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Reading Quiz
1. What quantity is
represented by
the symbol ?
A.
B.
C.
D.
E.
Electronic potential
Excitation potential
EMF
Electric stopping power
Exosphericity
2. What is the SI unit of
capacitance?
A. Capaciton
B. Faraday
C. Hertz
D. Henry
E. Exciton
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
3. The electric field
4. This chapter investigated
A. is always perpendicular to an
equipotential surface.
B. is always tangent to an
equipotential surface.
C. always bisects an equipotential
surface.
D. makes an angle to an
equipotential surface that
depends on the amount of
charge.
A.
B.
C.
D.
E.
parallel capacitors
perpendicular capacitors
series capacitors.
Both a and b.
Both a and c.
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
What quantity is represented by
the symbol ?
A. Electronic potential
B. Excitation potential
C. EMF
D. Electric stopping power
E. Exosphericity
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
What is the SI unit of capacitance?
A. Capaciton
B. Faraday
C. Hertz
D. Henry
E. Exciton
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
The electric field
A. is always perpendicular to an
equipotential surface.
B. is always tangent to an
equipotential surface.
C. always bisects an equipotential
surface.
D. makes an angle to an equipotential
surface that depends on the amount
of charge.
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
This chapter investigated
A.
B.
C.
D.
E.
parallel capacitors
perpendicular capacitors
series capacitors.
Both a and b.
Both a and c.
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
Finding the Potential from the Electric Field
The potential difference between two points in space is
where s is the position along a line from point i to point f.
That is, we can find the potential difference between two
points if we know the electric field.
We can think of an integral as an area under a curve. Thus a
graphical interpretation of the equation above is
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
EXAMPLE 30.2 The potential of a parallelplate capacitor
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
EXAMPLE 30.2 The potential of a parallelplate capacitor
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
EXAMPLE 30.2 The potential of a parallelplate capacitor
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
Finding the Electric Field from the Potential
In terms of the potential, the component of the electric field
in the s-direction is
Now we have reversed Equation 30.3 and have a way to
find the electric field from the potential.
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
EXAMPLE 30.4 Finding E from the slope of V
QUESTION:
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
EXAMPLE 30.4 Finding E from the slope of V
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
Exam 1 Review
• Chapters 26 – 30
• Up to and including section 30.4
• The exam won’t cover sections 30.5 to the end of the
chapter
• The exam will cover
• Field lines and surfaces of equipotential for different
charge configurations
• Force and Electric Field of point charges
• Potential and Potential Energy of point charges
• Using Gauss’ Law to determine something about field
or charge
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.
Group Problems
• Start Ch 29 HW
• Chapter 30 HW may be on exam (topics up to and
including those covered in Sections 30.1 – 30.4)
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.