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Energy Storage Devices
Objective of Lecture
Describe the construction of a capacitor and how
charge is stored.
Introduce several types of capacitors
Discuss the electrical properties of a capacitor
The relationship between charge, voltage, and
capacitance
 Charging and discharging of a capacitor
Relationship between voltage, current, and capacitance;
power; and energy
Equivalent capacitance when a set of capacitors are in
series and in parallel
Capacitors
Basic capacitor construction
Dielectric
material
Plate 1
Plate 2
The dielectric
material is an
insulator therefore
no current flows
through the
capacitor
Capacitors
Composed of two conductive plates separated by an
insulator (or dielectric).
Commonly illustrated as two parallel metal plates
separated by a distance, d.
C = ε A/d
where ε = εr εo
εr is the relative dielectric constant
εo is the vacuum permittivity
Effect of Dimensions
Capacitance increases with
increasing surface area of the plates,
decreasing spacing between plates, and
increasing the relative dielectric constant of the
insulator between the two plates.
Types of Capacitors
Fixed Capacitors
Nonpolarized
 May be connected into circuit with either terminal of
capacitor connected to the high voltage side of the circuit.
 Insulator: Paper, Mica, Ceramic, Polymer
Electrolytic
 The negative terminal must always be at a lower voltage than
the positive terminal
 Plates or Electrodes: Aluminum, Tantalum
Nonpolarized
Difficult to make nonpolarized capacitors that store a
large amount of charge or operate at high voltages.
Tolerance on capacitance values is very large
 +50%/-25% is not unusual
http://www.marvac.com/fun/ceramic_capacitor_codes.a
spx
PSpice Symbol
Electrolytic
Pspice Symbols Fabrication
http://www.digitivity.com/articles/2008/11/choosing-the-right-
capacitor.html
Variable Capacitors
Cross-sectional area is changed as one set of plates
are rotated with respect to the other.
http://www.tpub.com/neets/book2/3f.htm
PSpice Symbol
MEMS Capacitor
MEMS (Microelectromechanical system)
Can be a variable capacitor by changing the distance
between electrodes.
Use in sensing applications as well as in RF electronics.
http://www.silvaco.com/tech_lib_TCAD/simulationstandard/2005/aug/a3/a3.html
Electric Double Layer Capacitor
Also known as a supercapacitor or ultracapacitor
Used in high voltage/high current applications.
 Energy storage for alternate energy systems.
http://en.wikipedia.org/wiki/File:Supercapacitor_diagram.svg
Electrical Properties of a Capacitor
Acts like an open circuit at steady state when
connected to a d.c. voltage or current source.
Voltage on a capacitor must be continuous
There are no abrupt changes to the voltage, but there
may be discontinuities in the current.
An ideal capacitor does not dissipate energy, it takes
power when storing energy and returns it when
discharging.
Energy Storage
Charge is stored on the plates of the capacitor.
Equation:
Q = CV
Units:
Farad = Coulomb/Voltage
Farad is abbreviated as F
Sign Conventions
• The sign convention used with a
capacitor is the same as for a power
dissipating device.
• When current flows into the positive side
of the voltage across the capacitor, it is
positive and the capacitor is dissipating
power.
• When the capacitor releases energy back
into the circuit, the sign of the current will
be negative.
Charging a Capacitor
At first, it is easy to store charge in the capacitor.
As more charge is stored on the plates of the
capacitor, it becomes increasingly difficult to place
additional charge on the plates.
Coulombic repulsion from the charge already on the
plates creates an opposing force to limit the addition of
more charge on the plates.
 Voltage across a capacitor increases rapidly as charge is
moved onto the plates when the initial amount of charge on
the capacitor is small.
 Voltage across the capacitor increases more slowly as it
becomes difficult to add extra charge to the plates.
Discharging a Capacitor
At first, it is easy to remove charge in the capacitor.
Coulombic repulsion from charge already on the plates
creates a force that pushes some of the charge out of the
capacitor once the force (voltage) that placed the charge in
the capacitor is removed (or decreased).
As more charge is removed from the plates of the
capacitor, it becomes increasingly difficult to get rid of the
small amount of charge remaining on the plates.
Coulombic repulsion decreases as charge spreads out on the
plates. As the amount of charge decreases, the force needed
to drive the charge off of the plates decreases.
 Voltage across a capacitor decreases rapidly as charge is removed
from the plates when the initial amount of charge on the capacitor
is small.
 Voltage across the capacitor decreases more slowly as it becomes
difficult to force the remaining charge out of the capacitor.
Current-Voltage Relationships
∫=
=
=
=
1
1
t
t
CC
C
C
C
C
o
dti
C
v
dt
dv
Ci
dt
dq
i
Cvq
Power and Energy
dt
dv
Cvp
vip
C
CC
CCC
=
=
C
q
w
Cvw
C
CC
2
2
1
2
2
=
=
General Equations for Ceq
Parallel Combination Series Combination
If P capacitors are in parallel,
then
If S capacitors are in series,
then:
1
1
1
−
=






= ∑
S
s s
eq
C
C∑=
=
P
p
Peq CC
1

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Capacitors

  • 2. Objective of Lecture Describe the construction of a capacitor and how charge is stored. Introduce several types of capacitors Discuss the electrical properties of a capacitor The relationship between charge, voltage, and capacitance  Charging and discharging of a capacitor Relationship between voltage, current, and capacitance; power; and energy Equivalent capacitance when a set of capacitors are in series and in parallel
  • 3. Capacitors Basic capacitor construction Dielectric material Plate 1 Plate 2 The dielectric material is an insulator therefore no current flows through the capacitor
  • 4. Capacitors Composed of two conductive plates separated by an insulator (or dielectric). Commonly illustrated as two parallel metal plates separated by a distance, d. C = ε A/d where ε = εr εo εr is the relative dielectric constant εo is the vacuum permittivity
  • 5. Effect of Dimensions Capacitance increases with increasing surface area of the plates, decreasing spacing between plates, and increasing the relative dielectric constant of the insulator between the two plates.
  • 6. Types of Capacitors Fixed Capacitors Nonpolarized  May be connected into circuit with either terminal of capacitor connected to the high voltage side of the circuit.  Insulator: Paper, Mica, Ceramic, Polymer Electrolytic  The negative terminal must always be at a lower voltage than the positive terminal  Plates or Electrodes: Aluminum, Tantalum
  • 7. Nonpolarized Difficult to make nonpolarized capacitors that store a large amount of charge or operate at high voltages. Tolerance on capacitance values is very large  +50%/-25% is not unusual http://www.marvac.com/fun/ceramic_capacitor_codes.a spx PSpice Symbol
  • 9. Variable Capacitors Cross-sectional area is changed as one set of plates are rotated with respect to the other. http://www.tpub.com/neets/book2/3f.htm PSpice Symbol
  • 10. MEMS Capacitor MEMS (Microelectromechanical system) Can be a variable capacitor by changing the distance between electrodes. Use in sensing applications as well as in RF electronics. http://www.silvaco.com/tech_lib_TCAD/simulationstandard/2005/aug/a3/a3.html
  • 11. Electric Double Layer Capacitor Also known as a supercapacitor or ultracapacitor Used in high voltage/high current applications.  Energy storage for alternate energy systems. http://en.wikipedia.org/wiki/File:Supercapacitor_diagram.svg
  • 12. Electrical Properties of a Capacitor Acts like an open circuit at steady state when connected to a d.c. voltage or current source. Voltage on a capacitor must be continuous There are no abrupt changes to the voltage, but there may be discontinuities in the current. An ideal capacitor does not dissipate energy, it takes power when storing energy and returns it when discharging.
  • 13. Energy Storage Charge is stored on the plates of the capacitor. Equation: Q = CV Units: Farad = Coulomb/Voltage Farad is abbreviated as F
  • 14. Sign Conventions • The sign convention used with a capacitor is the same as for a power dissipating device. • When current flows into the positive side of the voltage across the capacitor, it is positive and the capacitor is dissipating power. • When the capacitor releases energy back into the circuit, the sign of the current will be negative.
  • 15. Charging a Capacitor At first, it is easy to store charge in the capacitor. As more charge is stored on the plates of the capacitor, it becomes increasingly difficult to place additional charge on the plates. Coulombic repulsion from the charge already on the plates creates an opposing force to limit the addition of more charge on the plates.  Voltage across a capacitor increases rapidly as charge is moved onto the plates when the initial amount of charge on the capacitor is small.  Voltage across the capacitor increases more slowly as it becomes difficult to add extra charge to the plates.
  • 16. Discharging a Capacitor At first, it is easy to remove charge in the capacitor. Coulombic repulsion from charge already on the plates creates a force that pushes some of the charge out of the capacitor once the force (voltage) that placed the charge in the capacitor is removed (or decreased). As more charge is removed from the plates of the capacitor, it becomes increasingly difficult to get rid of the small amount of charge remaining on the plates. Coulombic repulsion decreases as charge spreads out on the plates. As the amount of charge decreases, the force needed to drive the charge off of the plates decreases.  Voltage across a capacitor decreases rapidly as charge is removed from the plates when the initial amount of charge on the capacitor is small.  Voltage across the capacitor decreases more slowly as it becomes difficult to force the remaining charge out of the capacitor.
  • 19. General Equations for Ceq Parallel Combination Series Combination If P capacitors are in parallel, then If S capacitors are in series, then: 1 1 1 − =       = ∑ S s s eq C C∑= = P p Peq CC 1