared-to-2 + v2-compared-to-3

Do examples.

Why would anyone think there's a need to change: Fizz as observer vs. Tre'nbeth in the rocket ship as observer.

The interval as an invariant between reference frames.

The scalar product.



Class 13

Circular Motion

r(t) = R (cos(theta) i-hat + sin(theta) j-hat)

How do we get v(t)?

How do we get a(t)?

Define average angular velocity: .

omegaaverage = (change in theta)/(time interval involved)

Relation between v and R.

Relation between a and v.



Class 14

Momentum

p = gamma mv

gamma = sqrt(1 - v2/c2), approximately 1 at low speed

F = dp/dt.



Class 15

Momentum

Center of mass. The VCM and ACM.

Newton's Third Law

Is approximation that object is a point so bad after all?

Impulse is change in momentum over the time--integral of F dt.



Class 16

Momentum Conservation

Conservation Laws and symmetry

Noether's theorem

Momentum conservation in particle decays: neutron decay into proton.

Inferring the neutrino.



Class 17

Momentum Conservation

Examples of momentum conservation.

Inelastic collisions.



Class 18

Work

motivation

work done = F (dot) displacement [only if F is constant]

The integral method

the joule

work done against gravity: Wh = mgh

Internal work



Class 19

Energy and Power

kinetic energy

gravitational potential energy

spring potential energy

power: P = dW/dt.

the watt



Class 20

Conservation of Energy

Mechanical energy

bar diagrams

Conservation of energy in a closed system (the universe or a subsystem)

Noether's theorem

Machines

Ideal machines: (force)IN(distance)IN = FOUT dOUT

Real machines: WOUT < WIN

distortion (elasticity), thermal energy, etc.



Class 21

Thermal Energy, Relativistic Energy, Elastic Collisions

purely elastic collisions

Thermal energy

Relativistic energy (mass energy)

E2 = p2 c2 + m2 c4

becomes

(massless) pc

(massive) gamma m c2



Class 22

Simple Harmonic Motion

demonstration

springs and Hooke's Law

phase diagrams

Equation for SHM for a spring

Equation for SHM for a simple pendulum

cycle

y(t) = A cos (omega t + delta)

period, T

frequency, f

amplitude, A

damped harmonic oscillation



Class 23

Waves

pulse vs. wave

both carry momentum and energy

amplitude and wavelength

transverse vs. longitudinal waves

wave speed: c = f (wavelength) = fl



Class 24

Waves

y(x) = A cos (k x + d-prime)

k = 2 p/l

traveling waves

psi(x,t) = A cos (w t +/- k x + d)

transverse speed; partial derivative

transverse acceleration; partial derivative

the wave equation [wave equation]

dispersion of waves



Class 25

Waves and Superposition

adding waves--superposition: the displacement at a position in space when more than one wave is incident is the sum of the individual displacements

reflection of pulses and waves from ends



Class 26

Waves and Superposition

Strings, normal modes

nodes and antinodes

air columns

beats

resonance



Class 27

Resonance

beats

response curve

constructive and destructive interference

Young's experiment

diffraction



Class 28

Bandwidth

The bandwidth theorem: [bandwidth]

group velocity and phase velocity

the resonance curve

The Heisenberg Uncertainty Principle and the bandwidth theorem [Heisenberg]



Class 29

Conservative forces

The fundamental definition of work: d(work) = F (dot) d(displacement) = F € dr

A force is conservative when the work done against the force depends only on the starting and ending points, NOT ON THE PATH taken.

For conservative forces one may define a potential energy (another way of saying the same thing as above).

Potential energy U:

U(r2) - U(r1) = - integral from r1 to r2 of F€dr.

Then we may say: delta-W1-goes-to-2 = K2 - K1 = -[U(r-2) - U(r1)], which leads to

K + U = constant



Class 30

Potential energy

Discuss typical potential energy curves.

See that F(z) approximately equals -delta-U/delta-z.

In general,

F(r) = - gradient [U(r)].

Definition of the gradient operator: i-hat partial/partial-x + j-hat partial/partial-y + k-hat partial/partial-z.

Equipotential energy curves and the gradient.

Stability:

d2 U/dx2 > 0: stable

d2 U/dx2 < 0: unstable

d2 U/dx2 = 0: unclear; use higher derivatives to find out what happens.




take me to Gordon's home page

take me to the journal assignments

take me to the syllabus

take me to the quiz page




aubrecht@mps.ohio-state.edu [latest revision, 11 September 2003]