Date post: | 20-Dec-2015 |
Category: |
Documents |
View: | 217 times |
Download: | 3 times |
Capacitance
Physics 102Professor Lee
CarknerLecture 12
At which times do you have a final (select all that apply)?
(These are the times for multi-section finals, don’t answer if you don’t have a final at any of these times.)
A) Monday 6-8pmB) Tuesday 6-8 pmC) Wednesday 6-8 pmD) Wednesday 3-5 pmE) Thursday 3-5 pmF) I have a multi-section final, but I don’t know when
PAL #11 Potential
Find potential 1 meter and 5 meters away from -7.00nC charge
V = kQ/r V1 = (8.99X109)(7X10-9)/1 = 62.93 V
V5 = (8.99X109)(7X10-9)/5 = 12.59 V
Change in potential energy between the two points
V = 62.93-12.59 = 50.34 V PE = qV = (1.6X10-19)(50.34) = 8.05X10-18 J
PAL #11 Potential
What is energy and velocity at 1 meter? Negative charge repels negative charge, so
electron slows down KEf = KEi - PE
KEi = ½mv2 = (0.5)(9.1X10-31)(8.77X106)2 = 3.50X10-17 J
KEf = 3.50X10-17 – 8.05X10-18 = 2.7X10-17 J
v = (2KEf/m)½ = [(2)(2.7X10-17)/(9.1X10-31)]½ = 7.7X106 m/s
PAL #11 Potential
(Optional part b) What is initial speed a long distance away?
For large distance away, V = 0 V = 12.95-0 = 12.95 V (between 5 meters and
very far away) PE = qV = (1.6X10-19)(12.95) = 2.07X10-18 J Energy at gun is equal to the energy at 5 meters plus
this PE
KEf = 3.50X10-17 + 2.07X10-18 = 3.71X10-17 J v = [(2)(3.71X10-17)/(9.1X10-31)]½ = 9.03X106
m/s
Equipotentials
Each line represents one value of V Particles moving along an
equipotential do not gain or lose energy
Equipotentials cannot cross
Blue = field = E
Dashed = potential = V
Capacitance A capacitor is a device that can store
charge and thus energy
The amount of charge depends on the potential difference across the capacitor and the intrinsic properties of the device This intrinsic property is called capacitance
and is represented by C
Capacitance Defined The amount of charge stored by a capacitor is just:
Q = C V Or, defining the capacitance:
C = Q/V
The units of capacitance are farads (F)1 F = 1 C/V
Typical capacitances are much less than a farad:
e.g. microfarad = F = 1 X 10-6 F
Capacitor Info A capacitor generally consists of two parallel metal
plates
Consider a battery connected across two metal plates
Electrons are attracted to the positive terminal and are lost by the second plate
Plates can’t touch or charge would move together and
cancel out
Capacitor Diagram
--
+ +V VQ
Capacitor Properties The capacitance depends
on four things:
The distance between them (d)
The dielectric constant of the material between the plates ()
The permittivity of free
space (0) A constant: 0 = 8.85 X 10-12
C2/N m2
C = 0(A/d)
Dielectrics in Capacitors
The properties of the material between the plates is important
The polarized material partially cancels out the electric field between the plates
Dielectrics
The dielectric reduces the effective voltage
A dielectric allows a capacitor to store more charge with the same voltage
The dielectric also allows you to move the plates closer together without touching
Breakdown The dielectric must be an insulator
If the voltage is large enough, the charge will jump across anyway
While Q = CV, there is a limit to how much we can increase Q by increasing V
Normally about 20 million volts
Energy in a Capacitor
Every little batch of charge increases the potential difference between the plates and increases the work to move the next batch
Charge stops moving when the V across the plates is equal to the max V possible for the circuit
Total Energy
Energy = 1/2 Q V =1/2 C (V)2 = Q2/2C since Q = C V
At very large V the capacitor will discharge by itself
Using Capacitors Capacitors store energy Generally only for short periods of time
Useful when you need a quick burst of energy
For a flash, capacitor is discharged into a gas (like xenon) that will glow when ionized
Since capacitance depends on d, can also use capacitance to measure separation
Next Time
Exam #2 Bring calculator and pencil For Monday January 12
Read 18.1-18.5, 18.8-18.9 Homework Ch 18, P: 3, 4, 26, 27
PAL #13 Capacitors 0.005 C stored on capacitor at 1000 volts What is capacitance?
Q= CV C = Q/V = 0.005/1000 = 5X10-6 F = 5 F
Jury-rig a replacement out of metal foil and Teflon coating (k = 2.1, thickness = 0.01 mm). C = 0A/d A = Cd/0 = (5X10-6)(0.00001)/(2.1)(8.85X10-12) A = 2.69 m2
How can such a device be portable? Roll it up, making sure the foil won’t short
Electric Potential Chart
sign of U sign of V sign of W naturally?
+ charge moves with E field
+ charge moves against E field
-charge moves with E field
-charge moves against E field
--
--
-
-+
++
+
++ Yes
Yes
No
No
When a charge +Q is placed at the corner of a square the potential at the center is 3 volts. What is the potential at the center if charges of +Q are placed on all corners of the square?
A) 0 VB) 3 VC) 9 VD) 12 VE) 24 V
If a positive charge moves with the field,
A) PE increases, V decreases, Work positiveB) PE increases, V decreases, Work negativeC) PE increases, V increases, Work negativeD) PE decreases, V increases, Work positiveE) PE decreases, V decreases, Work positive
If a positive charge moves against the field,
A) PE increases, V decreases, Work positiveB) PE increases, V decreases, Work negativeC) PE increases, V increases, Work negativeD) PE decreases, V increases, Work positiveE) PE decreases, V decreases, Work positive
If a negative charge moves with the field,
A) PE increases, V decreases, Work positiveB) PE increases, V decreases, Work negativeC) PE increases, V increases, Work negativeD) PE decreases, V increases, Work positiveE) PE decreases, V decreases, Work positive
If a negative charge moves against the field,
A) PE increases, V decreases, Work positiveB) PE increases, V decreases, Work negativeC) PE increases, V increases, Work negativeD) PE decreases, V increases, Work positiveE) PE decreases, V decreases, Work positive
If a charged particle moves along an equipotential line (assuming no other forces),
A) Its potential energy does not change
B) No work is doneC) Its kinetic energy does not changeD) Its velocity does not changeE) All of the above