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1 Lecture 7.1 : Current and Resistance Lecture Outline: Current and Current Density Conductivity and Resistivity Resistance and Ohm’s Law Feb. 25, 2014 Textbook Reading: Ch. 30.3 - 30.5
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Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

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Page 1: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

1

Lecture 7.1 :Current and Resistance

Lecture Outline:Current and Current DensityConductivity and ResistivityResistance and Ohm’s Law

Feb. 25, 2014

Textbook Reading:Ch. 30.3 - 30.5

Page 2: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Announcements

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•Homework #7 is now posted. Due next Tue., March 4, at 9am.

•Optional review session for Exam #2 is scheduled for Tue., March 4, from 5-7pm in Stolkin. Bring your clickers.

Page 3: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Last Lecture...

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Conduction electrons are like free particles moving through a metal lattice.

No Electric FieldAverage Velocity is Zero

With Electric FieldAverage Velocity is NonZero

Page 4: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Last Lecture...

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Electrons are the charge carriers in metals!

electron current (ie) = number of electrons per second that pass through a conductor in a given time.

ie = neA�d =nee⇥A

mE

Page 5: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Clicker Question #1

5

A wire carries a current. If both the wire diameter and the electron drift speed are doubled, the electron current increases by a factor of

A. 2.B. 4.C. 6.D. 8.E. Some other value.

ie ∝ Aνd

Page 6: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Current and Current Density

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I � dQ

dt

Current was known long before electrons were discovered, so conventional definition of current is in terms of Charge:

1 ampere = 1 A ≡ 1 coulomb per second = 1 C/s

I =Q

�t=

eNe

�t= eie

Conventional current and electron current are related:

Page 7: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Current and Current Density

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By convention, current is defined to flow in the direction in which

positive charges would move! (i.e. - in the direction of the Electric Field)

Page 8: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Current and Current Density

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We define current density (J) to arrive at a property intrinsic to a material, and not specific to the cross-sectional Area of a conductor.

J � I

A= nee�d

The current in a 100 Watt lightbulb is 0.85 A. The filament inside the bulb is 0.25 mm in diameter. What is the current density in the filament?

Page 9: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Current and Current Density

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Current is a conserved quantity! The current is the same at all points in a current-carrying wire.

Current is not “used up” by the paddle...but energy is required to turn the paddle.

Page 10: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Clicker Question #2

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A and B are identical lightbulbs connected to a battery as shown. Which is brighter?

A. Bulb A.B. Bulb B.C. The bulbs are equally bright.

Page 11: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Current and Current Density

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�Iin =

�Iout

Kirchoff’s Junction Law:

Current = ?

Page 12: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Conductivity and Resistivity

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J = nee�d = nee

�e⇥E

m

⇥=

nee2⇥

mE

J = �E

� = conductivity =nee2⇥

mDefine a new

property of materials

Conductivity describes how easily electrons can move through a material. (Also depends on temperature)

Page 13: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Clicker Question #3

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The current density in this wire is

A. 4 × 106 A/m2.B. 2 × 106 A/m2.C. 4 × 103 A/m2.D. 2 × 103 A/m2.E. Some other value.

Current Density: J = Current/Area = (8A)/(0.002m x 0.002m) = 2x106 A/m2

Which way does the current density vector point?

Page 14: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Clicker Question #4

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Both segments of the wire are made of the same metal. Current I1 flows into segment 1 from the left. How does current I1 in segment 1 compare to current I2 in segment 2?

A. I1 > I2.B. I1 = I2.C. I1 < I2.D. There’s not enough information to

compare them.

Page 15: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Clicker #5

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Both segments of the wire are made of the same metal. Current I1 flows into segment 1 from the left. How does current density J1 in segment 1 compare to current density J2 in segment 2?

A. J1 > J2.B. J1 = J2.C. J1 < J2.D. There’s not enough information to

compare them.

Smaller cross-section area

Page 16: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Conductivity and Resistivity

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� = resistivity =1

⇥=

m

nee2⇤

Inverse of conductivity (resistivity) tells how reluctant electrons are to move through a material.

Page 17: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Resistance and Ohm’s Law

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E =�V

�s=

�V

LI = JA = A⇥E =

A

�E

Potential Difference across conductor creates Electric field.

R = resistanceOhm’s Law: I =

A

�L�V � �V

R

Page 18: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Resistance and Ohm’s Law

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Resistance (R) characterizes ability of current to flow through specific piece of conductor with a specific geometry.

R =�L

A

1 ohm = 1 Ω ≡ 1 Volt/Ampere = 1 V/A

Wire 2 is twice the length and twice the diameter of wire 1. What is the ratio R2/R1 of their resistances?

Page 19: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Conductivity and Resistivity

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Superconductivity!

Some materials exhibit zero resistance to current if they are cooled to low enough temperatures.

Page 20: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Conductivity and Resistivity

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A 3.0 mm diameter wire carries a 12 A current when the electric field is 0.085 V/m. What is the wire’s resistivity?

Page 21: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Resistance and Ohm’s Law

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Ohm’s Law: Establishing a potential difference ΔV across the ends of a conductor with resistance R causes a current I through the current.

I =�V

R

Example: What resistor would have a 15 mA current if connected across the terminals of a 9.0 V battery?

Page 22: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Resistance and Ohm’s Law

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In this course, we will assume wires are ideal (R = 0 Ω ), so they don’t have any potential drop across them.

Real wires have some resistance, and use up some energy in a circuit.

Page 23: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Resistance and Ohm’s Law

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Resistors are placed in electrical circuits to control the voltage at different points in the circuit.

Resistors are made out of materials, such as carbon, that are poor conductors.

Page 24: Lecture 7.1 : Current and ResistanceAnnouncements 2 •Homework #7 is now posted.Due next Tue., March 4, at 9am. •Optional review session for Exam #2 is scheduled for Tue., March

Reminders

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•Homework #7 is now posted.•Come see me if you have any questions or concerns.