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Transcript
Lecture PowerPoints
Physics for Scientists and
Engineers, 3rd edition
Fishbane
Gasiorowicz
Thornton
© 2005 Pearson Prentice Hall
This work is protected by United States copyright laws and is provided solely for
the use of instructors in teaching their courses and assessing student learning.
Dissemination or sale of any part of this work (including on the World Wide Web)
will destroy the integrity of the work and is not permitted. The work and materials
from it should never be made available to students except by instructors using
the accompanying text in their classes. All recipients of this work are expected to
abide by these restrictions and to honor the intended pedagogical purposes and
the needs of other instructors who rely on these materials.
Chapter 27
Direct-Current Circuits
Main Points of Chapter 27
• emf and its meaning
• Internal resistance
• Kirchhoff’s loop and junction rules
• Multi-loop circuits
• Measuring instruments
• RC circuits
27-1 EMF
• An emf is a source of energy in a circuit that
causes charges to move
• Circuit with battery and resistor: potential
difference between battery terminals causes
current to flow through resistor
• Chemical reactions inside battery send
charge back to terminal
• Definition of emf:
(27-1)
27-1 EMF
Internal resistance
• Battery with emf of 9 V will not
necessarily have 9 V potential
difference between its terminals, due
to internal resistance:
(27-5)
where r is the internal resistance.
27-2 Kirchhoff’s Loop Rule
• Single-loop circuit has just one path for current
• Beginning at any point in circuit and going all the
way around must involve a total potential change
of zero (you come back to where you started)
• When moving in the direction of the current,
potentials decrease across resistors and increase
across batteries
• Sum of potential changes around a closed path is
zero:
(27-9)
27-2 Kirchhoff’s Loop Rule
Basic single-loop circuit:
27-2 Kirchhoff’s Loop Rule
• When moving around the loop
opposite to the direction of the current,
potential difference increases across
resistors and decreases across
batteries
• Across a capacitor from – side to +
side, potential increases; in other
direction it decreases
27-3 Kirchhoff’s Junction Rule
• All the current that comes into a junction
must go out again
• The algebraic sum of the currents
entering a junction equals zero
(27-11)
27-3 Kirchhoff’s Junction Rule
• Solving multi-loop circuits:
• Use both junction and loop equations
• Some will be redundant
• Need as many independent equations as
there are unknown currents
• A circuit with n junctions will have n – 1
independent junction equations
27-3 Kirchhoff’s Junction Rule
Example:
• This circuit requires three independent equations
• This circuit has two junctions; two of the
equations will have to be loop equations
27-4 Measuring Instruments
• Ammeter measures current
• Voltmeter measures
potential difference
• Ohmmeter measures
resistance
• Multimeter does all three
27-4 Measuring Instruments
• Ammeter: connect in series; very small
resistance compared to other circuit
elements, so current is not affected
• Voltmeter: connect in parallel; large
resistance, so voltage is not affected
• Internal resistance of voltmeter can be
varied to allow different voltage scales
27-5 RC Circuits
RC circuit with battery and switch
• Switch at position A: battery charges capacitor
• Switch at position B: capacitor discharges
through resistor
27-5 RC Circuits
Current stops flowing when capacitor is fully
charged:
Charge as a function of time:
(27-22)
Current as a function of time:
Time constant:
(27-23)
27-5 RC Circuits
Current and charge as functions of time
27-5 RC Circuits
Discharging: charge
decreases with same
time constant
Summary of Chapter 27
• Sources of emf are sources of electric
energy
• emf is defined by work it can do:
(27-1)
• Kirchhoff’s loop rule:
(27-9)
• Kirchhoff’s junction rule:
(27-11)
Summary of Chapter 27, cont.
• Capacitor being charged by battery has
charge and current:
(27-22)
(27-23)
• When discharging,
(27-26)