Download Chapter 16 Electric Potential, Energy, and Capacitance

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Maxwell's equations wikipedia , lookup

Electromagnetism wikipedia , lookup

Lorentz force wikipedia , lookup

Electrical resistivity and conductivity wikipedia , lookup

Introduction to gauge theory wikipedia , lookup

History of electromagnetic theory wikipedia , lookup

Potential energy wikipedia , lookup

Aharonov–Bohm effect wikipedia , lookup

Electric charge wikipedia , lookup

Electrostatics wikipedia , lookup

Transcript
Chapter 16
Electric Potential, Energy,
and Capacitance
Units of Chapter 16
Electric Potential Energy and Electric Potential
Difference
Equipotential Surfaces and the Electric Field
Capacitance
Dielectrics
Capacitors in Series and in Parallel
16.1 Electric Potential Energy and
Electric Potential Difference
It takes work to move a charge against an electric
field. Just as with gravity, this work increases the
potential energy of the charge.
16.1 Electric Potential Energy and
Electric Potential Difference
Just as with the electric field, it is convenient to
define a quantity that is the electric potential
energy per unit charge. This is called the electric
potential.
Unit of electric potential: the volt, V
16.1 Electric Potential Energy and
Electric Potential Difference
The potential difference between parallel plates
can be calculated relatively easily:
For a pair of oppositely charged parallel plates, the
positively charged plate is at a higher electric
potential than the negatively charged one by an
amount ΔV.
16.1 Electric Potential Energy and
Electric Potential Difference
As with potential energy,
only changes in the
electric potential can be
defined. The choice of V
= 0 is arbitrary.
16.1 Electric Potential Energy and
Electric Potential Difference
Potential differences are defined in terms of
positive charges, as is the electric field. Therefore,
we must account for the difference between
positive and negative charges.
Positive charges, when released, accelerate toward
regions of lower electric potential.
Negative charges, when released, accelerate toward
regions of higher electric potential.
16.1 Electric Potential Energy and
Electric Potential Difference
Electric potential
difference of a point
charge:
16.1 Electric Potential Energy and
Electric Potential Difference
Whether the electric potential increases or
decreases when towards or away from a point
charge depends on the sign of the charge.
Electric potential increases when moving nearer to
positive charges or farther from negative charges.
Electric potential decreases when moving farther from
positive charges or nearer to negative charges.
16.1 Electric Potential Energy and
Electric Potential Difference
The electric potential energy of a system of two
charges is the change in electric potential
multiplied by the charge.
16.1 Electric Potential Energy and
Electric Potential Difference
The additional potential
energy due to a third
charge is the sum of its
potential energies relative
to the first two. Further
charges extend the sum.
16.2 Equipotential Surfaces and the
Electric Field
An equipotential surface is one
on which the electric potential
does not vary; it takes no work
to move a charge along an
equipotential surface.
16.2 Equipotential Surfaces and the
Electric Field
Equipotentials are
always perpendicular to
electric field lines.
This enables you to draw
one if you know the
other.
16.2 Equipotential Surfaces and the
Electric Field
Here, these
principles have been
used to draw the
electric field lines and
equipotentials of an
electric dipole.
16.2 Equipotential Surfaces and the
Electric Field
The direction of the electric
field E is that in which the
electric potential decreases
the most rapidly.
Its magnitude is given by:
16.2 Equipotential Surfaces and the
Electric Field
16.2 Equipotential Surfaces and the
Electric Field
Equipotential surfaces outside
a conductor
16.2 Equipotential Surfaces and the
Electric Field
The electron-volt (eV) is the amount of energy
needed to move an electron through a potential
difference of one volt.
The electron-volt is a unit of energy, not
voltage, and is not an SI standard unit. It is,
however, quite useful when dealing with
energies on the atomic scale.
Michael Faraday
• (1791-1867)
• Physicist + chemist
• Worked on magnetic fields
and the conduction of
electricity
• “Farads”
• Devilishly handsome
Count Alessandro Giuseppe Antonio
Anastasio Gerolamo Umberto Volta
• (1745-1827)
• Invented the
battery
• “Volts”
Batteries
• Batteries are represented in circuit
diagrams as:
where the larger side is
the positive terminal, and the smaller is the
negative.
16.3 Capacitance
A pair of parallel plates will store electric energy if
charged oppositely; this arrangement is called a
capacitor.
Capacitor
This
build this
up ofside
negative
charge
This
leaves
positively
will
create
an
electric
field
charged as the electrons arerepelling
pushed
from
the opposite
plate.
toelectrons
the positive
terminal
of the battery.
Before the battery is attached,
the wire is neutral.
+ -
Battery
16.3 Capacitance
The charge is related to the potential difference;
the ratio is called the capacitance.
SI unit of capacitance: the farad, F
16.3 Capacitance
For a parallel-plate capacitor,
The quantity inside the parentheses is called
the permittivity of free space, and is
represented by ε0.
εo A
C=
d
16.3 Capacitance
The energy stored in a
capacitor is the energy
required to charge it:
16.4 Dielectrics
“Dielectric” is another word for insulator. A
dielectric inside a capacitor increases the
capacitor’s energy storage by an amount
characterized by the dielectric constant, κ.
16.4 Dielectrics
A dielectric in an electric field becomes polarized;
this allows it to sustain a larger electric field for the
same potential difference.
16.4 Dielectrics
The capacitance of a capacitor containing a
dielectric is increased:
16.4 Dielectrics
Inserting a dielectric
into a capacitor while
either the voltage or
the charge is held
constant has the
same effect—the
ratio of charge to
voltage increases.
16.5 Capacitors in Series and in Parallel
Capacitors in series all have the same charge; the
total potential difference is the sum of the potentials
across each capacitor.
Note that this gives the
inverse of the capacitance.
16.5 Capacitors in Series and in Parallel
Capacitors in parallel all have the same potential
difference; the total charge is the sum of the charge
on each.
16.5 Capacitors in Series and in Parallel
We can picture capacitors in parallel as forming
one capacitor with a larger area:
Review of Chapter 16
Electric potential difference between two points is
the work done per unit charge in moving a charge
between those two points.
Equipotential surfaces are surfaces on which the
electric potential is constant.
Electric potential for a point charge:
Electric potential energy for a pair of point
charges:
Review of Chapter 16
Electric potential energy for an array of point
charges:
The electric field is in the direction of maximum
change of the electron potential.
Magnitude:
Review of Chapter 16
An electron-volt is the energy gained by an
electron accelerating through a potential difference
of one volt.
A capacitor consists of two metallic plates;
capacitors store electric energy.
Capacitance:
Review of Chapter 16
Capacitance of a parallel-plate capacitor:
Energy stored in a capacitor:
Review of Chapter 16
A dielectric is a nonconductor; it increases
capacitance.
Dielectric constant:
Capacitors in series:
Capacitors in parallel: