Kinematics and Mechanics
x = x0 + v0x t + 1/2ax t
2
vx = v0x + ax t
2
2
vx = v0x + 2ax (x x0 )
Fx = max
Fcentripetal
mv 2
=
r
Vg = mgh
Ktrans = 1/2mv 2
p = mv
p
t
W
P =
t
F =
Fe =
P = I V = I2 R =
V2
R
VC = V0 (et/RC )
Req = R1 + R2 + R3 = i Ri
1
1
1
1
1
Kinematics and Mechanics x = x0 + v0x t + 1/2ax t2 vx = v0x + ax t Fx = max
2 2 vx = v0x + 2ax (x - x0 )
J = c E Current & Circuits Q I= t V =I R L R= A P = I V = I2 R = VC = V0 (e-t/RC ) Req = R1 + R2 + R3 = i Ri 1 1 1 1 1 = + + = i Req R1 R 2 R3 Ri Magn
E1 Basic Electrostatics
General Physics
1
Electrostatics
Complete the tutorial on electrostatics
(both sides of handout)
Tape activity
www.sos.siena.edu/~rfinn/phys140s09/
tape.pdf
Electrostatics
electric charges that are not moving
Definition of new symb
E2 - Electric Field
Electrostatic & gravitational force
act at a distance, no direct push or pull
Electric Field
conceived by Michael Faraday
extends out from every charged object
other charges interact with field
direction of field determined by motion i
General Physics
Lab 2
Siena College
Electric Fields and Potential
Object
This experiment further explores the electrostatic interaction between charged objects. The
concepts of electric field and potential are illustrated primarily through exercises with
Name
Date
Pd
E&M Unit 4 - Magnetism: Worksheet 3
1. A straight wire 50 cm long conducts a 6.0 A current directed up out of the page. If the wire
experiences a force of 0.24 N to the right due to a magnetic field perpendicular to its length,
what is the ma
General Physics
Lab 1
Siena College
In 1686, Newton published the first quantitative description of the gravitational force between any two
objects. He explained that the force of gravity is directly proportional to the product of the masses, m1
and m2, a