Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force  Indicate which pairs of charges will repel and.

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Presentation transcript:

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force  Indicate which pairs of charges will repel and which will attract.  Explain what factors affect the strength of the electric force.  Describe the characteristics of the electric field due to a charge. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force  Electric charge is an electrical property of matter that creates electric and magnetic forces and interactions.  Like charges repel, and opposite charges attract. The two types of charges are called positive and negative.  An object’s electric charge depends on the imbalance of its protons and electrons. Electrons are negatively charged, protons are positively charged, and neutrons are neutral (no charge). Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Negatively charged objects have more electrons than protons. Positively charged objects have fewer electrons than protons.  The SI unit of electric charge is the coulomb, C. A proton has a charge of 1.6  10 –19 C An electron has a charge of 1.6  10 –19 C. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force  Conductors allow charges to flow; insulators do not.  Objects can be charged by the transfer of electrons. The outermost electrons can be easily transferred from one atom to another. Charging by friction is when one material gains electrons and becomes negatively charged, and the other loses electrons and becomes positively charged. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force  Objects can also be charged without friction. One way to charge a neutral object without friction is by touching it with a charged object. Objects charged in this manner are said to be charged by contact.  Charges move within uncharged objects. The charges in a neutral conductor can be redistributed without contacting a charged object. Although the total charge on the conductor will be zero, the opposite sides will have an induced charge. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force When a negative rod touches a neutral doorknob, electrons move from the rod to the doorknob. The transfer of electrons to the metal doorknob gives the doorknob a net negative charge. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force  Electric force is the force of attraction or repulsion between objects due to charge.  Electric force depends on charge and distance. The electric force between two objects is proportional to the product of the charges on the objects. The electric force is inversely proportional to the square of the distance between two objects. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force  Electric force acts through a field. An electric field is a region in space around a charged object that causes a stationary charged object to experience an electric force. One way to show an electric field is by drawing electric field lines.  Electric field lines point in the direction of the electric force on a positive charge.  The electric field lines around a positive charge point outward.  The electric field lines around a negative charge point inward. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Electric field lines never cross one another. Field lines show both the direction of an electric field and the relative strength due to a given charge.  More lines are drawn for greater charges to indicate greater force. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 1 Electrical Charge and Force Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current  Describe how batteries are sources of voltage.  Explain how a potential difference produces a current in a conductor.  Define resistance.  Calculate the resistance, current, or voltage, given the other two quantities.  Distinguish between conductors, superconductors, semiconductors, and insulators. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current  Electrical potential energy is the ability to move an electric charge from one point to another. The electrical potential energy depends on the distance between two charged objects for both an attractive and a repulsive electric force. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current The electrical potential energy between two negative charges decreases as the distance between them increases. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current The electrical potential energy of a charge depends on its position in an electric field. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved.  Potential difference is measured in volts. The potential difference between any two points, is the work that must be done against electric forces to move a unit charge from one point to the other. The volt, V, is equivalent to one joule per coulomb (1 J/C). Potential difference is often called voltage. Section 2 Current Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current  There is a voltage across the terminals of a battery. A cell is a device that is a source of electric current because of a potential difference, or voltage, between the terminals.  One terminal is positive, and the other is negative. Batteries convert chemical energy into electrical energy. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current  A voltage sets charges in motion.  Current is the rate that electric charges move through a conductor. The SI unit of current is the ampere, A. 1 amp = 1 C/s A battery is a direct current source because the charges always move from one terminal to the other in the same direction. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current  Resistance is the opposition posed by a material or a device to the flow of current. Resistance is caused by internal friction, which slows the movement of charges through a conducting material.  Resistance can be calculated from current and voltage. Chapter 16 The SI unit of resistance is the ohm, Ω. 1 Ω = 1 V/A A resistor is a special type of conductor used to control current.

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current  Resistance The headlights of a typical car are powered by a 12 V battery. What is the resistance of the headlights if they draw 3.0 A of current when turned on? 1.List the given and unknown values. Given: Unknown: Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current 2.Write the equation for resistance. R = 4.0  Chapter 16 3.Insert the known values into the equation, and solve.

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 2 Current  Conductors have low resistances.  Some materials become superconductors below a certain temperature. Certain metals and compounds have zero resistance when their temperature falls below a certain temperature called the critical temperature.  Semiconductors are intermediate to conductors and insulators. The controlled addition of specific atoms of other materials as impurities dramatically increases a semiconductor’s ability to conduct electric charge. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  Use schematic diagrams to represent circuits.  Distinguish between series and parallel circuits.  Calculate electric power using voltage and current.  Explain how fuses and circuit breakers are used to prevent circuit overload. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  An electric circuit is a path through which charges can be conducted. An electric circuit is a set of electrical components connected such that they provide one or more complete paths for the movement of charges.  The conducting path produced when a light bulb is connected across the battery’s terminals is called a closed circuit.  Without a complete path, there is no charge flow and therefore no current. This is called an open circuit. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  Switches interrupt the flow of charges in a circuit. You can use a switch to open and close a circuit.  A schematic diagram is a graphical representation of a circuit that uses lines to represent wires and different symbols to represent components. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  Series circuits have a single path for current.  In a series circuit, the components of a circuit form a single path for current. The current in each device is the same. The resistances may be different. The voltage across each device in a series circuit can be different. If one element along the path in a series circuit is removed, the circuit will not work. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  Parallel circuits have multiple paths for current.  A parallel circuit is a circuit in which all of the components are connected to each other side by side. The voltage across each device is the same. The current in each device does not have to be the same. A break in any one path in a parallel circuit does not interrupt the flow of electric charge in the other paths. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Series and Parallel When bulbs are connected in series, charges must pass through both light bulbs to complete the circuit. When devices are connected in parallel, charges have more than one path to follow. The circuit can be complete even if one light bulb burns out. Section 3 Circuits Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  Electrical energy is the energy that is associated with charged particles because of their positions.  Electric power is the rate at which electrical energy is used in a circuit. Chapter 16 The SI unit for power is the watt (W). 1 W = 1 A  1 V

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  Electric Power When a hair dryer is plugged into a 120 V outlet, it has a 9.1 A current in it. What is the hair dryer’s power rating? 1.List the given and unknown values. Given: Unknown: Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  When electrical wires carry more than a safe level of current, the circuit is said to be overloaded.  A short circuit can happen if a wire’s insulation wears down, two wires may touch, creating an alternative pathway for current.  Fuses melt to prevent circuit overloads. A fuse an electrical device that contains a metal strip that melts when current in the circuit becomes too great. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits  Circuit breakers open circuits with high current. A circuit breaker a switch that opens a circuit automatically when the current exceeds a certain value. The circuit breaker acts as a switch. Unlike fuses, circuit breakers can be reset by turning the switch back on. Chapter 16

Copyright © by Holt, Rinehart and Winston. All rights reserved. Section 3 Circuits Chapter 16