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.
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.
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?
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.
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
trigonometry
components
reference frame/coordinate system
addition
subtraction
length
meaning
Compare two and three dimensions to one dimension
Do Newton's Third Law examples and problems
Pairs act on different bodies.
The sum of the forces acting on a body is zero.
This is a vector relation.
Do examples.
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.
What does mass do?
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.
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
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)
Instantaneous speed and velocity compared to average speed and velocity.
The m/s, the km/h.
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)
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.
Air resistance or drag models:
Explain without air resistance
Explain how to model air resistance
What does "finite difference" mean?
Using a spreadsheet to calculate (write the "program" in class).
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.
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.
p = gamma mv
gamma = sqrt(1 - v2/c2), approximately 1 at low speed
F = dp/dt.
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.
Conservation Laws and symmetry
Noether's theorem
Momentum conservation in particle decays: neutron decay into proton.
Inferring the neutrino.
Examples of momentum conservation.
Inelastic collisions.
motivation
work done = F (dot) displacement [only if F is constant]
The integral method
the joule
work done against gravity: Wh = mgh
Internal work
kinetic energy
gravitational potential energy
spring potential energy
power: P = dW/dt.
the watt
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.
purely elastic collisions
Thermal energy
Relativistic energy (mass energy)
E2 = p2 c2 + m2 c4
becomes
(massless) pc
(massive) gamma m c2
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
pulse vs. wave
both carry momentum and energy
amplitude and wavelength
transverse vs. longitudinal waves
wave speed: c = f (wavelength) = fl
y(x) = A cos (k x + k = 2 traveling waves
psi(x,t) = A cos ( transverse speed; partial derivative
transverse acceleration; partial derivative
the wave equation
dispersion of waves
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
Strings, normal modes
nodes and antinodes
air columns
beats
resonance
beats
response curve
constructive and destructive interference
Young's experiment
diffraction
The bandwidth theorem:
group velocity and phase velocity
the resonance curve
The Heisenberg Uncertainty Principle and the bandwidth theorem
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
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 the journal assignments
Class 24
Waves
Class 25
Waves and Superposition
Class 26
Waves and Superposition
Class 27
Resonance
Class 28
Bandwidth
Class 29
Conservative forces
Class 30
Potential energy
aubrecht@mps.ohio-state.edu [latest revision, 11 September 2003]