Title: Monday, January 5, 2009
1Monday, January 5, 2009
 Spherical Distribution Laws
2Announcements
 USAYPT participantsI need paperwork and fees by
tomorrow at the latest!  New notes packetwere starting EM!
3When we say that an object is charged, what do
we really mean?
 If a particle bears an electrical charge, we can
generally assume it has an excess of electrons
(negative charge) or an excess of protons
(positive charge).  Fine point usually, only electrons move, so
positive charge (an excess of protons) is really
an absence of electrons.
4Fundamentals of Electrical Charge
 Charge on electron e
 Charge on proton e
 e 1.602 ? 1019 Coulombs , C
 Any charge q is a multiple of the number of extra
electrons or missing electrons such that q ne
5Lets talk about spherical distribution.
 What do you think we mean by a spherical
distribution law? Give an examples.
6Lets talk about spherical distribution.
 Write the formula for the surface area of a
sphere.
7Spherical distribution law for gravity
Newtons Law of Gravity
G 6.7 ? 1011 Nm2/kg2 m1 and m2 are spherical
or point masses in kg. r is the separation
between the centers of the masses
8Spherical distribution law for electrical force
 k 8.99 ? 109 Nm2/C2
 q1 and q2 are spherical or point charges in
Coulombs.  r is the separation between the centers of the
charges
Coulombs Law
9How are electrical and gravitational forces
similar?
 They both follow spherical distribution laws. The
forces diminish as the surface area of a sphere.
10How are electrical and gravitational forces
different?
 Electrical forces can be attractive or repulsive,
while gravitational forces are only attractive.  Gravitational forces are much weaker than
electrical forces.
11For Two Charges
 The electrostatic force is repulsive if the
charges are of the same sign and attractive if
the charges are of unlike sign.  The force exerted on charge A by charge B is
always equal and opposite of the force exerted by
charge B on charge A (Newtons 3rd Law)
12For More Than Two Charges
 Determine the force on a charge due to each of
the other charges in the vicinity.  Do a vector addition.
When you are determining electrostatic force, you
focus on one charge.
q
Its all about me! Who is nearby who can affect
me?
13Sample problem Using unit vector notation, write
an expression for the force exerted on the upper
right charge by the other two charges.
5.0 mC
2.0 mC

0.10 m
0.10 m
5.0 mC
14Tuesday, January 6, 2009
 Gravitational and Electric Fields
15Announcements
 USAYPT participantsI need paperwork and fees
today.
16Sample problem Two identical balls of mass m and
charge q are hanging from strings of length L.
Derive an expression for q in terms of m, ?, L,
and fundamental constants.
?
L
L
m,q
m,q
17What is meant by a force field?
 A force field creates a force when an object is
placed in it. It is a property of empty space.  An electric field creates an electric force on a
charge placed in it.  The electric field is created by a charge
distribution.  A gravitational field creates a gravitational
force on a mass placed in it.  The gravitational field is created by a mass
distribution.
18Gravitational Field
 Draw the gravitational field around the earth.
19Gravitational Field
 How can you calculate the gravitational force on
a small mass in a gravitational field?
20Gravitational Field
 What is an equation that can be used for
gravitational field calculations?
21Gravitational Field
 What is the value of the gravitational field at
the surface of the earth?
22And nowthe Electric Field
 Boot up computer.
 Go to my folder on the N drive
 Go to Period 2, Projects, Volume 2
 When you are at the right place, look up.
23The Electric Field
 Draw the electric field around a positive charge.
24The Electric Field
 Draw the electric field around a negative charge.
25The Electric Field
 How can you calculate the electric force on a
small charge in an electric field from the
magnitude of the electric field?
26The Electric Field
 What is an equation that can be used for electric
field calculations?  What is the limitation of the equation shown
above?
27Summary of the Electric Field
 This equation can be used to calculate the
electric field a distance r away from a the
center of a spherically symmetric charge
distribution of qo Coulombs.  Another charge q entering the electric field
created by qo will experience a force F, which
can be calculated by the equation F qE.
28Summary of Electric Field Direction
 The direction of the electric field at a point in
space is the direction that a small positive
charge at rest (a test charge) wishes to move
if it is placed at that location.  Thus, the electric field points away from
positive charges and toward negative charges.  If more than one charges is generating the field,
vector addition must be done to add the fields
produced by each of the charges to get the
resulting field. This is called superposition
of the individual fields.
29Wednesday, January 7, 2008
30Announcements
 Saturday practice for USAYPT from 1000 to 200
PM. Who can come?  Get out homework Ch23 7,8,9 for self correction.
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34 Sample problem Determine where the electric
field is zero if a 2.0 mC charge is located at
the origin and a 3.0 mC charge is located at x
1.0 meter.
35Limitations of Coulombs Law
 Coulombs Law equations for Force and Field can
only be used directly for point charges or
spherically symmetric charges.  For more complicated continuous charge
distributions we need to break up the charge
distribution into little bitty pieces and use
Coulombs Law and superposition together to
determine the electric field at a given location
in space near the charge distribution.
36Linear Charge Distribution
 When charge resides on a long thin object such as
a wire or a ring, we call that a linear charge
distribution.  It is sometimes convenient for us to define a
linear charge density, ?, which is charge per
unit length.  ? Q/L dQ/dL
37Surface Charge Distribution
 When charge resides on larger surface, we call it
a surface charge distribution.  It is sometimes convenient for us to define a
surface charge density, s, which is charge per
unit area.  s Q/A dQ/dA
38General Procedure  continued
 You need to integrate over a spatial variable
(not charge!). Appropriate choices are linear
distance, arc length, or angle (x,y,s,q,f)  Find a common variable that r and/or dq both
depend on.  See if symmetry (and trig) can be used to
simplify the problem by elimination of offaxis
components of E.  Find the appropriate limits to the integral.
 Dont skip setup steps. The physics is in the
setup!
39Volume Charge Distribution
 When charge resides distributed within a solid
object, we have a volume charge distribution.  It is sometimes convenient for us to define a
surface charge density, r, which is charge per
unit area.
40General Procedure for Electric Field Calculations
 Each little infinitesimally small charge dq in a
charge distribution containing Q total Coulombs
creates its own tiny electric field dE at a point
P in space a distance r from dq.  I can add all these little infinitesimal fields
dE together to get the field at point P.  What does this sound like to you?
41Thursday, January 8, 2008
 More on Charge Distributions
42Announcements
 Get out HW Ch 23 13,14,15 to grade.
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45Sample Problem
 Determine the electric field magnitude and
direction a distance y away from an extremely
long, straight wire of charge density l.
y
46Sample Problem
 Determine the electric field magnitude and
direction a distance x away from a ring of radius
R bearing charge Q.
x
R
47Friday, January 9, 2009
 Motion of Charged Particle in Efield
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50 Sample Problem Determine the electric field
magnitude and direction at point P in the figure
shown. The semicircular ring bears charge 2.0mC
and has a radius of 0.50 m.
P
R
51Motion of Charged Particles in Electric Fields
 If the electric field is constant, acceleration
will be constant, and kinematic equations can be
employed.  The motion is not unlike projectile motion.
52Sample problem
 What is the speed and position of an electron
released from rest in this electric field after
3.0 ns?
e
E 320 N/C
53Sample problem
 What is the velocity and position of this
electron 3.0 ns after it enters the field?
E 320 N/C
y
e
x
v 20,000 m/s
54Static Electricity Experiment 1
 Blow up the balloon and charge it by rubbing it
against your hair. Can you deflect a flowing
stream of water with the charged balloon?  Is the water charged? If not, why is it being
deflected? See if your group can come up with a
plausible answer.
55Static Electricity Experiment 2
 Cut 2 20cm strips of transparent tape (mass of
each 65 mg). Fold about 1 cm tape over at one end
of each strip to create a handle. Press both
pieces of tape sidebyside on your lab table and
rub your finger back and forth across the strips.
Quickly pull the strips off the lab table. Hold
the handles together and the strips will repel
each other, forming an inverted V. Estimate the
charge on each strip. Assume the charges act as
though they are at the center of mass of the
strip.  Hint Begin by drawing a Free Body Diagram!
56Monday, January 12, 2009
57Announcements
 Get out homework (page 7 in packet)
58Flux
 Flux means flow.
 Consider three rectangular wire loops in a vector
field.  Which one has maximum flux (or flow) of the field
lines through it?
max flux no flux intermediate
flux
59To Increase Flux
 Increase the field
 Increase the area of the loop
 Make sure the hoop is appropriately angled
max flux no flux intermediate
flux
60The Area Vector
 The area vector is defined as a vector
perpendicular to a surface with magnitude equal
to the scalar area of the surface.  Consider the angle between v and A.
A
A
A
For what angle is the flux maximum?
61Flux Equation
 The flux is proportional to field vector
magnitude, area vector magnitude, and the cosine
of the angle between them.
A
A
A
What vector operation does this sound like?
62Flux Equation
A
A
A
What vector operation does this sound like?
63Flux Equation for Electric Field
Units Nm2/C
A
A
A
64Area Vectors For a Closed Shape
 This rectangular prism has six surfaces. Each
surface has an area vector that points outward
from center of the prism, and is normal to the
surface.
65Another Example
 This cylinder is a bit more complicated. The top
and bottom have areas that can easily be
calculated, and the corresponding vectors point
outward. On the sides, we must define and
infinite number of infinitesimally small areas,
each of which defines a little vector (dA) that
points outward.
66The Calculation of Flux Over a Closed Surface in
a Vector Field
 At each point on the closed surface, we must take
the dot product with the vector field to get the
flux for that small area. Then we add all these
dot products up together to get the flux for the
entire surface. This leads to some interesting
observations.  If there is a source of the vector field in the
closed shape, the flux over its surface is
positive.  If there is a sink of the vector field in the
closed shape, the flux over its surface is
negative.  If there is neither a source or sink of the
vector field in the closed shape, the flux over
its surface is zero.
67What do we mean by source and sink of an
electric field?
 The source is where the field starts, and the
sink is where the field terminates.  In an electric field, the source is the positive
charge, and the sink is the negative charge.  Therefore,
 If a closed shape encloses a positive charge, the
flux is positive.  If a closed shape encloses a negative charge, the
flux is negative.  If the closed shape encloses no net charge, the
flux is zero.
68Mathematical Representation
 For a general vector field, v
 For an electric field, E
In an electric field, the closed shape we
integrate the flux over is referred to as a
Gaussian surface.
69 Sample Problem Calculate the electric flux
through a spherical surface of radius 2.0 m
containing a point charge of 3mC at its center.
70 Problem 24.1 Draw an electric dipole, and sketch
three Gaussian surfaces for which one has
positive electric flux, one has negative electric
flux, and one has zero electric flux.
71 Problem 24.2 A vertical field of 2.4 x 104 N/C
exists above Earths surface when thunderstorm is
brewing. What is flux through car of approximate
rectangular size of 5.0 m by 3.0 m if it is
traveling on a road with a 10o slope.
72 Problem 24.6 A uniform field of ai bj
intersects a surface of area A. What is the flux
through the area if the surface lies in (a) the
xy plane? (b) the xz plane (c) the xy plane?
73 Problem 24.9 A cone with base radius R and
height h is located on a horizontal table. A
horizontal uniform field E penetrates the cone.
Determine the electric flux that enters the
lefthand side of the cone.
74Tuesday, January 13, 2009
 Gausss Law of Electricity
75Announcements
 Get out homework Problems 23 46,47,52
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79Gauss Law of Electricity
 q net charge (C) enclosed inside a given
Gaussian surface. This is a sum of all and 
charges  ?o electrical permittivity of free space
 8.85 ? 1012F/m
 8.85 ? 1012C2/Nm2
 ?E electrical flux over the Gaussian surface
80Other forms of Gausss Law
Integral forms give indication of enclosed charge.
Differential form gives indication charge
density. For more information see
http//hyperphysics.phyastr.gsu.edu/hbase/electri
c/maxeq2.html
81Gaussian Surface
 A Gaussian surface is simply any closed shape in
space, which can be of any arbitrary shape.  All Gaussian surfaces give the same answer in
Gausss Law if they enclose the same net charge!
So, to make the math easier, Gaussian surfaces
are typically chosen for convenience and high
symmetry with regard the electric field.
82Whats Gausss Law Good For?
 Gausss Law can be used to determine how much
charge is enclosed in a surface.  More commonly, Gausss Law is used to determine
the electric field at a point in space.
83Sample Problem
A point charge q is located a distance d from a
long infinite wire. Determine the electric flux
through the plane due to the point charge.
84Nonconstant Fields
 Do some investigating of the properties of
electric fields at  http//www.falstad.com/mathphysics.html
85January 14, 2009
 Application of Gausss Law
86Announcements
 Get out HW problems 24 3,5,7,8
 Exciting movie
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89Sample Problem Consider two Gaussian surfaces, a
sphere of radius R and a cube of side 4R. In each
is a positive point charge of q. How does the
electric flux compare for the two surfaces?
90 Sample Problem Derive the electric field a
distance y away from a long charged wire bearing
a linear charge distribution l. (NOT IN PACKET)
y
91 Sample Problem Derive the electric field outside
a charged nonconducting cylinder with an even
charge distribution.
92 Sample Problem Derive the electric field INSIDE
a charged nonconducting cylinder with an even
charge distribution.
93January 15, 200 8
94Announcements
 Problems 24 13,14,15
 Movie!
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