1. General Physics (PHY 2140) Lecture 7
Electrostatics and electrodynamics
Capacitance and capacitors
capacitors with dielectrics
Electric current
current and drift speed
resistance and Ohm’s law
Chapter 16-17
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2. Reminder (for those who don’t read syllabus)
Reading Quizzes (bonus 5%):
It is important for you to come to class prepared, i.e. be familiar with the
material to be presented. To test your preparedness, a simple five-minute
quiz, testing your qualitative familiarity with the material to be discussed in
class, will be given at the beginning of some of the classes. No make-up
reading quizzes will be given.
There could be one today…
… but then again…
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3. Lightning Review Last lecture: Capacitance and capacitors
Parallel-plate capacitor
Combinations of capacitors
Parallel
Series
Energy stored in a capacitor
Review Problem: Consider an isolated simple parallel-plate capacitor whose plates are given equal and opposite charges and are separated by a distance d. Suppose the plates are pulled apart until they are separated by a distance D>d. The electrostatic energy stored in a capacitor is
a. greater then
b. the same as
c. smaller then
before the plates were pulled apart.
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4. 16.10 Capacitors with dielectrics
A dielectrics is an insulating material (rubber, glass, etc.)
Consider an insolated, charged capacitor
Notice that the potential difference decreases (k = V0/V)
Since charge stayed the same (Q=Q0) → capacitance increases
dielectric constant: k = C/C0
Dielectric constant is a material property +Q -Q
Insert a dielectric V0 V
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5. Capacitors with dielectrics - notes
Capacitance is multiplied by a factor k when the dielectric fills the region between the plates completely
E.g., for a parallel-plate capacitor
The capacitance is limited from above by the electric discharge that can occur through the dielectric material separating the plates
In other words, there exists a maximum of the electric field, sometimes called dielectric strength, that can be produced in the dielectric before it breaks down
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6. Dielectric constants and dielectric strengths of various materials at room temperature
Dielectric constant, k
Dielectric strength (V/m)
Vacuum
1.00 --
Air
3 ´106
Water 80
Fused quartz
3.78
9 ´106
For a more complete list, see Table 16.1
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7. Example
Take a parallel plate capacitor whose plates have an area of 2.0 m2 and are separated by a distance of 1mm. The capacitor is charged to an initial voltage of 3 kV and then disconnected from the charging source. An insulating material is placed between the plates, completely filling the space, resulting in a decrease in the capacitors voltage to 1 kV. Determine the original and new capacitance, the charge on the capacitor, and the dielectric constant of the material.
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8. The dielectric constant and the new capacitance are
Take a parallel plate capacitor whose plates have an area of 2 m2 and are separated by a distance of 1mm. The capacitor is charged to an initial voltage of 3 kV and then disconnected from the charging source. An insulating material is placed between the plates, completely filling the space, resulting in a decrease in the capacitors voltage to kV. Determine the original and new capacitance, the charge on the capacitor, and the dielectric constant of the material.
Given:
DV1=3,000 V
DV2=1,000 V
A = 2.00 m2
d = 0.01 m
Find:
C=?
C0=?
Q=?
k=?
Since we are dealing with the parallel-plate capacitor, the original capacitance can be found as
The dielectric constant and the new capacitance are
The charge on the capacitor can be found to be
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9. Reorientation of polar molecules
How does an insulating dielectric material reduce electric fields by producing effective surface charge densities?
Reorientation of polar molecules + - + -
Induced polarization of non-polar molecules + -
Dielectric Breakdown: breaking of molecular bonds/ionization of molecules.
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10. 17.1 Electric Current
Whenever charges of like signs move in a given direction, a current is said to exist.
Consider charges are moving perpendicularly to a surface of area A.
Definition: the current is the rate at which charge flows through this surface. A + I
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11. 17.1 Electric Current - Definition
Given an amount of charge, DQ, passing through the area A in a time interval Dt, the current is the ratio of the charge to the time interval. A + I
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12. 17.1 Electric Current - Units
The SI units of current is the ampere (A).
1 A = 1 C/s
1 A of current is equivalent to 1 C of charge passing through the area in a time interval of 1 s.
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13. 17.1 Electric Current – Remark 1
Currents may be carried by the motion of positive or negative charges.
It is conventional to give the current the same direction as the flow of positive charge.
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14. 17.1 Electric Current – Remark 2
In a metal conductor such as copper, the current is due to the motion of the electrons (negatively charged).
The direction of the current in copper is thus opposite the direction of the electrons. - - v - - I
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15. 17.1 Electric Current – Remark 3
In a beam of protons at a particle accelerator (such as RHIC at Brookhaven national laboratory), the current is the same direction as the motion of the protons.
In gases and electrolytes (e.g. Car batteries), the current is the flow of both positive and negative charges.
                      
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16. 17.1 Electric Current – Remark 4
It is common to refer to a moving charge as a mobile charge carrier.
In a metal the charge carriers are electrons.
In other conditions or materials, they may be positive or negative ions.
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17. 17.1 Electric Current – Example Current in a light bulb
The amount of charge that passes through the filament of a certain light bulb in 2.00 s is 1.67 c. Find.
(A) the current in the light bulb.
(B) the number of electrons that pass through the filament in 1 second.
                                        
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18. The amount of charge that passes through the filament of a certain light bulb in 2.00 s is 1.67 c. Find. (A) the current in the light bulb.
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19. The amount of charge that passes through the filament of a certain light bulb in 2.00 s is 1.67 c. Find. (b) the number of electrons that pass through the filament in 1 second.
Reasoning:
In 1 s, C of charge passes the cross-sectional area of the filament.
This total charge per second is equal to the number of electrons, N, times the charge on a single electron.
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20. The amount of charge that passes through the filament of a certain light bulb in 2.00 s is 1.67 c. Find. (b) the number of electrons that pass through the filament in 1 second. Solution:
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21. 15.2 Current and Drift Speed
Consider the current on a conductor of cross-sectional area A. A vd q
vdDt
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22. 15.2 Current and Drift Speed (2)
Volume of an element of length Dx is : DV = A Dx.
Let n be the number of carriers per unit of volume.
The total number of carriers in DV is: n A Dx.
The charge in this volume is: DQ = (n A Dx)q.
Distance traveled at drift speed vd by carrier in time Dt: Dx = vd Dt.
Hence: DQ = (n A vd Dt)q.
The current through the conductor: I = DQ/ Dt = n A vd q.
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23. 15.2 Current and Drift Speed (3)
In an isolated conductor, charge carriers move randomly in all directions.
When an external potential is applied across the conductor, it creates an electric field inside which produces a force on the electron.
Electrons however still have quite a random path.
As they travel through the material, electrons collide with other electrons, and nuclei, thereby losing or gaining energy.
The work done by the field exceeds the loss by collisions.
The electrons then tend to drift preferentially in one direction.
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24. 15.2 Current and Drift Speed - Example
Question:
A copper wire of cross-sectional area 3.00x10-6 m2 carries a current of 10. A. Assuming that each copper atom contributes one free electron to the metal, find the drift speed of the electron in this wire. The density of copper is 8.95 g/cm3.
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25. n = 6.02x1023 atom/mol x 8.95 g/cm3 x ( 63.5 g/mol)-1
Question:
A copper wire of cross-sectional area 3.00x10-6 m2 carries a current of 10 A. Assuming that each copper atom contributes one free electron to the metal, find the drift speed of the electron in this wire. The density of copper is 8.95 g/cm3.
Reasoning: We know:
A = 3.00x10-6 m2
I = 10 A.
r = 8.95 g/cm3.
q = 1.6 x C.
n = 6.02x1023 atom/mol x 8.95 g/cm3 x ( 63.5 g/mol)-1
n = 8.48 x 1022 electrons/ cm3.
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26. A = 3.00x10-6 m2 ; I = 10 A.; r = 8.95 g/cm3.; q = 1.6 x 10-19 C.
Question:
A copper wire of cross-sectional area 3.00x10-6 m2 carries a current of 10 A. Assuming that each copper atom contributes one free electron to the metal, find the drift speed of the electron in this wire. The density of copper is 8.95 g/cm3.
Ingredients:
A = 3.00x10-6 m2 ; I = 10 A.; r = 8.95 g/cm3.; q = 1.6 x C.
n = 8.48 x 1022 electrons/ cm3.
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27. 15.2 Current and Drift Speed - Comments
Drift speeds are usually very small.
Drift speed much smaller than the average speed between collisions.
Electrons traveling at 2.46x10-6 m/s would would take 68 min to travel 1m.
So why does light turn on so quickly when one flips a switch?
The info travels at roughly 108 m/s…
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28. Mini-quiz
Consider a wire has a long conical shape. How does the velocity of the electrons vary along the wire?
Every portion of the wire carries the same current: as the cross sectional area decreases, the drift velocity must increase to carry the same value of current. This is dues to the electrical field lines being compressed into a smaller area, thereby increasing the strength of the electric field.
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29. 17.3 Resistance and Ohm’s Law - Intro
When a voltage (potential difference) is applied across the ends of a metallic conductor, the current is found to be proportional to the applied voltage. DV I
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30. 17.3 Definition of Resistance
In situations where the proportionality is exact, one can write.
The proportionality constant R is called resistance of the conductor.
The resistance is defined as the ratio.
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31. 17.3 Resistance - Units
In SI, resistance is expressed in volts per ampere.
A special name is given: ohms (W).
Example: if a potential difference of 10 V applied across a conductor produces a 0.2 A current, then one concludes the conductors has a resistance of 10 V/0.2 a = 50 W.
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32. 17.3 Ohm’s Law Georg Simon Ohm (1787-1854)
Resistance in a conductor arises because of collisions between electrons and fixed charges within the material.
In many materials, including most metals, the resistance is constant over a wide range of applied voltages.
This is a statement of Ohm’s law.
Georg Simon Ohm ( )
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33. Linear or Ohmic Material
Non-Linear or
Non-Ohmic Material
Linear or Ohmic Material I I DV DV
Semiconductors
e.g. diodes
Most metals, ceramics
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34. Ohm’s Law
R understood to be independent of DV.
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35. The symbol for a resistor in circuit diagrams.
Definition:
Resistor: a conductor that provides a specified resistance in an electric circuit.
The symbol for a resistor in circuit diagrams.
       
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36. Example: Resistance of a Steam Iron
All household electric devices are required to have a specified resistance (as well as many other characteristics…). Consider that the plate of a certain steam iron states the iron carries a current of 7.40 A when connected to a 120 V source. What is the resistance of the steam iron?
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