Post on 25-Jul-2018
Physics 132: Lecture 15ys cs 3 ectu e 5Elements of Physics II
A d f T dAgenda for Today ResistanceResistance ResistorsResistors SeriesSeries ParallelParallel
Ohm’s lawOhm’s lawElectric CircuitsElectric Circuits Electric CircuitsElectric Circuits CurrentCurrent Kirchhoff’s lawsKirchhoff’s laws
Physics 201: Lecture 1, Pg 1
Kirchhoff s lawsKirchhoff s laws
Electromotive force
Electromotive force (emf) is the maximum Electromotive force (emf) is the maximum potential difference a battery or power source can give a circuit. A b h f f 12 V A car battery has an emf of 12 V
Sometimes shown as a script (E)
Symbol for emf
-+
Physics 201: Lecture 1, Pg 2
Electrical Current
When we connect the two terminals of an emf to When we connect the two terminals of an emf to a circuit ( a continuous conducting path), charge will move continuously through the circuit.
Since there is a potential difference electrons in circuit will feel a force
Electrons will flow in direction of positive
terminal
emf Battery “pushes”
electrons
Physics 201: Lecture 1, Pg 3
Electrical Current
This flow is called electric current This flow is called electric current Net amount of charge through a point in the
circuit per unit time.
Units Ampere = Coulomb/second
qtq I
Physics 201: Lecture 1, Pg 4
ExampleThe electron drift speed in a wire is exceedingly
slow-typically only a fraction of a millimeter per second. Yet when you turn on a flashlight switch, the light comes on almost instantly. Resolve this apparent paradox.
Physics 201: Lecture 1, Pg 5
ExampleThe electron drift speed in a wire is exceedingly slow-typically p g y yp y
only a fraction of a millimeter per second. Yet when you turn on a flashlight switch, the light comes on almost instantly. Resolve this apparent paradox.pp p
Correct:It's like water analogy on page 877. as water (electrons) start flowing intoIt s like water analogy on page 877. as water (electrons) start flowing into
one end of the pipe(wire), water(electron) from the other end of pipe (wire) start turning paddle wheel immediately. therefore light can come instantly as
you turn on the switch.y
There is a line of electrons in the wire. That means the electrons are right next to each other, so as soon as you turn the flashlight on, electrons will start to move, but there is an electron already there behind the part that
produces the light so as electrons are added from the electrical current, the light is produced immediately.
Physics 201: Lecture 1, Pg 6
Clicker Question 1:When a light bulb is emitting light in a circuit as g g g
below the number of electrons entering the light bulb is:(a) larger than the number leaving the light bulb(a) larger than the number leaving the light bulb(b) equal to the number leaving the light bulb(c) smaller than the number leaving the light bulb
Physics 201: Lecture 1, Pg 7
Plinko Disks = electrons Disk bounces through
atoms on it’s way down theatoms on it’s way down the incline
Angle of incline = emfg(potential difference)
Y t b d Youtube demo
Physics 201: Lecture 1, Pg 8
Resistance Resistance: Traveling through a conductor, electrons bump into
things which slows them downthings which slows them down. : Resistivity: Density of bumps L: Length of conductor
ALρR
A: Cross sectional area of conductor
A
Aρ
A All electrical devices will resist the flow
of electrical current
L
Physics 201: Lecture 1, Pg 9
PlinkoALρR A
Physics 201: Lecture 1, Pg 10
Clicker Question 2:
Iskinny
Below we have a skinny wire and a thick wire connected to identical batteries. Which case will have the larger current?
(a) Thick Wire( )(b) Skinny Wire(c) They will have the same current Ithick
Physics 201: Lecture 1, Pg 11
Clicker Question 3:Below we have circuit with a resistor and a wire. Which part will have
?the larger current?(a) Wire(b) Resistor(c) They will have the same current
Iwire
Iresistor
Physics 201: Lecture 1, Pg 12
Conservation of Current
Physics 201: Lecture 1, Pg 13
Charge Distribution The nonuniform distribution of surface charges along a
wire creates a net electric field inside the wire that points from the more positive end toward the more negative endp gof the wire.
This is the internal electric field that pushes the electron current through the wirecurrent through the wire.
Physics 201: Lecture 1, Pg 14
Clicker Question 4:Is this a possible surface charge distribution for a current carrying
?wire?
(a) yes(b) no
Physics 201: Lecture 1, Pg 15
Electric Current The direction of current flow – from the positive terminal to
the negative one – was decided before it was realized that electrons are negatively charged Therefore current flowselectrons are negatively charged. Therefore, current flows around a circuit in the direction a positive charge would move; electrons move the other way. However, this does not matter in most circuitsnot matter in most circuits.
Physics 201: Lecture 1, Pg 16
Kirchhoff’s Junction Law
For a junction, the law of conservation of current
requires that
where the symbol ymeans summation.
This basic conservation statement is called
Kirchhoff’s junction law
Physics 201: Lecture 1, Pg 17
law.
Kirchhoff’s Loop LawKirchhoff s Loop LawVoltage drops must add to zero
We can think of the voltage difference as a height We can think of the voltage difference as a height difference
R
I
Down Volts Up VoltsRDown Volts Up Volts
Electron must end up at same place it started!!
Physics 201: Lecture 1, Pg 18
Ohm’s law
With conductors the more resistance the less With conductors the more resistance the less current can flow
IRV Ohm’s law
• Hi h i t l t
IRV VI• Higher resistance lower current
Units are Ohms () RI
Physics 201: Lecture 1, Pg 19
Resistor
A device that resists current A device that resists current
Used to control current flow in a circuitUsed o co o cu e o a c cu
Resistor in a circuit:
Generally in a circuit the resistance of the connecting wires are very small and we canconnecting wires are very small and we can neglect them. Wires will resist current, but we will assume they have zero
Physics 201: Lecture 1, Pg 20
resistance!!
LRResistorALρR
Generally in a circuit the resistance of the connecting wires are very small and we can neglect them.
Student: How come the resistance of a wire is very very small, considering wires are usually longer than they are wide, so the Length is greater than the Area – shouldn’t the resistance be large?
Student: The textbook says about an ideal wire, but I don't understand how it i bl t t t if lt 0 Th kis possble to create a current if voltage = 0. Thanks
Physics 201: Lecture 1, Pg 21
Kirchhoff’s Loop LawKirchhoff s Loop Lawfor the Simplest Circuit in the World
R
I
R• Example
Calculate I when emf =24 Volts and R = 8 – Calculate I when emf =24 Volts and R = 8 – Ohm’s Law: V=IR
I 24/8 3 Amps– I = 24/8 = 3 Amps
Physics 201: Lecture 1, Pg 22
Clicker Question 5:Below we have two circuits, with identical batteries and three identical
Ccylindrical conductors. Compare the current in the two circuits:(a) IA > IB
(b) IA = IB
(c) IA < IB
Physics 201: Lecture 1, Pg 23
Circuit A Circuit B
Clicker Question 6: A light bulb is connected to a battery in case A.
In case B an identical light bulb is added inIn case B an identical light bulb is added in series. What happens to the brightness of the original bulb?(a) it stays the same(a) it stays the same(b) it decreases(c) it increases
Physics 201: Lecture 1, Pg 24
Case A Case B
Series wiring When two objects are connected end to end in a circuit, they are
id t b i isaid to be in series. Here R1 and R2 are in series
R1R2
Current must be same in each resistor!!
Voltage drop across R1 plus Voltage drop across R2should equal the emf of the battery
Physics 201: Lecture 1, Pg 25
should equal the emf of the battery
Resistors in series One wire:
If charge goes through one resistor, it must go through other.
I1 = I2 = IeqV V V V1 + V2 = Veq
Add Req = R1 + R2 Adding Voltage IR + IR =I(R + R ) R1 Adding Voltage IR1 + IR2=I(R1 + R2) Adding length Req=(L1+L2)/A
1
R2
Req
2
The equivalent resistance of resistors in series is just the addition of the resistors
Physics 201: Lecture 1, Pg 26
the addition of the resistors
Clicker Question 7:In the circuit below, what is the voltage across R1?
a) 12 VR = 4 R = 2 b) zero
c) 6 V
R1 = 4 R2 = 2
d) 8 V
e) 4 V 12 V
Physics 201: Lecture 1, Pg 27
Clicker Question 7:In the circuit below, what is the voltage across R1?
R1 = 4 R2 = 2 R1 4 R2 2
12 V
Physics 201: Lecture 1, Pg 28
Clicker Question 8:Below we have two circuits, with identical batteries and three identical
C fcylindrical conductors. Compare the current drawn from the batteries in the two circuits:(a) IA > IB
(b) IA = IB
(c) IA < IB
Physics 201: Lecture 1, Pg 29
Circuit A Circuit B