CAPACITORS
AND CHARGE
STORAGE
•Capacitor - is a
device that is used to
store electrical
potential energy.
•-Uses: tuning the
frequency of radio
receivers, eliminating
sparking in automobile
ignition systems, and
storing energy in
An energized (or charged)
capacitor is useful because
energy can be reclaimed
from the capacitor when
needed for a specific
Parallel-plate capacitor -
typical design for a
capacitor consists of two
parallel metal plates
separated by a small
How to energize a capacitor?
The capacitor is energized
by connecting the plates to
the two terminals of a battery
or other sources of potential
difference
When this
connection is made,
charges are removed
from one of the plates,
leaving the plate with a
•An equal and opposite amount of
charge accumulates on the other
plate. Charge transfer between
the plates stops when the
potential difference between the
plates is equal to the potential
difference between the terminals
Capacitance -is defined
as the ratio of the net charge
on each plate to the potential
difference created by the
separated charges.
The SI unit for capacitance is the farad, F, which
is equivalent to a coulomb per volt (C/V). In
practice, most typical capacitors have
capacitances ranging from microfarads (1 µF = 1
× 10−6 F) to picofarads (1 pF = 1 × 10−12 F).
Capacitance depends on the size and shape of the capacitor
The capacitance of a parallel-plate capacitor with
no material between its plates is given by the
following expression:
The capacitance of a
sphere increases as
the size of the sphere
increases.
The material between a capacitor’s
plates can change its capacitance
-So far, we have assumed that the
space between the plates of a
parallel-plate capacitor is a vacuum.
However, in many parallel-plate
capacitors, the space is filled with a
material called a dielectric.
dielectric -is an insulating
material, such as air, rubber,
glass, or waxed paper. When a
dielectric is inserted between
the plates of a capacitor, the
capacitance increases.
The capacitance increases because
the molecules in a dielectric can
align with the applied electric field,
causing an excess negative charge
near the surface of the dielectric at
the positive plate and an excess
positive charge near the surface of
the dielectric at the negative plate.
According to the
expression:
Q = C∆V, if the charge
increases and the potential
difference is constant, the
-A capacitor with a
dielectric can store more
charge and energy for a
given potential difference
than the same capacitor
ENERGY AND CAPACITORS
The electrical potential energy stored in a
capacitor that is charged from zero to some
charge, Q, is given by the following
expression:
*Note that this equation is also an
expression for the work required to charge
the capacitor.
•By substituting the definition of capacitance
(C = Q/∆V), we can see that these alternative
forms are also valid:
•PEelectric = 1/2 C(∆V)2
•PEelectric = Q2/ 2C
To determine the potential energy, use the
alternative form of the equation for the potential
energy of a charged capacitor:
SOLVE:
A 4.00 µF capacitor is connected to a
12.0 V battery.
a. What is the charge on each plate of the
capacitor?
b. If this same capacitor is connected to a
1.50 V battery, how much electrical
potential energy is stored?
ANSWERS:
a. 4.80 × 10 −5 C
b. 4.50 × 10 −6 J
SUMMARY:
SUMMARY:
SUMMARY:

CAPACITORS.pptx

  • 1.
  • 2.
    •Capacitor - isa device that is used to store electrical potential energy.
  • 3.
    •-Uses: tuning the frequencyof radio receivers, eliminating sparking in automobile ignition systems, and storing energy in
  • 4.
    An energized (orcharged) capacitor is useful because energy can be reclaimed from the capacitor when needed for a specific
  • 5.
    Parallel-plate capacitor - typicaldesign for a capacitor consists of two parallel metal plates separated by a small
  • 6.
    How to energizea capacitor? The capacitor is energized by connecting the plates to the two terminals of a battery or other sources of potential difference
  • 7.
    When this connection ismade, charges are removed from one of the plates, leaving the plate with a
  • 8.
    •An equal andopposite amount of charge accumulates on the other plate. Charge transfer between the plates stops when the potential difference between the plates is equal to the potential difference between the terminals
  • 9.
    Capacitance -is defined asthe ratio of the net charge on each plate to the potential difference created by the separated charges.
  • 11.
    The SI unitfor capacitance is the farad, F, which is equivalent to a coulomb per volt (C/V). In practice, most typical capacitors have capacitances ranging from microfarads (1 µF = 1 × 10−6 F) to picofarads (1 pF = 1 × 10−12 F).
  • 12.
    Capacitance depends onthe size and shape of the capacitor The capacitance of a parallel-plate capacitor with no material between its plates is given by the following expression:
  • 15.
    The capacitance ofa sphere increases as the size of the sphere increases.
  • 16.
    The material betweena capacitor’s plates can change its capacitance -So far, we have assumed that the space between the plates of a parallel-plate capacitor is a vacuum. However, in many parallel-plate capacitors, the space is filled with a material called a dielectric.
  • 17.
    dielectric -is aninsulating material, such as air, rubber, glass, or waxed paper. When a dielectric is inserted between the plates of a capacitor, the capacitance increases.
  • 18.
    The capacitance increasesbecause the molecules in a dielectric can align with the applied electric field, causing an excess negative charge near the surface of the dielectric at the positive plate and an excess positive charge near the surface of the dielectric at the negative plate.
  • 19.
    According to the expression: Q= C∆V, if the charge increases and the potential difference is constant, the
  • 20.
    -A capacitor witha dielectric can store more charge and energy for a given potential difference than the same capacitor
  • 21.
    ENERGY AND CAPACITORS Theelectrical potential energy stored in a capacitor that is charged from zero to some charge, Q, is given by the following expression: *Note that this equation is also an expression for the work required to charge the capacitor.
  • 22.
    •By substituting thedefinition of capacitance (C = Q/∆V), we can see that these alternative forms are also valid: •PEelectric = 1/2 C(∆V)2 •PEelectric = Q2/ 2C
  • 24.
    To determine thepotential energy, use the alternative form of the equation for the potential energy of a charged capacitor:
  • 25.
    SOLVE: A 4.00 µFcapacitor is connected to a 12.0 V battery. a. What is the charge on each plate of the capacitor? b. If this same capacitor is connected to a 1.50 V battery, how much electrical potential energy is stored?
  • 26.
    ANSWERS: a. 4.80 ×10 −5 C b. 4.50 × 10 −6 J
  • 27.
  • 28.
  • 29.