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Electric Energy and Circuits Chapter 15

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Electric Energy and Circuits. Chapter 15. Potential Difference. Recall potential energy – the amount of energy an object could have due to its position. Ex. A book on a desk vs on the floor, a sky diver on the ground or 5000 ft in the air. The potential to move implies stored energy. - PowerPoint PPT Presentation

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Page 1: Electric Energy and Circuits

Electric Energy and CircuitsChapter 15

Page 2: Electric Energy and Circuits

Potential Difference•Recall potential energy – the amount of

energy an object could have due to its position.

•Ex. A book on a desk vs on the floor, a sky diver on the ground or 5000 ft in the air.

•The potential to move implies stored energy.•For an electric current to operate there

must be a difference in the amount of energy.

Page 3: Electric Energy and Circuits

•The electric potential difference between any two points in a circuit is the quotient of the change in the electric potential energy of charges passing between those points and the quantity of the charge.

•Electric potential difference - V or volt•Change in electrical potential energy -

ΔEQ, measured in joules•Charge - q measured in Coulombs

Page 4: Electric Energy and Circuits

•One joule per coulomb is equal to one volt.

•Recall from Physics 521 work and energy are interchangeable. Work = ΔEnergy

Page 5: Electric Energy and Circuits

•Variations of the formula for finding the electric potential difference.

•1 Volt = 1 Newton-meter/Coulomb = J/C

Page 6: Electric Energy and Circuits

•Do Sample Problem on Page 691•Do Practice Problems on Page 692 #s 1-3

Page 7: Electric Energy and Circuits

Electric Current•When the ends of a conductor are at

different potentials (voltage), charge flows from the region of higher potential to the region of lower potential across the ends of the conductor.

•The flow of charges will continue until both ends of the conductor reach the same potential, at which time it will stop flowing.

Page 8: Electric Energy and Circuits

•To continue a flow of charge in a conductor, a difference of potential must be maintained across the ends of the conductor.

•This requirement is provided by an “power supply” (for example, a battery converts chemical energy into electrical energy; a solar cell converts light energy into electric energy; a generator converts mechanical energy into electrical energy).

Page 9: Electric Energy and Circuits

•External energy from the pump sets up a potential difference between the two ends of the conductor by maintaining a constant negative charge in one area and a constant positive charge in another area (terminals of a battery).

• If these 2 points, at a different potential, are connected by a conducting wire, electric charge will flow from an area of high potential energy to the area of low potential energy within a closed loop called an electric circuit.

Page 10: Electric Energy and Circuits

•A circuit consists of a device which continuously increases the PE of the charges (power supply) connected to a device (load) that continuously reduces the PE of the charges by providing resistance to their movement (i.e. electric motor).

•This loss of PE of the charges as they move through the circuit can be converted into other forms of energy (i.e. a motor converts electric energy into kinetic energy and a lamp converts electric energy into light energy).

Page 11: Electric Energy and Circuits

•Electric pumps do not create electric charges or electrons, but only provide energy to move them through a circuit.

•The total amount of charge or energy in a circuit never changes; it is conserved.

• In any circuit, the PE increase (qV) provided by the charge pump (battery) equals the PE decrease as the current moves through a resistance (i.e. motor) because of the Law of Conservation of Energy.

Page 12: Electric Energy and Circuits

•When the flow takes place in one direction, it is called direct current (DC); and when it flows back and forth it is called alternating current (AC).

•open circuit- there is a break somewhere in the circuit which prevents current from flowing (i.e. an open switch).

•closed circuit- all connections are complete and current flows.

Page 13: Electric Energy and Circuits

Current vs Electron Flow•Early concepts (early 1800s) of current

electricity “assumed” a positive current.•JJ Thomson discovered the electron in 1901

and then scientists realized that it was the negative electron that was moving.

•However, current (I) means the flow of positive charges from anode (+) to cathode (-) in a circuit.

•The electron flow is from cathode (-) to anode (+).

Page 14: Electric Energy and Circuits

•The electric current is the flow of charges per unit of time.

•Current – I measured in amperes (A)•Charge – q measured in coulombs (C)•Time interval – Δt measured in seconds (s)

Page 15: Electric Energy and Circuits

•Do Sample Problem on Page 695•Do Practice Problems on Page 696 #s 4-

11

Page 16: Electric Energy and Circuits

Current and the Elementary Charge•Current is the flow of charges.•Elementary charge (e) is the amount of

charge on 1 electron – 1.60 × 10-19 C.•(Also the proton is + 1.60 × 10-19 C.)

q = Ne

•Do Model Problem on Page 699•Do Practice Problems on Page 700 #s 12-

15

Page 17: Electric Energy and Circuits

Electric Circuits•Schematic diagram- diagram of an

electric circuit using standard symbols for the electric circuit components (Figs. 15.10-15.12 on Page 701).

•See Conceptual Problems on Page 702

Page 18: Electric Energy and Circuits

Steps for Drawing Schematic Diagrams• 1. Draw the battery symbol on the left side of the page; put the positive

terminal on top.

• 2. Draw a wire connecting the conventional current out of the positive terminal. When you reach a resistor or another device, draw the symbol for it.

• 3. If you reach a point where there are 2 or more current paths (i.e. a voltmeter), draw in the diagram and follow one path until the two paths join again, then draw the second path.

• 4. Follow the path until you get to the negative terminal of the battery.

• 5. Check your drawing to ensure you have included all parts and that the current paths are complete.

• The direction of current flow is the direction that positive charges would move (this is called conventional current).

Page 19: Electric Energy and Circuits

Types of Electric Circuits•Series Circuit- a method of connecting

all circuit elements (loads and power source) which provides only one path through which current can flow.

•Parallel Circuit- a method of connecting two or more circuit elements between 2 points which provides more than one current path.

Page 20: Electric Energy and Circuits

Ammeters and Voltmeters•An ammeter, which measures the amount of

current, must be connected in series (same path as everything else) to give an accurate reading of current flow.

•A voltmeter, which measures the potential difference across a circuit device, must be attached in parallel (with one terminal on each side of the device across which it is measuring the potential difference).

•The potential difference across the device equals the potential difference across the voltmeter.

•See Figure 15.13 on Page 703

Page 21: Electric Energy and Circuits
Page 22: Electric Energy and Circuits

ResistanceSection 15.3•Voltage is an electrical pressure that can

produce current (a flow of charge) within a conductor.

•The amount of current that will flow in a circuit depends on the potential difference (voltage) across the circuit and the resistance the conductor (circuit) provides the moving charges.

Page 23: Electric Energy and Circuits

•Resistance (R) - the obstruction or resistance to the flow of electrical charges in a circuit.

•Fixed Resistor- a device designed to have a specific resistance. It is used to control the current in circuits or parts of circuits.

•Variable Resistor- also called a rheostat or potentiometer- a device consisting of a coil of resistance wire and a sliding contact point.

•This allows for varied amounts of current to flow in the circuit according to the equation V = IR.

•Ex: fans with different speeds and dimming lights.

Page 24: Electric Energy and Circuits

Factors Affecting Resistance in Electric Conductors1. Resistance increases proportionately

with the length.

2. Resistance varies inversely as the cross-sectional area.

Page 25: Electric Energy and Circuits

•By combining these proportionalities and using the resistivity constant, we get the following equation for the resistance of a conductor:

•Resistance is measured in ohms.•Resistivity() - measured in ∙m (See Table

15.1)

Page 26: Electric Energy and Circuits

•The resistance of a conductor also depends on the conductivity of material used and its temperature (a short, thick, cold conductor reduces resistance).

•Note that superconductors have zero resistance and therefore, no voltage drop across them.

Page 27: Electric Energy and Circuits

•Do Sample Problem on Page 707•Do Practice Problems on Page 708 #s 16 -

20

Page 28: Electric Energy and Circuits

•Ohm’s Law states that the resistance of an object is constant and independent of the voltage across it....the potential difference across a load equals the product of the current through the load and the resistance of the load (limited to metal conductors at stable temperatures).

Ohm’s Law

Page 29: Electric Energy and Circuits

•Ohm (Ω)- resistance of a device that allows current of 1 amp to flow when a potential difference of 1 volt is applied across the resistance. 1 Ω= 1Volt/Amp

•Ohm’s Law means that the current in a circuit , kept at a constant temperature, is directly proportional to the voltage across a circuit and inversely proportional to the resistance of the circuit. Therefore, the greater the voltage, the greater the current and the greater the resistance, the lesser the current.

Page 30: Electric Energy and Circuits

•Since I = V/R, the current flowing through a circuit can be regulated in 2 ways:

•1. increase or decrease the voltage across the circuit (i.e. to get a stronger charge pump or use more batteries).

•2. increase or decrease the resistance of the circuit using devices called resistors.

• If a device doesn’t obey Ohm’s Law, the graph of I versus V is non-linear (non-ohmic).

Page 31: Electric Energy and Circuits

•Do Sample Problem on Page 713•Do Practice Problems on Page 714 #s 21 -

26

Page 32: Electric Energy and Circuits

Series and Parallel CircuitsSection 15.4•Series Circuit – a complete path for

current to flow in which the electrical devices form a single path.

•Parallel Circuit –a circuit in which there are 2 or more paths for current to flow.

Page 33: Electric Energy and Circuits

Series Circuits•A break anywhere in the path stops current

flow in the entire circuit.•The total resistance of the circuit equals the

sum of the individual resistors.•The current (I) equals the voltage provided

by the source (V) divided by the total resistance (R).

•The voltage drop (potential difference) across each device is proportional to its resistance since more energy is needed to move charges through a large resistance. (V=IR)

Page 34: Electric Energy and Circuits

•The sum of the voltage drops across the resistance of each device is equal to the total voltage supplied by the source.

V = V1 + V2 + V3 + ... + VN (VN to represent any number of sources)

Since V = IRThen V= IR1 + IR2 + IR3 + ... + IRN

So then V = I(R1 + R2 + R3 + ... + RN)Therefore I = V/(R1 + R2 + R3 + ... +

RN)

Page 35: Electric Energy and Circuits

•The same current will exist in a series circuit with a single resistor that has a resistance equal to the sum of the individual resistances.

•The number of electrons moving or flowing (I) does not change.

•Equivalent resistance (Req) – a single resistance that has the same effect as a number of resistances in a series circuit. It is larger than any single resistance.

Req = R1 + R2 + R3 + ... + RN

Page 36: Electric Energy and Circuits

•To find the current with multiple resistors you should first find Req then use I = V/Req.

•The net change in electrical potential around the series circuit must be zero.

•The charge pump increases the PE of the charges but each resistor decreases the PE of the charges.

•This results in a net electrical potential change of zero.

Page 37: Electric Energy and Circuits

•To find the potential drop across each resistor in series you must use the equivalent resistance (Req) to find current (I), then you multiply I by the resistance of each individual device to find the potential drop across each device.

Page 38: Electric Energy and Circuits

•Do Model Problem on Page 718•Do Practice Problems on Page 719 - 720

#s 27-31

Page 39: Electric Energy and Circuits

Parallel Circuits•The potential difference across each path

is the same because each device connects the same two points of the parallel circuit.

•The total current is divided among the parallel branches. Current passes more readily into low resistors so that current (I) is inversely proportional to R (smaller R, more I). I = V/R

•The total current is the sum of the currents through each path. I = I1 + I2 + I3

Page 40: Electric Energy and Circuits

•As the number of parallel branches increases, the overall resistance of the circuit decreases.

•To find the current through each branch: I1 = V/R1

•To find the total current: I = V/R1 + V/R2 + V/R3

I = V(1/R1 + R2 + R3)

Page 41: Electric Energy and Circuits

•Equivalent resistance (1/Req) of three parallel resistors:

•The Req in a parallel circuit is less than the resistance of any resistor in the circuit.

Page 42: Electric Energy and Circuits

•Do Model Problem on Page 722-724•Do Practice Problems on Page 724 #s 32-

35

Page 43: Electric Energy and Circuits

Electric Circuit Overloads•An electric circuit overload may occur

when too many current drawing devices are connected in parallel.

•The overall resistance is reduced with each device added in parallel, so more current is allowed to flow.

•This adds sufficient thermal energy which may melt insulation on wires causing a short circuit when bare wires touch.

Page 44: Electric Energy and Circuits

•Short Circuit - a very low resistance connection between 2 points in a circuit where the resistance should be very high.

•Fuse – a safety device, added in series, which melts to stop current flow when it becomes too large.

•Circuit Breaker – an automatic switch that opens when the current meets a certain value. If a current that is greater than the set value flows, then it will overload and the circuit breaker opens to stop all current flow.

Page 45: Electric Energy and Circuits

Series – Parallel Combination Circuits•Steps1. If any resistors are in parallel, calculate the

equivalent resistance that would replace them.

2. If any equivalent resistors are now connected in series, calculate a new equivalent resistance that can replace them.

3. Repeat steps 1 & 2 until you can reduce the circuit to 1 resistor then find the current through the entire circuit. Finally, the voltage drops and current through each resistor can be found.

Page 46: Electric Energy and Circuits

Diagrams• Series Circuit • Parallel Circuit

Page 47: Electric Energy and Circuits

•Recall definitions of ammeters and voltmeters.

•In an ammeter, the resistance should be as low as possible so it does not change the current.

•In a voltmeter, the resistance should be high so the current does not go through the voltmeter.

Page 48: Electric Energy and Circuits

•Do Your Ohmwork (worksheet)•True/False worksheet

•Do Sample Problem on Pages 725- 727•Do Practice Problems on Page 728 #s 36

& 37

Page 49: Electric Energy and Circuits

Energy Transfer in Electric Circuits•As we have seen earlier, electrical energy can

be transferred into other forms of energy.

•Electrical power (the power of an electrical appliance) measures the rate at which electric charge or energy is transferred in a circuit (rate appliance does work).

•For resistors that obey Ohm’s Law, power equals the potential difference (Volts) across a circuit multiplied by the current (Amps).

Page 50: Electric Energy and Circuits

•When a battery converts one Joule of chemical energy to electrical energy per second, then the rate of transfer (power) is 1 J/s or 1 Watt (W).

•Power is determined by multiplying the potential difference across the appliance (V) by the current (I) moving through the appliance expressed in a term called Watts (J/s).

Page 51: Electric Energy and Circuits

•Power = voltage x current (P = IV)

•Power (P) measured in Watts (W)•Potential difference (V) measured in volts

(V)•Current (I) measured in amps (A)

Page 52: Electric Energy and Circuits

•Do Sample Problem on Page 736•Do Practice Problems on Page 737 #s 40 -

42

Page 53: Electric Energy and Circuits

•Also:

P = VI and V = IR, So by substitution: P = I × I × R or P =

I2R

Or P = VI and I =V/R,So P = V × V/R or P = V2/R

Page 54: Electric Energy and Circuits

•This means that the power lost in a resistor is directly proportional to the square of the current that passes through it and its resistance.

•The energy is changed from electrical into thermal energy and the resistor gets hot (ex. Heater).

•The electrical energy transferred to a resistor in a time interval (t) is equal to E = I2Rt.

Page 55: Electric Energy and Circuits

•If all the electric energy is transferred into thermal energy of the resistor, the increase in thermal energy is given by: E = I2Rt or E = Pt.

•This energy is expressed in Joules.•If not all the energy is transferred into

thermal energy, then figure out how much by using % efficiency.

Page 56: Electric Energy and Circuits
Page 57: Electric Energy and Circuits

•Do Model Problem on Page 742•Do Practice Problems on Page 744 #s 46-

50

Page 58: Electric Energy and Circuits

Transmitting Electric Energy•In order to transmit energy over long distances,

the energy lost to heat (P=I2R) must be controlled.

•To minimize this loss, there must be a reduction in the current (I) and/or the resistance (R).

•Since P = VI and the loss of power to heat is proportional to I2, in order to maintain large amounts of electrical power in transmission lines low current (I) at high voltage (V)is required.

Page 59: Electric Energy and Circuits

• Consumer energy cost –the cost of energy to use electrical devices.

• It is equal to the devices rate of consumption (J/s or W) multiplied by the number of seconds it was used. This gives Joules of energy.

• Rather than use this small unit of energy, electric companies measure energy consumption in kilowatt hours.

• Kilowatt hour – the unit of electric energy which is equal to 1000 Watts delivered for 1 hour or 1000 Watts in 3600 seconds.1kWh = 1000 J/s × 3600 s = 3.6 × 106 J

Page 60: Electric Energy and Circuits

•Do Model Problem on Page 745•Do Practice Problems on Page 746 #s 51-

53

Page 61: Electric Energy and Circuits

Chapter 15 Review•Do #s 1, 2, 3, 5, 6, 7, 10, 14, 21, 23-27, &

31 on Pages 747 -749