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Transcript
Electric Field
The Concept of the Electric Field

In the force model of the electric field, the positive charge A exerts an
attractive force on charge B.
© 2015
Pearson
Education,
Inc.
The Concept of the Electric Field

In the field model, it is the
alteration of space around charge
A that is the agent that exerts a
force on charge B.

The alteration of space is what we
call a field.

The charge makes an alteration
everywhere in space.
© 2015
Pearson
Education,
Inc.
The Concept of the Electric Field

The space around a charge is altered to create an electric field.

The alteration of space around a mass is called the gravitational field.

The alteration of space around a magnet is called the magnetic field.
The field model describes how charges interact:
1.
A group of charges, which we will call the source charges, alters the space around
them by creating an electric field E.
2.
If another charge is then placed in this electric field, it experiences a force F exerted by
the field.
© 2015
Pearson
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
The
Field
Model
We define
the electric
field E at the point as
E
F
qtest ch arg e
k
Qq
2
r
E
qtc
Q
Ek 2
r

The units are newtons/coulomb, N/C.

The magnitude E of the electric field is called the electric field strength.

The direction of the vector is determined by which way it is pointing
© 2015
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The Field Model
In the field model, the field is the agent that exerts an electric force on a particle with charge q.
1.
2.
3.
4.
The electric field, a vector, exists at every point in space. Electric
field diagrams will show a sample of vectors, but there is an
electric field vector at every point whether one is shown or not.
the electric field vector points AWAY from a POSITVE charge
source
the electric field vector points TOWARD a NEGATIVE charge
source
The electric field does not depend on the magnitude of the
charge used to probe the field (test charge). The electric field
depends only on the source charges that create the field.
© 2015
Pearson
Education,
Inc.
The Electric Field of a Point Charge

An electric field diagram for a
positive point charge is
constructed by drawing electric
field vectors at a number of points
around the positive charge.

All the vectors point straight away
from the positive charge.

E-field becomes weaker the
farther away from the source
© 2015
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The Electric Field of a Point Charge

The electric field diagram for a
negative charge is drawn with the
vectors pointing toward the negative
point charge.

This would be the direction of the
force on a positive probe charge.
© 2015
Pearson
Education,
Inc.
The Electric Field of a Point Charge
For an electric field diagram:
1.
The diagram is just a representative sample of electric field vectors. The field exists at all
the other points. A well-drawn diagram gives a good indication of what the field would
be like at a neighboring point.
2.
The arrow indicates the direction and the strength of the electric field at the point to
which it is attached—at the point where the tail of the vector is placed. The length of
any vector is significant only relative to the lengths of other vectors.
3.
Although we have to draw a vector across the page, from one point to another, an
electric field vector does not “stretch” from one point to another. Each vector
represents the electric field at one point in space.
© 2015
Pearson
Education,
Inc.
Example Problem
A small bead, sitting at the origin, has a charge of +10 nC. At the point (3.0
cm, 4.0 cm), what is the magnitude and direction of the electric field due to
this bead?
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Example Finding the field near a dipole
A dipole consists of a
positive and negative
charge separated
by a small distance.
What is the electric
field strength along
the line connecting
the charges at a
point 1.2 cm to the
right of the positive
charge?

The electric field
due to multiple
charges is the
vector sum of the
electric field due
to each of the
charges.
Enet  E1  E2  ...
© 2015
Pearson
Education,
Inc.
Example Problem
Determine the magnitude and the direction of the electric field at point A.
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Uniform Electric Fields

A parallel-plate capacitor is the
arrangement of two electrodes closely
spaced and charged equally but oppositely.

An electrode is a conducting plate.
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Uniform Electric Fields

Inside a parallel-plate capacitor, the
horizontal components of the
individual fields cancel.

The vertical components add to
give an electric field vector pointing
from the positive plate to the
negative plate.
© 2015
Pearson
Education,
Inc.
Uniform Electric Fields

Inside a parallel-plate capacitor, the electric field
at every point is the same in both strength and direction.

This is called a uniform electric field.
Q
E
0 A
© 2015
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Uniform Electric Fields

There are a few things to note about a parallel-plate capacitor:

The field depends on the charge-to-area ratio Q/A, which is
often called the charge density. If the charges are packed
more closely, the fields will be larger.

Our analysis requires the separation of the plates to be small
compared to their size. If this is true, the spacing between the
plates does not affect the electric field.

The shape of the electrodes is not relevant as long as the
electrodes are close together.
© 2015
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Example: Finding the field in an air cleaner
Long highway tunnels must have air cleaners to remove
dust and soot coming from passing cars and trucks. In one
type, known as an electrostatic precipitator, air passes between two
oppositely charged metal plates, as in FIGURE 20.31.
© 2015
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Example: Finding the field in an air
cleaner (cont.)
The large electric field between the plates ionizes dust and soot particles,
which then feel a force due to the field. This force causes the charged
particles to move toward and stick to one or the other plate, removing them
from the air. A typical unit has dimensions and charges as shown in Figure
20.31. What is the electric field between the plates?
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Electric Field Lines

Electric field lines are imaginary lines drawn
through a region of space to help visual the
electric field.

The electric field lines are drawn so that

The tangent to a field line at any point is
in the direction of the electric field E at
the point, and

The field lines are closer together where
the electric field strength is greater.

Field lines cannot cross. The tangent to
the field line is the electric field vector,
which indicates the direction of the
force on a positive charge. The force
must be in a unique, well-defined
direction, so two field lines cannot cross.
© 2015
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Electric Field Lines
The electric field is
created by charges.
Field lines start on a
positive charge and
end on a negative
charge.
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Conceptual Example 20.9 Drawing
electric field lines for a charged
sphere and a plate
FIGURE 20.36 shows a positively charged metal sphere above a conducting
plate with a negative charge. Sketch the electric field lines.
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Conductors and Electric Fields
In a conductor in electrostatic
equilibrium, none of the
charges are moving.
 Charges in a conductor are free
to move. If there is an electric
field they will move, and the
conductor could not be in
electrostatic equilibrium.
 Therefore, the electric field is
zero at all points inside a conductor in
electrostatic equilibrium.

© 2015
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Conductors and Electric Fields



Any excess charge inside a
conductor must lie at its surface.
Any charge on the interior would
create an electrical field there, in
violation of our conclusion that
the field inside is zero.
Physically, the repulsive forces
of the charges cause them to
move as far apart as possible
without leaving the conductor.
© 2015
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Conductors and Electric Fields


The electric field right at the
surface of a charged conductor
is perpendicular to the surface.
If the electric field had a
component tangent to the surface,
it would exert a force on charges
at the surface and cause them to
move along the surface, violating
the assumption that all charges
are at rest.
© 2015
Pearson
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Conductors and Electric Fields

The electric field within a conducting
enclosure is zero.

A conducting box can be used to
exclude electric fields from a region of
space; this is called screening.

Metal walls are ideal for screening, but
wire screens or wire mesh can be
used.
© 2015
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Conductors and Electric Fields

Although any excess charge of a
conductor will be found on the
surface, it may not be uniformly
distributed.

At sharp points, the density of the
charge is higher, and therefore
the electric field is stronger.
© 2015
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Conductors and Electric Fields

The electric field near very sharp points may be strong enough to ionize
the air around it.

A lightning rod has a sharp point so that if a building is beginning to
accumulate charge, meaning a lightning strike might be imminent, a large
field develops at the tip of the rod.

Once the field ionizes the air, excess charge from the building can
dissipate into the air, reducing the electric field and the likelihood of a
lightning strike.

The lightning rod is intended to prevent a lightning strike.
© 2015
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Forces and Torques in an Electric Field

The force exerted on a charge in a known electric field is
© 2015
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Example: Finding the force on an electron in
the atmosphere
Under normal
circumstances, the
earth’s electric field
outdoors near
ground level is
uniform, about 100
N/C, directed down.
What is the electric
force on a free
electron in the
atmosphere? What
acceleration does
this force cause?
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Example Problem
What is the magnitude and direction of the electric force on charge A? 2 ways to solve
© 2015
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Forces and Torques in an Electric Field

An electric
dipole in a
uniform
electric field
experiences
no net force.

There is a net torque on a dipole in
a uniform electric field, which
causes it to rotate.

The electric dipole moment is a
vector pointing from the negative
to the positive charge of a dipole.
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Forces and Torques in an Electric Field

The equilibrium position of a dipole
in an electric field is with the electric
dipole moment aligned with the
field.
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Example Problem
An electric field E = (200,000 N/C, right)
causes the 2.0 g ball to hang at an
angle. What is θ?
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Electric Field Lines
Text: p. 651
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Pearson
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Electric Field Lines
Text: p. 651
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Summary: General Principles
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Summary: General Principles
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Summary: Important Concepts
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Summary: Important Concepts
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Summary: Applications
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Summary: Applications
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Summary: Applications
© 2015
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Summary
Text: p.
657
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Pearson
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Summary
© 2015
Pearson
Education,
Inc.