Chapter 26 DC Circuits. Copyright 2009 Pearson Education, Inc.

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Transcription:

Chapter 26 DC Circuits

26-1 EMF and Terminal Voltage Electric circuit needs battery or generator to produce current these are called sources of emf. Battery is a nearly constant voltage source, but does have a small internal resistance, which reduces the actual voltage from the ideal emf:

26-1 EMF and Terminal Voltage This resistance behaves as though it were in series with the emf.

26-1 EMF and Terminal Voltage Example 26-1: Battery with internal resistance. A 65.0-Ω resistor is connected to the terminals of a battery whose emf is 12.0 V and whose internal resistance is 0.5 Ω. Calculate (a) the current in the circuit, (b) the terminal voltage of the battery, V ab, and (c) the power dissipated in the resistor R and in the battery s internal resistance r. Solution p:678

A series connection has a single path from the battery, through h each circuit it element in turn, then back to the battery.

The current through each resistor is the same; the voltage depends on the resistance. The sum of the voltage drops across the resistors equals the battery voltage:

From this we get the equivalent resistance (that single resistance that gives the same current in the circuit):

A parallel connection splits the current; the voltage across each resistor is the same:

The total current is the sum of the currents across each resistor:,

This gives the reciprocal of the equivalent resistance:

An analogy using water may be helpful in visualizing parallel circuits. The water (current) splits into two streams; each falls the same height, and the total current is the sum of the two currents. With two pipes open, the resistance to water flow is half what it is with one pipe open.

Conceptual Example 26-2: Series or parallel? (a) The lightbulbs in the figure are identical. Which configuration produces more light? (b) (b) Which way do you think the headlights of a car are wired? Ignore change of filament resistance R with current. Solution p:681

Conceptual Example 26-3: An illuminating surprise. A 100-W, 120-V lightbulb and a 60-W, 120-V lightbulb are connected in two different ways as shown. In each case, which bulb glows more brightly? Ignore change of filament resistance with current (and temperature). Solution p:p681

Example 26-4: Circuit with series and parallel resistors. How much current is drawn from the battery shown? Solution p:681

Example 26-5: Current in one branch. What is the current through h the 500-Ω Ω resistor shown? (Note: This is the same circuit as in the previous problem.) The total current in the circuit was found to be 17 ma.

Conceptual Example 26-6: Bulb brightness in a circuit. The circuit shown has three identical lightbulbs, each of resistance R. (a) When switch S is closed, how will the brightness of bulbs A and B compare with that t of bulb C? (b) What happens when switch S is opened? Use a minimum of mathematics in your answers. Solution p:682

Example 26-7: A two-speed fan. One way a multiple-speed ventilation fan for a car can be designed is to put resistors in series with the fan motor. The resistors reduce the current through the motor and make it run more slowly. Suppose the current in the motor is 5.0 A when it is connected directly across a 12-V battery. (a) What series resistor should be used to reduce the current to 2.0 A for low-speed operation? (b) What power rating should the resistor have? Solution P:682

Example 26-8: Analyzing a circuit. A 9.0-V battery whose internal resistance r is 0.50 Ω is connected in the circuit shown. (a) How much current is drawn from the battery? (b) What is the terminal voltage of the battery? (c) What is the current in the 6.0-Ω resistor? Solution p:683

26-3 Kirchhoff s Rules Some circuits cannot be broken down into series and parallel connections. For these circuits we use Kirchhoff s rules.

26-3 Kirchhoff s Rules Junction rule: The sum of currents entering a junction equals the sum of the currents leaving it.

26-3 Kirchhoff s Rules Loop rule: The sum of the changes in potential around a closed loop is zero.

26-3 Kirchhoff s Rules Problem Solving: Kirchhoff s Rules 1. Label each current, including its direction. 2. Identify unknowns. 3. Apply junction and loop rules; you will need as many independent equations as there are unknowns. 4. Solve the equations, being careful with signs. If the solution for a current is negative, that current is in the opposite direction from the one you have chosen.

26-3 Kirchhoff s Rules Example 26-9: Using Kirchhoff s rules. Calculate the currents I 1, I 2, and I 3 in the three branches of the circuit in the figure. Solution p:685

26-7 Ammeters and Voltmeters Summary: An ammeter must be in series with the current it is to measure; a voltmeter t must be in parallel with the voltage it is to measure.

Summary of Chapter 26 A source of emf transforms energy from some other form to electrical energy. A battery is a source of emf in parallel with an internal resistance. Resistors in series:

Summary of Chapter 26 Resistors in parallel: Kirchhoff s rules: 1. Sum of currents entering a junction equals sum of currents leaving it. 2. Total potential difference around closed loop is zero.