Title: Capacitance
1Chapter 26
- Capacitance
- and
- Dielectrics
2Capacitance
- The capacitance, C, is a measure of the amount of
electric charge stored (or separated) for a given
electric potential - SI unit Farad (F) 1 F 1 C / V
- A 1 Farad capacitance is very large µF or pF
capacitances are more common
3Capacitor
- A capacitor is a device used in a variety of
electric circuits to store electric charge - Capacitance of a capacitor is the ratio of the
magnitude of the charge on either conductor
(plate) to the magnitude of the potential
difference between the conductors (plates) - This capacitance of a device depends on the
geometric arrangement of the conductors
4Parallel-Plate Capacitor
- This capacitor consists of two parallel plates
(each of area A) separated by a distance d each
carrying equal and opposite charges - Each plate is connected to a terminal of the
battery - The battery is a source of potential difference
- If the capacitor is initially uncharged, the
battery establishes an electric field in the
connecting wires
5Parallel-Plate Capacitor
- The field applies a force on electrons in the
wire just outside of the plates, causing the
electrons to move onto the negative plate until
equilibrium is achieved - The plate, the wire and the terminal are all at
the same potential, and there is no field present
in the wire and the movement of the electrons
ceases - At the other plate, electrons are moving away
from the plate and leaving it positively charged
6Parallel-Plate Capacitor
- The electric field due to one plate
- The total electric field between the plates is
given by - The field outside the plates is zero
7Parallel-Plate Capacitor
- In the final configuration, the potential
difference across the capacitor plates is the
same as that between the terminals of the battery - For a parallel-plate capacitor whose plates are
separated by air
8Electric Field in a Parallel-Plate Capacitor
- The electric field between the plates is uniform
near the center and nonuniform near the edges - The field may be taken as constant throughout the
region between the plates
9Spherical Capacitor
10Chapter 26Problem 5
- An air-filled capacitor consists of two parallel
plates, each with an area of 7.60 cm2, separated
by a distance of 1.80 mm. A 20.0-V potential
difference is applied to these plates. Calculate
(a) the electric field between the plates, (b)
the surface charge density, (c) the capacitance,
and (d) the charge on each plate.
11Electric Circuits
- A circuit is a collection of objects usually
containing a source of electrical energy (such as
a battery) connected to elements that convert
electrical energy to other forms - A circuit diagram a simplified representation
of an actual circuit is used to show the path
of the real circuit - Circuit symbols are used to represent various
elements (e.g., lines are used to represent
wires, batterys positive terminal is indicated
by a longer line)
12Capacitors in Parallel
- When capacitors are first connected in parallel
in the circuit, electrons are transferred from
the left plates through the battery to the right
plates, leaving the left plates positively
charged and the right plates negatively charged - The flow of charges ceases when the voltage
across the capacitors equals that of the battery - The capacitors reach their maximum charge when
the flow of charge ceases
13Capacitors in Parallel
- The total charge is equal to the sum of the
charges on the capacitors Qtotal Q1 Q2 - The potential differences across the capacitors
is the same and each is equal to the voltage of
the battery - A circuit diagram for two
- capacitors in parallel
14Capacitors in Parallel
- The capacitors can be replaced with one capacitor
with a equivalent capacitance Ceq the
equivalent capacitor must have exactly the same
external effect on the circuit as the original
capacitors
15Capacitors in Parallel
- For more than two capacitors in parallel
- The equivalent capacitance of a parallel
combination of capacitors is greater than any of
the individual capacitors
16Capacitors in Series
- When a battery is connected to the circuit,
electrons are transferred from the left plate of
C1 to the right plate of C2 through the battery - As this negative charge accumulates on the right
plate of C2, an equivalent amount of negative
charge is removed from the left plate of C2,
leaving it with an excess positive charge - All of the right plates gain charges of Q and
all the left plates have charges of Q
17Capacitors in Series
- An equivalent capacitor can be found that
performs the same function as the series
combination - The potential differences add up to the battery
voltage
18Capacitors in Series
- For more than two capacitors in series
- The equivalent capacitance is always less than
any individual capacitor in the combination
19Problem-Solving Strategy
- Be careful with the choice of units
- Combine capacitors
- When two or more unequal capacitors are connected
in series, they carry the same charge, but the
potential differences across them are not the
same - The capacitances add as reciprocals and the
equivalent capacitance is always less than the
smallest individual capacitor
20Problem-Solving Strategy
- Be careful with the choice of units
- Combine capacitors
- When two or more capacitors are connected in
parallel, the potential differences across them
are the same - The charge on each capacitor is proportional to
its capacitance - The capacitors add directly to give the
equivalent capacitance
21Problem-Solving Strategy
- Redraw the circuit and continue
- Repeat the process until there is only one single
equivalent capacitor - To find the charge on, or the potential
difference across, one of the capacitors, start
with your final equivalent capacitor and work
back through the circuit reductions
22Equivalent Capacitance
23Chapter 26Problem 25
- Find the equivalent capacitance between points a
and b in the combination of capacitors shown in
the figure
24Energy Stored in a Capacitor
- Before the switch is closed, the energy is stored
as chemical energy in the battery - When the switch is closed, the energy is
transformed from chemical to electric potential
energy - The electric potential energy is related to the
separation of the positive and negative charges
on the plates - A capacitor can be described as a device that
stores energy as well as charge
25Energy Stored in a Capacitor
- Assume the capacitor is being charged and, at
some point, has a charge q on it - The work needed to transfer a charge from one
plate to the other - The total work required
- The work done in charging the capacitor appears
as electric potential energy U
26Energy Stored in a Capacitor
- This applies to a capacitor of any geometry
- The energy stored increases as the charge
increases and as the potential difference
increases - The energy can be considered to be stored in the
electric field - For a parallel-plate capacitor, the energy can be
expressed in terms of the field as U ½ (eoAd)E2
27Capacitors with Dielectrics
- A dielectric is an insulating material (e.g.,
rubber, plastic, etc.) - When placed between the plates of a capacitor, it
increases the capacitance C ? Co ? eo (A/d) - ? - dielectric constant
- The capacitance is
- multiplied by the factor ?
- when the dielectric
- completely fills the region
- between the plates
28Capacitors with Dielectrics
- Tubular metallic foil interlaced with thin
sheets of paraffin-impregnated paper rolled into
a cylinder - Oil filled (for high-V capacitors) interwoven
metallic plates are immersed in silicon oil - Electrolytic (to store large amounts of charge at
relatively low voltages) electrolyte is a
solution that conducts electricity via motion of
ions in the solution
29Dielectric Strength
- For any given plate separation, there is a
maximum electric field that can be produced in
the dielectric before it breaks down and begins
to conduct - This maximum electric field is called the
dielectric strength
30(No Transcript)
31Chapter 26Problem 37
- Determine (a) the capacitance and (b) the maximum
voltage that can be applied to a Teflon-filled
parallel-plate capacitor having a plate area of
175 cm2 and an insulation thickness of 0.040 0 mm.
32Electric Dipole
- An electric dipole consists of two charges of
equal magnitude and opposite signs separated by
2a - The electric dipole moment p is directed along
the line joining the charges from q to q and
has a magnitude of p 2aq - Assume the dipole is placed in a uniform field,
external to the dipole (it is not the field
produced by the dipole) and makes an angle ? with
the field - Each charge has a force of F Eq acting on it
33Electric Dipole
- The net force on the dipole is zero
- The forces produce a net torque on the dipole
- t 2Eqa sin ? pE sin ?
- The torque can also be expressed as the cross
product of the moment and the field - The potential energy can be expressed as
34An Atomic Description of Dielectrics
- Molecules are said to be polarized when a
separation exists between the average position of
the negative charges and the average position of
the positive charges - Polar molecules are those in which this condition
is always present - Molecules without a permanent polarization are
called nonpolar molecules - The average positions of the positive and
negative charges act as point charges, thus polar
molecules can be modeled as electric dipoles
35An Atomic Description of Dielectrics
- A linear symmetric molecule has no permanent
polarization (a) - Polarization can be induced by placing the
molecule in an electric field (b) - Induced polarization is the effect that
predominates in most materials used as
dielectrics in capacitors
36An Atomic Description of Dielectrics
- The molecules that make up the dielectric are
modeled as dipoles in the absence of an electric
field they are randomly oriented - An external electric field produces a torque on
the molecules partially aligning them with the
electric field
37An Atomic Description of Dielectrics
- The presence of the positive (negative) charge on
the dielectric effectively induces some of the
negative (positive) charge on the metal - This allows more charge on the plates for a given
applied voltage and the capacitance increases
38- Answers to Even Numbered Problems
- Chapter 26
- Problem 12
- 17.0 µF
- 9.00V
- 45.0 µC and 108 µC
39- Answers to Even Numbered Problems
- Chapter 26
- Problem 36
- 13.3 nC
- 272 nC
40Answers to Even Numbered Problems Chapter 26
Problem 50 (b) 40.0 µF (c) 6.00 V across 50
µF with charge 300 µF 4.00 V across 30 µF with
charge 120 µF 2.00 V across 20 µF with charge 40
µF 2.00 V across 40 µF with charge 80 µF