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© 2014 Pearson Education, Inc.
Electric Current
and Electric Circuits
Chapter Contents
• Electric Current, Resistance, and Semiconductors
• Electric Circuits
• Power and Energy in Electric Circuits
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• All electric circuits have one thing in
common—they depend on the flow of electric
charge.
• When electric charge flows from one place to
another, we say it forms an electric current. The
more charge that flows, and the faster it flows,
the greater the electric current.
• In general, electric charge is carried through a
circuit by electrons.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• Suppose an amount of charge ΔQ flows past a
given point in a wire in the time Δt. The electric
current, I, in the wire is simply defined as the
amount of charge divided by the amount of time.
• The following equation is used to determine the
current flowing in a wire.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The unit of current is the ampere (A), or amp for
short. It is named for the French physicist
André-Marie Ampère (1775–1836).
• A current of 1 amp is defined as the flow of
1 coulomb of charge in 1 second:
1 A = 1 C/s
• A 1-amp current is fairly strong. Many electronic
devices, like cell phones and digital music players,
operate on currents that are a fraction of an amp.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The following Conceptual Example illustrates
how the current depends on both the amount of
charge flowing and the amount of time.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The following example shows that the number of
electrons flowing in a typical circuit is extremely
large. The situation is similar to the large
number of water molecules flowing through a
garden hose.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
© 2014 Pearson Education, Inc.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• When charge flows through a closed path and
returns to its starting point, we say that the closed
path is an electric circuit.
• In a type of circuit known as a direct-current
circuit, or DC circuit, the current always flows in
the same direction. Circuits that run on batteries
are typically DC circuits.
• Circuits with currents that periodically reverse their
direction are referred to as alternating-current
circuits, or AC circuits. The electricity provided by
a wall plug in your house is AC.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• Although electrons move fairly freely in metal
wires, something has to push on them to get
them going and keep them going. It's like water
in a garden hose; the water flows only when a
force pushes on it. Similarly, electrons flow in a
circuit only when an electrical force pushes on
them.
• Figure (a) below shows
that there is no water
flow if both ends of the
garden hose are held
at the same level.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• Figure (b) shows that water flows from the end where the
gravitational potential energy is high to the end where it is
low. The difference in gravitational potential energy
between the two ends of the hose results in a force on the
water—which in turn produces a flow. A battery performs
a similar function in an electric circuit.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• A battery uses chemical reactions to produce a
difference in electric potential between its two
ends, which are referred to as the terminals. The
symbol for a battery is .
• A battery's positive terminal has a high electrical
potential and is denoted with a plus (+) sign; the
negative terminal has a low electric potential and
is denoted with a minus sign (−).
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• When a battery is connected to a circuit, electrons
move in a closed path from one terminal of the
battery through the circuit and back to the other
terminal of the battery. The electrons leave from
the negative terminal of the battery and return to
the positive terminal.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The situation is similar to the flow of blood in your
body. Your heart acts like a battery, causing blood
to flow through a closed circuit of arteries and
veins in your body.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The figure below shows a simple electrical system
consisting of a battery, a switch, and a lightbulb
connected together in a flashlight.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The circuit diagram in figure (b) below shows that
the switch is open—creating an open circuit.
When a circuit is open, no charge can flow. When
the switch is closed, electrons flow through the
circuit and the light glows.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The figure below shows a mechanical equivalent
of the flashlight circuit. The person lifting the
water corresponds to the battery, the paddle
wheel corresponds to the lightbulb, and the
water is like the electric charge.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The difference in electric potential between the
terminals of the battery is the electromotive force,
or emf. Symbolically, the electromotive force is
represented by the symbol ε (the Greek letter
epsilon). The unit of emf is the same as that of
electrical potential, namely, the volt.
• The electromotive force is not really a force.
Instead, the emf determines the amount of work a
battery does to move a certain amount of charge
around a circuit.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• To be specific, the magnitude of the work done
by a battery with the emf ε as charge ΔQ moves
from one terminal to the other is
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The following example illustrates how the charge
that passes through a circuit and the work done by
the battery moving that charge can be determined.
© 2014 Pearson Education, Inc.
I = 0.44 A (C/s) t = 64 s ΔQ = I Δt
ΔQ = (0.44 C/s) 64 s
= 28 C
© 2014 Pearson Education, Inc.
ΔQ = 28 C ԑ = 1.5 V W = ΔQ ԑ
W = (28 C) 1.5 J/C
= 42 J
Electric Current, Resistance, and
Semiconductors
• When drawing an electric circuit, it's helpful to include an
arrow to indicate the flow of current. By convention, the
direction of the current in an electric circuit is the direction
in which a positive test charge would move.
• In typical circuits, the charges that flow are actually
negatively charged electrons. As a result, the flow of
electrons and the current arrow point in opposite directions,
as indicated in the figure below.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• As surprising as it may seem, electrons move rather
slowly through a wire. Their path is roundabout because
they are involved in numerous collisions with the atoms
in the wire, as indicated in the figure below.
• A electron's average speed, or drift speed, as it is called,
is about 10−4 m/s—that's only about a hundredth of a
centimeter per second!
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• At this speed, it would take an electron about
3 hours to go from a car's battery to the headlights.
However, we know that the lights come on almost
immediately. Why the discrepancy?
• While the electrons move with a rather slow
average speed, the influence they have on one
another, due to the electrostatic force, moves
through the wire at nearly the speed of light.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• Electrons flow through metal wires with relative
ease. In the ideal case, the electrons move with
complete freedom. Real wires, however, always
affect the electrons to some extent.
• Collisions between electrons and atoms in a
wire cause a resistance to the electron's motion.
This effect is similar to friction resisting the
motion of a box sliding across a floor.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• To move electrons against the resistance of a
wire, it is necessary to apply a potential
difference between the wire's ends.
• Ohm's law relates the applied potential
difference to the current produced and the wire's
resistance. To be specific, the three quantities
are related as follows:
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• Ohm's law is named for the German physicist
Georg Simon Ohm (1789–1854).
• Rearranging Ohm's law to solve for the resistance,
we find
R = V/I
• From this expression, it is clear that resistance has
units of volts per amp. A resistance of 1 volt per
amp defines a new unit—the ohm. The Greek letter
omega (Ω) is used to designate the ohm. Thus,
1 Ω = 1 V/A
• A device for measuring resistance is called an
ohmmeter.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• A resistor is a small device used in electric
circuits to provide a particular resistance to
current. The resistance of a resistor is given in
ohms, as shown in the following Quick Example.
• In an electric circuit, a resistor is signified by a
zigzag line, 222.. , as a reminder of the zigzag
path of the electrons in the resistor.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• The following chart summarizes the elements of
electric circuits, their symbols, and their physical
characteristics.
© 2014 Pearson Education, Inc.
© 2014 Pearson Education, Inc.
Sample Problem
If 240 C of charge passes a point in a circuit in
300s, what is the current through that point in the
circuit?
© 2014 Pearson Education, Inc.
𝑄 = 240 𝐶
𝑡 = 300𝑠
𝐼 =
𝑄
𝑡
𝐼 =
240 𝐶
300𝑠
𝐼 =
0.8 𝐶
𝑠
𝐼 = 0.8 𝐴
𝐼 =?
Sample Problem
How many electrons per hour flow past a point in a
circuit if it bears 11.4 mA of direct current?
© 2014 Pearson Education, Inc.
𝐼 =
𝑄
𝑡
𝑛 =
𝑄
𝑒
𝑄 = (11.4 𝑥 10−3
𝐴)(3600𝑠)
𝐼 = 11.4 𝑚𝐴
𝐼 = 11.4 𝑥 10−3
𝐴
𝑡 = 3600 𝑠
𝑄 = 𝐼 𝑡
𝑄 = 41.04 𝐶
𝑒 = 1.6 𝑥 10−19
𝐶
𝑛 =
41.04 𝐶
1.6 𝑥 10−19𝐶
𝑛 = 2.565 𝑥 1020
𝑄 =?
Sample Problem
A defibrillator sends a 6.00 A current through the
chest of a patient by applying a 10,000 V. What is
the resistance of the path?
© 2014 Pearson Education, Inc.
𝑉 = 10,000 𝑉
𝐼 = 6.00 𝐴
𝑅 =?
𝑅 =
𝑉
𝐼
𝑅 = 1.67 𝑥 103
Ω
𝑅 =
10,000 𝑉
6.00 𝐴
Sample Problem
If a circuit has a resistance of 18 Ω and a current of
15 A, what the voltage?
© 2014 Pearson Education, Inc.
𝑅 = 18 Ω
𝐼 = 15 𝐴
𝑉 =?
𝑅 =
𝑉
𝐼
𝑉 = 270 𝑉
𝑉 = 𝐼𝑅
𝑉 = (15 𝐴)(18 Ω)
Sample Problem
What is current in a wire with a potential difference
of 10 V across its ends a resistance of 2 ohms?
© 2014 Pearson Education, Inc.
𝑅 = 2 Ω
𝑉 = 10 𝑉
𝐼 =?
𝑅 =
𝑉
𝐼
𝐼 = 5 𝐴
𝐼 =
𝑉
𝑅
𝐼 =
10 𝑉
2 Ω
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• A wire's resistance is affected by several factors.
• The resistance of a wire depends on the material from
which it is made. For example, if a wire is made of
copper, its resistance is less than if it is made from iron.
The resistance of a given material is described by its
resistivity, ρ.
• A wire's resistance also depends on it length, L, and its
cross-sectional area, A. To understand these factors,
let's consider water flowing through a hose. If the hose is
very long, its resistance to the water is correspondingly
large. On the other hand, a wide hose, with a greater
cross-sectional area, offers less resistance to the water.
© 2014 Pearson Education, Inc.
Electric Current, Resistance, and
Semiconductors
• Combining these observations regarding the
factors that affect a wire's resistance, we can
write the following relationship:
• The units of resistivity are ohm-meters (Ω·m),
and its magnitude varies greatly with the type of
material. Insulators have large resistivities;
conductors have low resistivities.
© 2014 Pearson Education, Inc.
Sample Problem
What is the resistivity of a substance which has a
resistance of 1000 Ω if the length of the material is
4.0 cm and its cross sectional are is 0.20 cm2?
© 2014 Pearson Education, Inc.
𝑅 = 1000 Ω 𝐿 = 4.0 𝑐𝑚 − 0.04 𝑚
𝐴 = 0.20 𝑐𝑚2 − 2 𝑥10−5
𝑚2
𝑅 = 𝜌
𝐿
𝐴
𝜌 = 0.5Ω𝑚
𝜌 =
𝑅𝐴
𝐿
𝜌 =
(1000 Ω)(2𝑥10−5
𝑚2)
0.04 𝑚
𝜌 = ?
=
2
4
Ω𝑚
Electric Current, Resistance, and
Semiconductors
• As a wire is heated, its resistivity tends to increase. This
effect occurs because atoms that are jiggling more
rapidly are more likely to collide with electrons and slow
their progress through the wire.
• The following table summarizes the four factors that
affect the resistance of a wire.
© 2014 Pearson Education, Inc.
© 2014 Pearson Education, Inc.

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Electric current, emf and electric circuit

  • 1. © 2014 Pearson Education, Inc. Electric Current and Electric Circuits
  • 2. Chapter Contents • Electric Current, Resistance, and Semiconductors • Electric Circuits • Power and Energy in Electric Circuits © 2014 Pearson Education, Inc.
  • 3. Electric Current, Resistance, and Semiconductors • All electric circuits have one thing in common—they depend on the flow of electric charge. • When electric charge flows from one place to another, we say it forms an electric current. The more charge that flows, and the faster it flows, the greater the electric current. • In general, electric charge is carried through a circuit by electrons. © 2014 Pearson Education, Inc.
  • 4. Electric Current, Resistance, and Semiconductors • Suppose an amount of charge ΔQ flows past a given point in a wire in the time Δt. The electric current, I, in the wire is simply defined as the amount of charge divided by the amount of time. • The following equation is used to determine the current flowing in a wire. © 2014 Pearson Education, Inc.
  • 5. Electric Current, Resistance, and Semiconductors • The unit of current is the ampere (A), or amp for short. It is named for the French physicist André-Marie Ampère (1775–1836). • A current of 1 amp is defined as the flow of 1 coulomb of charge in 1 second: 1 A = 1 C/s • A 1-amp current is fairly strong. Many electronic devices, like cell phones and digital music players, operate on currents that are a fraction of an amp. © 2014 Pearson Education, Inc.
  • 6. Electric Current, Resistance, and Semiconductors • The following Conceptual Example illustrates how the current depends on both the amount of charge flowing and the amount of time. © 2014 Pearson Education, Inc.
  • 7. Electric Current, Resistance, and Semiconductors • The following example shows that the number of electrons flowing in a typical circuit is extremely large. The situation is similar to the large number of water molecules flowing through a garden hose. © 2014 Pearson Education, Inc.
  • 8. Electric Current, Resistance, and Semiconductors © 2014 Pearson Education, Inc.
  • 9. Electric Current, Resistance, and Semiconductors © 2014 Pearson Education, Inc.
  • 10. © 2014 Pearson Education, Inc.
  • 11. Electric Current, Resistance, and Semiconductors • When charge flows through a closed path and returns to its starting point, we say that the closed path is an electric circuit. • In a type of circuit known as a direct-current circuit, or DC circuit, the current always flows in the same direction. Circuits that run on batteries are typically DC circuits. • Circuits with currents that periodically reverse their direction are referred to as alternating-current circuits, or AC circuits. The electricity provided by a wall plug in your house is AC. © 2014 Pearson Education, Inc.
  • 12. Electric Current, Resistance, and Semiconductors • Although electrons move fairly freely in metal wires, something has to push on them to get them going and keep them going. It's like water in a garden hose; the water flows only when a force pushes on it. Similarly, electrons flow in a circuit only when an electrical force pushes on them. • Figure (a) below shows that there is no water flow if both ends of the garden hose are held at the same level. © 2014 Pearson Education, Inc.
  • 13. Electric Current, Resistance, and Semiconductors • Figure (b) shows that water flows from the end where the gravitational potential energy is high to the end where it is low. The difference in gravitational potential energy between the two ends of the hose results in a force on the water—which in turn produces a flow. A battery performs a similar function in an electric circuit. © 2014 Pearson Education, Inc.
  • 14. Electric Current, Resistance, and Semiconductors • A battery uses chemical reactions to produce a difference in electric potential between its two ends, which are referred to as the terminals. The symbol for a battery is . • A battery's positive terminal has a high electrical potential and is denoted with a plus (+) sign; the negative terminal has a low electric potential and is denoted with a minus sign (−). © 2014 Pearson Education, Inc.
  • 15. Electric Current, Resistance, and Semiconductors • When a battery is connected to a circuit, electrons move in a closed path from one terminal of the battery through the circuit and back to the other terminal of the battery. The electrons leave from the negative terminal of the battery and return to the positive terminal. © 2014 Pearson Education, Inc.
  • 16. Electric Current, Resistance, and Semiconductors • The situation is similar to the flow of blood in your body. Your heart acts like a battery, causing blood to flow through a closed circuit of arteries and veins in your body. © 2014 Pearson Education, Inc.
  • 17. Electric Current, Resistance, and Semiconductors • The figure below shows a simple electrical system consisting of a battery, a switch, and a lightbulb connected together in a flashlight. © 2014 Pearson Education, Inc.
  • 18. Electric Current, Resistance, and Semiconductors • The circuit diagram in figure (b) below shows that the switch is open—creating an open circuit. When a circuit is open, no charge can flow. When the switch is closed, electrons flow through the circuit and the light glows. © 2014 Pearson Education, Inc.
  • 19. Electric Current, Resistance, and Semiconductors • The figure below shows a mechanical equivalent of the flashlight circuit. The person lifting the water corresponds to the battery, the paddle wheel corresponds to the lightbulb, and the water is like the electric charge. © 2014 Pearson Education, Inc.
  • 20. Electric Current, Resistance, and Semiconductors • The difference in electric potential between the terminals of the battery is the electromotive force, or emf. Symbolically, the electromotive force is represented by the symbol ε (the Greek letter epsilon). The unit of emf is the same as that of electrical potential, namely, the volt. • The electromotive force is not really a force. Instead, the emf determines the amount of work a battery does to move a certain amount of charge around a circuit. © 2014 Pearson Education, Inc.
  • 21. Electric Current, Resistance, and Semiconductors • To be specific, the magnitude of the work done by a battery with the emf ε as charge ΔQ moves from one terminal to the other is © 2014 Pearson Education, Inc.
  • 22. Electric Current, Resistance, and Semiconductors • The following example illustrates how the charge that passes through a circuit and the work done by the battery moving that charge can be determined. © 2014 Pearson Education, Inc.
  • 23. I = 0.44 A (C/s) t = 64 s ΔQ = I Δt ΔQ = (0.44 C/s) 64 s = 28 C © 2014 Pearson Education, Inc. ΔQ = 28 C ԑ = 1.5 V W = ΔQ ԑ W = (28 C) 1.5 J/C = 42 J
  • 24. Electric Current, Resistance, and Semiconductors • When drawing an electric circuit, it's helpful to include an arrow to indicate the flow of current. By convention, the direction of the current in an electric circuit is the direction in which a positive test charge would move. • In typical circuits, the charges that flow are actually negatively charged electrons. As a result, the flow of electrons and the current arrow point in opposite directions, as indicated in the figure below. © 2014 Pearson Education, Inc.
  • 25. Electric Current, Resistance, and Semiconductors • As surprising as it may seem, electrons move rather slowly through a wire. Their path is roundabout because they are involved in numerous collisions with the atoms in the wire, as indicated in the figure below. • A electron's average speed, or drift speed, as it is called, is about 10−4 m/s—that's only about a hundredth of a centimeter per second! © 2014 Pearson Education, Inc.
  • 26. Electric Current, Resistance, and Semiconductors • At this speed, it would take an electron about 3 hours to go from a car's battery to the headlights. However, we know that the lights come on almost immediately. Why the discrepancy? • While the electrons move with a rather slow average speed, the influence they have on one another, due to the electrostatic force, moves through the wire at nearly the speed of light. © 2014 Pearson Education, Inc.
  • 27. Electric Current, Resistance, and Semiconductors • Electrons flow through metal wires with relative ease. In the ideal case, the electrons move with complete freedom. Real wires, however, always affect the electrons to some extent. • Collisions between electrons and atoms in a wire cause a resistance to the electron's motion. This effect is similar to friction resisting the motion of a box sliding across a floor. © 2014 Pearson Education, Inc.
  • 28. Electric Current, Resistance, and Semiconductors • To move electrons against the resistance of a wire, it is necessary to apply a potential difference between the wire's ends. • Ohm's law relates the applied potential difference to the current produced and the wire's resistance. To be specific, the three quantities are related as follows: © 2014 Pearson Education, Inc.
  • 29. Electric Current, Resistance, and Semiconductors • Ohm's law is named for the German physicist Georg Simon Ohm (1789–1854). • Rearranging Ohm's law to solve for the resistance, we find R = V/I • From this expression, it is clear that resistance has units of volts per amp. A resistance of 1 volt per amp defines a new unit—the ohm. The Greek letter omega (Ω) is used to designate the ohm. Thus, 1 Ω = 1 V/A • A device for measuring resistance is called an ohmmeter. © 2014 Pearson Education, Inc.
  • 30. Electric Current, Resistance, and Semiconductors • A resistor is a small device used in electric circuits to provide a particular resistance to current. The resistance of a resistor is given in ohms, as shown in the following Quick Example. • In an electric circuit, a resistor is signified by a zigzag line, 222.. , as a reminder of the zigzag path of the electrons in the resistor. © 2014 Pearson Education, Inc.
  • 31. Electric Current, Resistance, and Semiconductors • The following chart summarizes the elements of electric circuits, their symbols, and their physical characteristics. © 2014 Pearson Education, Inc.
  • 32. © 2014 Pearson Education, Inc.
  • 33. Sample Problem If 240 C of charge passes a point in a circuit in 300s, what is the current through that point in the circuit? © 2014 Pearson Education, Inc. 𝑄 = 240 𝐶 𝑡 = 300𝑠 𝐼 = 𝑄 𝑡 𝐼 = 240 𝐶 300𝑠 𝐼 = 0.8 𝐶 𝑠 𝐼 = 0.8 𝐴 𝐼 =?
  • 34. Sample Problem How many electrons per hour flow past a point in a circuit if it bears 11.4 mA of direct current? © 2014 Pearson Education, Inc. 𝐼 = 𝑄 𝑡 𝑛 = 𝑄 𝑒 𝑄 = (11.4 𝑥 10−3 𝐴)(3600𝑠) 𝐼 = 11.4 𝑚𝐴 𝐼 = 11.4 𝑥 10−3 𝐴 𝑡 = 3600 𝑠 𝑄 = 𝐼 𝑡 𝑄 = 41.04 𝐶 𝑒 = 1.6 𝑥 10−19 𝐶 𝑛 = 41.04 𝐶 1.6 𝑥 10−19𝐶 𝑛 = 2.565 𝑥 1020 𝑄 =?
  • 35. Sample Problem A defibrillator sends a 6.00 A current through the chest of a patient by applying a 10,000 V. What is the resistance of the path? © 2014 Pearson Education, Inc. 𝑉 = 10,000 𝑉 𝐼 = 6.00 𝐴 𝑅 =? 𝑅 = 𝑉 𝐼 𝑅 = 1.67 𝑥 103 Ω 𝑅 = 10,000 𝑉 6.00 𝐴
  • 36. Sample Problem If a circuit has a resistance of 18 Ω and a current of 15 A, what the voltage? © 2014 Pearson Education, Inc. 𝑅 = 18 Ω 𝐼 = 15 𝐴 𝑉 =? 𝑅 = 𝑉 𝐼 𝑉 = 270 𝑉 𝑉 = 𝐼𝑅 𝑉 = (15 𝐴)(18 Ω)
  • 37. Sample Problem What is current in a wire with a potential difference of 10 V across its ends a resistance of 2 ohms? © 2014 Pearson Education, Inc. 𝑅 = 2 Ω 𝑉 = 10 𝑉 𝐼 =? 𝑅 = 𝑉 𝐼 𝐼 = 5 𝐴 𝐼 = 𝑉 𝑅 𝐼 = 10 𝑉 2 Ω
  • 38. © 2014 Pearson Education, Inc.
  • 39. Electric Current, Resistance, and Semiconductors • A wire's resistance is affected by several factors. • The resistance of a wire depends on the material from which it is made. For example, if a wire is made of copper, its resistance is less than if it is made from iron. The resistance of a given material is described by its resistivity, ρ. • A wire's resistance also depends on it length, L, and its cross-sectional area, A. To understand these factors, let's consider water flowing through a hose. If the hose is very long, its resistance to the water is correspondingly large. On the other hand, a wide hose, with a greater cross-sectional area, offers less resistance to the water. © 2014 Pearson Education, Inc.
  • 40. Electric Current, Resistance, and Semiconductors • Combining these observations regarding the factors that affect a wire's resistance, we can write the following relationship: • The units of resistivity are ohm-meters (Ω·m), and its magnitude varies greatly with the type of material. Insulators have large resistivities; conductors have low resistivities. © 2014 Pearson Education, Inc.
  • 41. Sample Problem What is the resistivity of a substance which has a resistance of 1000 Ω if the length of the material is 4.0 cm and its cross sectional are is 0.20 cm2? © 2014 Pearson Education, Inc. 𝑅 = 1000 Ω 𝐿 = 4.0 𝑐𝑚 − 0.04 𝑚 𝐴 = 0.20 𝑐𝑚2 − 2 𝑥10−5 𝑚2 𝑅 = 𝜌 𝐿 𝐴 𝜌 = 0.5Ω𝑚 𝜌 = 𝑅𝐴 𝐿 𝜌 = (1000 Ω)(2𝑥10−5 𝑚2) 0.04 𝑚 𝜌 = ? = 2 4 Ω𝑚
  • 42. Electric Current, Resistance, and Semiconductors • As a wire is heated, its resistivity tends to increase. This effect occurs because atoms that are jiggling more rapidly are more likely to collide with electrons and slow their progress through the wire. • The following table summarizes the four factors that affect the resistance of a wire. © 2014 Pearson Education, Inc.
  • 43. © 2014 Pearson Education, Inc.