Transcript Gauss`s Law
Chapter 15
Electric Forces and
Electric Fields
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Gauss’s Law
Sections 7-9
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What is the difference between
Electric Field (E) and Force (F)?
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1)
o
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th
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25%
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1)
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Bo
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1. E factors out the magnitude of
the test charge, it only depends
on the other charges
2. E is defined everywhere,
F only at one point
3. Both 1) and 2)
4. Neither 1) or 2)
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• Corn Field: corn at regularly space intervals
• Vector Field: a vector at each point in space
• Scalar Field: a number at each point in space
– Eg: Temperature
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• Electric Field
field
• Field lines:
an easy way to visualize fields
– Tangent to E
– Density of lines
proportional to E
• begin at (+), end at (-)
• # of lines proportional to q
• lines don’t cross
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• Conductors & Electrostatic equilibrium
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E=0 inside a conductor
excess charge lies on outer surface
E is perpendicular to surface
charge is greatest at highest curvature
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Why are you safe inside a car
during a thunder storm? 45
1. The rubber tires insulate the
car from the ground
2. Charge cannot come inside
the metal shell of the car
3. The rounded car has a lower
charge density
4. It’s not safe!
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sa
fe
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no
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Millikan Oil-Drop Experiment
Active Figure: The Millikan Oil-Drop Experiment
• Millikan Oil-Drop Experiment
– Found every charge had an integral multiple of e (q = n e)
– Measured the elementary charge, e = 1.610-19 C
Equilibrium
Drag -- Terminal velocity
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Van de Graaff
Generator
• An electrostatic generator designed
and built by Robert J. Van de Graaff
in 1929
• Charge is transferred to the dome
by means of a rotating belt
• Limited by ionization of air, which
carries charge away
• Eventually an electrostatic discharge
takes place
MU28T33
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Museum of Science, Boston
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Holifield Radioactive Ion Beam Facility
Oak Ridge National Laboratory 25.5 MeV
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Electric Flux
• Field lines penetrating an
area A perpendicular to
the field
• The product of EA
is the flux, Φ
(the number of
field lines!)
• In general:
ΦE = E A cos θ
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Electric Flux, cont.
• ΦE = E A cos θ
– The perpendicular to
the area A is at an
angle θ to the field
– When the area is constructed such that a
closed surface is formed, use the convention
that flux lines passing into the interior of the
volume are negative and those passing out of
the interior of the volume are positive
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Gauss’ Law
• Gauss’ Law: the electric flux through any closed surface is
proportional to the net charge Q inside the surface
E
EA cos
Qinside
surface
0
– εo=8.85 x 10-12 C2/Nm2 is the permittivity of free space
– The area in Φ is an imaginary surface, a Gaussian surface,
it does not have to coincide with the surface of a physical object
Active Figure: Electric Flux Through an Arbitrary Closed Surface
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Electric Field of a Charged Thin
Spherical Shell
• The calculation of the field outside the shell is
identical to that of a point charge
Q
Q
E
ke 2
2
4r o
r
• The electric field inside the shell is E = 0
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Electric Field of a Nonconducting Plane
Sheet of Charge
• Total charge Q is uniformly
distributed over surface A
• Charge density σ = Q/A
• Use a cylindrical Gaussian
surface
• The flux through the ends
is EA, no field through the
curved part of the surface
E
2 o
• Note, the field is uniform
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Electric Field of a Nonconducting Plane
Sheet of Charge, cont.
• The field must be
perpendicular to the
sheet
• The field is directed
either toward or
away from the sheet
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Parallel Plate Capacitor
• The device consists of
plates of positive and
negative charge
• The total electric field
between the plates is
given by
E
o
• The field outside the
plates is zero
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What is the total electric flux through
the surface of the cube
in a constant electric field E? 45
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E
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20%
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EL
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E
0
E L2
6 E L2
2 E L2
6E
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Maxwell’s Equation #1
or
TIME
or
SPACE
They all mean the same thing.
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