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Chapter 23
Circuits
Topics:
• Circuits containing
•
•
•
multiple elements
Series and parallel
combinations
Complex Multi-loop
Circuits
RC circuits
Sample question:
An electric eel can develop a potential difference of over 600 V. How
do the cells of the electric eel’s body generate such a large potential
difference?
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 23-1
RC Circuits
•
•
•
RC circuits are circuits containing resistors
and capacitors.
In RC circuits, the current varies with time.
The values of the resistance and the
capacitance in an RC circuit determine the
time it takes the capacitor to charge or
discharge.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
RC Circuits
The current and the
capacitor voltage decay to
zero after the switch
closes, but not linearly.
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RC Circuits
The decays of the voltage and the current
are exponential decays:
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
RC Circuits
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
QuickCheck
• The following circuits contain capacitors
that are charged to 5.0 V. All of the
switches are closed at the same time.
After 1 second has passed, which
capacitor is charged to the highest
voltage?
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
QuickCheck
Which capacitor discharges more quickly after the
switch is closed?
A. Capacitor A
B. Capacitor B
C. They discharge at
the same rate.
D. We can’t say without
knowing the initial
amount of charge.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Charging a Capacitor
•
•
•
In a circuit that charges a
capacitor, once the switch is
closed, the potential difference
of the battery causes a current
in the circuit, and the capacitor
begins to charge.
As the capacitor charges, it develops a
potential difference that opposes the current,
so the current decreases, and so does the rate
of charging.
The capacitor charges until ΔVC = ℇ.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Charging a Capacitor
• The equations that describe the capacitor
voltage and the current as a function of
time are
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Tau = RC
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Slide 23-29
Capacitor behavior while charging
Before Switch is thrown
After Capacitor is charged
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Additional Clicker Questions
2. In the circuit shown below, the switch is initially closed and the
bulb glows brightly. When the switch is opened, what happens
to the brightness of the bulb?
A.
B.
C.
D.
E.
The brightness of the bulb is not affected.
The bulb gets dimmer.
The bulb gets brighter.
The bulb initially brightens, then dims.
The bulb initially dims, then brightens.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 23-39
Answer
2. In the circuit shown below, the switch is initially closed and the
bulb glows brightly. When the switch is opened, what happens
to the brightness of the bulb?
B. The bulb gets dimmer.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 23-40
•
QuickCheck 23.26
The red curve shows how the capacitor
charges after the switch is closed at t = 0.
Which curve shows the capacitor charging if
the value of the resistor is reduced?
B
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
•
QuickCheck 23.26
The red curve shows how the capacitor
charges after the switch is closed at t = 0.
Which curve shows the capacitor charging if
the value of the resistor is reduced?
B
Smaller time constant.
Same ultimate amount
of charge.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Nuclear Decay and Half-Lives
•
•
•
•
If you start with N0 unstable nuclei, after an interval of time called
the half-life, you’ll have ½ N0 nuclei remaining.
The half-life t1/2 is the average time required for one-half the nuclei
to decay.
The number of nuclei N remaining at time t is
No matter how many nuclei there are at any point in time, the
number decays by half during the next half-life.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Nuclear Decay and HalfLives
• The figure shows the decay of a sample
of radioactive nuclei.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Nuclear Decay and Half-Lives
• The number of
radioactive atoms
decreases
exponentially with
time.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
QuickCheck
A sealed box is completely evacuated (perfect
vacuum),
then 1,000,000 radioactive atoms are added. Their halflife is 2 days. After 4 days have passed, how many
atoms are in the box?
A. 1,000,000
B. 500,000
C. 250,000
D.
0
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Nuclear Decay and Half-Lives
• The decay of radioactive nuclei is an
exponential decay.
• The equation for the number of atoms
after a half-life can be written in terms of
a time constant τ that is related to the
half-life:
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Chapter 24
Magnetic Fields and Forces
Topics:
• Magnets and the magnetic
•
•
•
•
field
Electric currents create
magnetic fields
Magnetic fields of wires,
loops, and solenoids
Magnetic forces on charges
and currents
Magnets and magnetic
materials
Sample question:
This image of a patient’s knee was made with magnetic fields, not
x rays. How can we use magnetic fields to visualize the inside of
the body?
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 24-1
3-D Arrows, Cross Products, and Right Hand Rule 1
• Showing vectors in 3D
• Cross Product
C = A´ B
C = A B sin a
For direction use Right-hand rule 1
• Right-hand rule 1 (RHR 1)C = A ´ B
=> for finding direction of cross-product vector
(Cross-Product Rule)
1. Point right hand in the direction of the first vector (vector A)
2. Rotate your right hand until you can point your fingers in the
direction of the second vector (vector B)
3. Thumb points in direction the cross-product vector (vector C)
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 24-2
Electric vs. Magnetic Interactions
1. Nature of Magnetic Interactions
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Slide 24-2
Discovering Magnetism
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Slide 24-6
The Magnetic Field
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Slide 24-7
Mapping Out the Field of a Bar Magnet
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Slide 24-8
Mapping Out the Magnetic Field Using Iron Filings
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Slide 24-9
Drawing Field Lines of a Bar Magnet
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Slide 24-10
Magnetic Fields Produced by Bar Magnets
A single bar magnet
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A single bar magnet
(closeup)
Slide 24-11
Magnetic Fields Produced by Bar Magnets
Two bar magnets,
unlike poles facing
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Two bar magnets,
like poles facing
Slide 24-12
Checking Understanding
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Slide 24-13
Magnetic Fields from Two Magnets
Bar Magnets A and B are placed at right angles. Two compasses, X and Y are placed so
that they are equidistant from the two magnets as shown
A.) The arrow in compass X indicates the direction
in which the North pole of the compass is pointing.
Indicate the North and South ends of both magnets
in the diagram
B.) Draw an arrow in compass Y to show the direction
in which the North pole of the compass needle
would point.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 24-2
Magnetic Fields Around Us
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Slide 24-14
Key Points
• Three types of magnetic interactions
1. no interaction with either pole of a magnet
=> object is non-magnetic
2. attracted to both poles of a magnet
=> object is magnetic
3. Attracted to one pole and repelled by the other pole
=> object is a magnet
• Magnetic field vector from a bar magnet is a super position of
the magnetic field vectors from the N and S poles:
•
•
Vector from N pole points away from N pole
Vector from S pole points towards S pole
• Field lines form complete loops inside and outside of magnet
•
•
•
Field lines outside magnet go from N to S poles
Field lines inside magnet go from S to N poles
Magnetic Field vectors at a point are tangential to Magnetic Field Lines
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Electric Currents Also Create Magnetic Fields
A long, straight
wire
A current loop
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A solenoid
Slide 24-15
The Magnetic Field of a Straight Current-Carrying Wire
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Slide 24-16
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Slide 24-17
Representing Vectors and Currents That Are
Perpendicular to the Page
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Slide 24-18
Checking Understanding
Point P is 5 cm above the wire as you look straight down at
it. In which direction is the magnetic field at P?
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Slide 24-19
Answer
Point P is 5 cm above the wire as you look straight down at
it. In which direction is the magnetic field at P?
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 24-20
Drawing Field Vectors and Field Lines of a
Current-Carrying Wire
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Slide 24-21
Drawing a Current Loop
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Slide 24-22
The Magnetic Field of a Current Loop
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Slide 24-23
The Magnetic Field of a Solenoid
A short solenoid
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A long solenoid
Slide 24-24
The Magnitude of the Field due to a Long, Straight,
Current-Carrying Wire
m0 I
B=
2p r
m0 = permeability constant = 1.257 ´ 10 T× m/A
-6
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Slide 24-25
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 24-26
Checking Understanding
The magnetic field at point P is zero. What are the magnitude
and direction of the current in the lower wire?
A. 10 A to the right.
B. 5 A to the right.
C. 2.5 A to the right.
D. 10 A to the left.
E. 5 A to the left.
F. 2.5 A to the left.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley.
Slide 24-27
Answer
The magnetic field at point P is zero. What are the magnitude
and direction of the current in the lower wire?
E. 5 A to the left.
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Slide 24-28