JUNE JORDANS POETRY FOR THE PEOPLE * AFRICAN AMERICAN STUDIES 156AC * SPRING 2010 SYLLABUS * INSTRUCTOR:
AYA DE LEON
POETRY FOR THE PEOPLE
SPRING 2010 SYLLABUS
POETRY FOR THE PEOPLE: INTRODUCTION TO T
Topics for 137A Midterm
1) 4 Postulates, probability, spread in distribution (wave) function
2) Eigen-functions and eigen-values, apply postulates to overlap problems, collapse of wavefcn
3) Operators
A Note Regarding the Final: The final exam will be held on Tues., 12/13/11,
from 3pm to 6pm, in 9 Evans. The final exam is a closed book exam, but you are
allowed to bring two pages of notes (you can
4 Postulates of Quantum Mechanics
1) Every physically realizable state of a particle can be described by a state vector (or
"wavefunction"), , that can be represented as a vector in the Hilbert space
Notes on Stokes Parameters
Brian Henning
November 11, 2010
Degrees of freedom
Jones vectors gave us a formalism for describing polarized light. What if the light is only partially
polarized? This is w
ELECTROMAGNETISM & OPTICS (PHYSICS 110B)
SPRING SEMESTER 2012
Instructor: Prof. Christopher F. McKee
Oce: C31 Hearst Field Annex (HFA); oce hours in B26 HFA
Email: [email protected]
Oce hours: Thurs
PHYSICS 110B Spring 2012
Midterm Review
Mai Truong
1. Let frame O move with speed v in the x-direction relative to O. A photon with
frequency measured in O moves at an angle relative to the x-axis.
(a
Problem 1
Problem 2
Problem 2
Problem 3
Problem 3
Problem 4
[15 pts] Let B (v) be a Lorentz boost associated with the 3-velocity v. Consider
B (v1 )B (v2 )B (v1 )B (v2 )
where v1 v2 = 0. Assume v1 1,
Midterm I Review Questions
Physics 110B
Week of 4/Oct/2010
Problem 1
Consider an innitely long line of charge with charge per unit length lying along the x -axis, at
rest in frame O . Find the four-ve
Final Exam Review Questions
Physics 110B
Week of 6/Dec/2010
Problem 1: Things move fast at the LHC
The Large Hadrom Collider is designed to collide protons at energies of 7 TeV (1 TeV = 1012 eV).
(a)
I n t r o d u c to r y P h y s i cs
U.C. Berkeley
Physics 8B, Fall 2011
Section I
Exam 1
October 5, 2011
Notes: Correct answers without supporting derivations will not receive credit. You mu st show y
Adriano Corrales, Adis Mara
Tengo un inters fuerte en cine y las relaciones entre sexos. El poema, Adis Mara,
cabe ambos reas, escribiendo de la explotacin de la actriz principal en la pelcula, Last T
Prof. Lydia L. Sohn
UC Berkeley, Fall 2013
ME290L: Introduction to Nanobiology
Spring 2013
Revised Syllabus
Week 1
Introduction to the Class and Class organization
Week 2
Basic Biology Refresher
Week
Lectures
Tu Th: 8:00-9:30am, 60 Evans
Instructor: Prof. Dung-Hai Lee
Office: 531 Birge
Office Hours: Tu 9:30-11am
[Note: Office hours are reserved for discussion of lectures, not to give hints for hom
1. Pressures on the right and left side of the gate
The pressure in the water as a function of z is found as follows:
dPw (z )
= w g Pw (z ) Pw (z = H ) =
dz
z
w g dz
z =H
and
Pw (z = H ) = Patm
(1.1)
I
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Showing a System is Linear and Shift Invariant Prepared by: Piotr Dollar
1
Showing Linearity
To show a system H is linear, we need to show that for all functions f1 and f2 , H satisfies the following
Midterm 1 Review
February 16, 2013
If youre ever stuck on a problem, go through a list of all the topics and write out
any equations that apply. Remember, there are only so many equations that you can
1. Find the current through the battery.
2. In this circuit, the weird looking resistor is called a variable resistoryou can manually adjust it
to have a resistance that you choose.
a. Suppose R1 is s
Midterm 1 Review
February 16, 2013
Electric eld
1 Gausss law for a cylinder
Consider a long thin cylindrical rod of uniform charge density, . The rod has radius s
and length 50s.
1.1
Find the rods lin
Magnetism
March 17, 2013
1 Magnetic elds: Overview
1. Magnetic elds are caused by moving charge, as opposed to electric elds which
can be caused just by stationary charges
2. Magnetic elds exert a for
April 16, 2013
1 Amperes Law
With Amperes law, the important thing to remember is that we want to take the integral
so our path is parallel to the magnetic eld at all points. This simplies our integra
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Problem 73
April 16, 2013
1 r < w
Close to the conductor, the long, at bar will basically look like an innite slab.
Since J gives current density per unit area, J = I/lw. We can rearrange this so I =