Title: Problem Solving Unit 9 Ohms Law
1Problem SolvingUnit 9Ohms Law
GE184 Problem Solving
- John Elberfeld
- JElberfeld_at_itt-tech.edu
- 518 872 2082
2Electrical Charges
- People have seen the effects of electricity for
thousands of years - Lightning, electric shocks, static cling
- Only two types of electric charges exist
positive ( ) and negative ( - )
3Atomic Structure
- Nucleus has positive protons and neutral neutrons
- Very light negative electrons revolve in orbit
around the nucleus - Only electrons move away from the atom and make
up electric current
4Electricity
- Electric current is the flow of electrons
- Electrons flow easily through some materials.
- Other materials resist the flow of electrons
5Conductors and Insulators
- Current electricity is the movement of electrons
- Conductors let electrons move easily and so offer
low resistance to current flow - Insulators oppose the flow of electrons and so
offer high resistance to current flow - Semiconductors offer moderate, controllable
resistance - Resistance to current flow depends on the atomic
structure of the material
6Conductors
- Conductors contain a large number of free
electrons. - High conductance means the material is a good
electricity conductor (low resistance)
7Insulators
- Insulators prevent the flow of electricity
- A material with high insulation (resistance) is a
poor conductor of electricity
8Current Flow
- Electron current flow occurs as electrons move
away from the negative terminal towards the
positive terminal.
9Analogy for Current Flow
10Charges
- Electrons have a negative charge
- Protons have a positive charge
- The charge on an electron is equal in magnitude
but opposite in sign to a proton - The charge on an electron is the smallest unit of
electrical charge that exists in nature
11Real World Measurements
- We usually deal with billions and billions of
electrons - 1 coulomb 6.25 x 1018 electrons
- The charge on a object depends on how many EXTRA
charged particles are there - Usually the number of electrons balances the
number of protons, so the net charge is 0
12Charges
- When an object has a negative charge, it has
more electrons than protons - Charge is determined by how many more electrons
it has - When an object has a positive charge, it is
missing electrons and has more protons than
electrons - Protons do NOT move only electrons move to and
from an object - A positively charged objects has had electrons
removed from it
13Large and Small Numbers
- In electricity, you will work with very large and
very small numbers - You must use engineering notation in your work
and in your answers - 736 400 736.4 x 103
- Engineering notation is like scientific notation,
but the exponent is always a multiple of three
(3) 3, 6, 9. -3, -6
14Powers of Ten
15Positive Powers of 10
- If you move the decimal point in the number to
the left, you are making the number smaller. - To keep the same value, you must multiply by a
bigger power of 10
16Negative Powers of 10
- If you move the decimal point in the number to
the right, you are making the number bigger. - To keep the same value, you must multiply by a
negative power of 10
17Engineering Notation
- Write the number using powers of ten.
- Move the decimal point left while increasing the
exponent or right while decreasing the exponent. - The final exponent must be zero or a number that
is evenly divisible by three. - The number itself must be greater than one and
less than 1000
18Practice Exercises NOW!
- Convert the following numbers into engineering
notation - 1 2 3 4 5 6 7. 1.234567 x 106
- .0 0 1 2 3 1.23 x 10-3
-
- 1 2 3 . 4 x 105 12.34 x 106
- 1. 2 3 x 10-7 123. x 10-9
19Set Your Calculator
- Set your calculator to Engineering mode
- If you are an electronics student, and you dont
have a good calculator with Engineering mode, buy
one as soon as possible (Casio is good) - In engineering mode, the calculator always shows
numbers as a power of ten with an exponent a
multiple of three
20Practice Exercises NOW!
- Enter the following numbers into your calculator
and compare results when you choose engineering
mode - 1 234 567
- .00123
- 12.3 x 105
- 1.23 x 10-7
- .0123 x 108
- .00123 x 10-5
- 123.5
21Calculations with Exponents
- When multiplying, you add exponents
- (10x10x10)x(10x10) 10x10x10x10x10 105
- 103 x 102 1032 105
- 6 x 104 x 2 x 102 12 x 106
- Use your calculator in Engineering notation to
find - 3.21 x 105 x 12.98 x 108
- 3.21 EXP 5 x 12.98 EXP 8 416.7 x 1012
22More Calculations
- When dividing, you subtract exponents
- 10x10x10x10x10 10x10 10210x10x10
- 105 /103 105-3 102
- 10x10 1
10-310x10x10x10x10 10x10x10 - 102 / 105 102-5 10-3
23Example
- Fact 1 Coulomb (C) 6.25 x 1018 electrons
- A capacitor stores a charge of 1.5 x 10-5 C. How
many extra electrons are in the capacitor? - 93.75 x 1012 electrons
- This is a simple unit conversion problem
24Example
- Fact 1 C 6.25 x 1018 electrons
- How many coulombs in 3.0 x 1013 electrons?
- 4.8 x10-6 C
25On your own
- Fact 1 C 6.25 x 1018 electrons
- If you have 25.2 x 1026 extra electrons, what is
the charge in coulombs in engineering notation? - If you have 428 x 10-6 coulomb, what number of
extra electrons do you have?
26Prefixes
- Engineers usually replace the power of ten with a
prefix - Because all powers of 10 are multiples of 3 in
Engineering Notation, we dont have so many to
remember - Some prefixes use Greek letters as symbols
- Procedure to use a prefix
- 1. Write the quantity in engineering notation.
- 2. Replace the power of ten with its prefix.
27Prefixes and Symbols
28Prefixes and Symbols
29Practice
106M103k10-3 m10-6 µ10-9 n
- Enter the following numbers in your calculator
set in Engineering notation, hit the enter key,
and use the proper prefix - 12 x 104 C 120x103 C 120 kC
- .066 x 10-4 C
- 2345 mC
- .03 µC
30Electric Current
- Current
- Movement of electrons from negatively charged
atoms to positively charged atoms. - Represented as I.
- Coulomb
- 6.25 x 1018 electrons.
- Represented as C.
31Electric Current
- Electric current is the motion of free electrons
through a material. - Current is measured in Amperes
- 1 Ampere of current has 1 coulomb of electrons
flowing past a given point in the wire in just 1
second - 1 A 1 C/s
32Current Symbol
- The symbol for current is the letter I.
- I Q/T
- C is already used for capacitors and coulombs, so
I is less confusing for current, and Q for charge - Units are Coulombs/second Ampere
- Batteries are a source of electric current
- Electrons flow from the negative terminal through
the wire to the positive terminal
33Conventional Current
- Before scientist knew about electrons, they
guessed that electricity was the flow of positive
particles, but they were wrong - However, many books and most electrical symbols
are drawn to show the direction this positive
current would flow.
Electrons
34Current
35Current Calculations
106M103k10-3 m10-6 µ10-9 n
- Fact I Q / t
- What is the current if a charge (Q) of 12 mC
passes a point in time (t) of .023 s? - I 12 mC / .023 s 522 mA
- What is the current if 76 kC passes a point 834
sec? - I
36Voltage
- Voltage is the push behind the moving electrons.
- Voltage gives the electrons energy and gets them
to move from a negative area to a positive area
37Resistance
- The property of a material where an opposition to
the flow of electrons is offered is known as
resistance. - Unit of resistance is Ohm and is denoted by the
Greek letter omega, O.
38Resistance
- Not every material will conduct electricity
- Copper and aluminum conduct electricity easily
and are labeled conductors and have low
resistance - Plastic and rubber do not conduct electricity
easily and are labeled insulators and have high
resistance
39Measuring Resistance
- Resistance is a measure of how much a material
opposes the flow of electricity through it - A material with a resistance of 1 ohm requires 1
volt of energy to get 1 coulomb of charge
through it per second - 1 ohm 1 O 1 V / A
40Resistance Ranges
- Conductors have resistances of a few ohms or less
- Insulators have resistances in range of millions
of ohms or more - There is no absolute insulator or perfect
conductor
41Ohms Law
- MEMORIZE V I R
- Ohms Law
- If you increase the voltage, you increase the
current proportionally - 3 times the voltage gives you three times the
current - Resistance (ohms) is the proportionality constant
and depends on the atomic structure of the
material conducting the current
42Experiment
43Graph of Data
x
V
x
x
x
x
I
44Reasoning
V I R
- Ohms Law V I R
- High voltage produces high current for a given
resistance - Low voltage produces low current for a given
resistance - For a given voltage, a high resistance produces a
low current - For a given voltage, a low resistance produces a
high current
45Electronic Circuit
- A battery with the voltage V pushes a current I
through a resistor R
V I R
46Ohms Law
V I R
- This is the BIG IDEA for the day (year)!
- V I R
- What if we divide both sides by R?
- V I R R R
- But R/R 1, so we dont need to write it down
- I V I V / R R
47Ohms Law
V I R
- V I R
- What if we divide both sides by I?
- V I R I I
- But I / I 1, so we dont need to write it down
- R V R V / I I
48Ohms Law
- Memorize V I R
- Use algebra to find
- I V / R
- R V / I
- If you can, learn all three variations, but you
can get by if you memorize - V I R
49Practice
- V I R
- What voltage (V) is needed to push a current of
10 Amperes (I) through a resistance of 7 Ohms (R)
?
50Practice
- V I R
- What voltage (V) is needed to push a current of
10 Amperes (I) through a resistance of 7 Ohms (R)
? - V I R
- V 10 A x 7 O
- V 70 V
51Practice
- V I R
- What current (I) flows through a resistance of 8
ohms when the resistor is connect to a 24 volt
battery?
52Practice
V I R
- What current (I) flows through a resistance of 8
ohms when the resistor is connect to a 24 volt
battery? - V I R
- 24 V I x 8 O
- I 24 V / 8 O
- I 3 A
53Practice
V I R
- What size resistor allows 4 amperes of current
through it when it is connected to a 12 Volt
power supply?
54Practice
V I R
- What size resistor allows 4 amperes of current
through it when it is connected to a 12 Volt
power supply? - V I R
- 12 V 4 A x R
- R 12 V / 4 A
- R 3 O
55Now we add prefixes
- Very few electronics labs deal with simple volts,
amps, and ohms. - There is almost always a prefix, like millivolts,
microamperes, and kilo ohms - To work with real electric data, you have to be
able to handle these units on your calculator
56Examples
- Ohms Law V I R k 103 µ 10-6 m10-3
- How much voltage must be connected across a 1.2 k
O resistor to cause 575 µA of current to flow? - V I R
- V 575 µA 1.2 k O
- V .69V 690 x 10-3V 690 mV
57Examples
103k10-3 m10-6 µ
- Ohms Law V I R
- How much current flow through a 25 O resistor
with 10 V across it? - V I R I V / R
- 10 V I 25 O
- I 10 V / 25 O
- I .4 A or 400 x 10-3A 400 mA
58Examples
103k10-3 m10-6 µ
- Ohms Law V I R
- If a certain resistor allows 250 mA to flow when
35 V are across it, what is the resistance? - V I R R V / I
- 35 V 250 mA R
- R 35 V / 250 ma
- R 140 O
59Examples
103k10-3 m10-6 µ
- Ohms Law V I R
- How much current flows through a 3.3k O resistor
with 4.5 mV across it? - V I R I V / R
- 4.5 mV I 3.3k O
- I 4.5 mV / 3.3k O
- I 1.36 µ A
60Series Circuit
- A series circuit has one path for current flow.
- The current is the same at any point in the
circuit.
61SERIES CIRCUITS
- Total resistance in a series circuit is the
summation of the individual resistor values - RT R1 R2 R3 . Rn
- Where n the number of resistors
62OHMS LAW
- Total resistance in a series circuit is equal to
the total circuit voltage divided by the total
current Remember, IT is the same at every point
in the circuit
VT ITRT IT VT / RT
63Single Resistor Circuit
- Single resistor example
- V I R
- 10 V 2 A x 5 O
64OHMS LAW EXAMPLES
- Voltage 25 V
- Resistance 25 ?
- I _____
65OHMS LAW EXAMPLES
- Voltage 15 V
- Resistance 1 k?
- I _______
66OHMS LAW EXAMPLES
- Resistance 50 ?
- Current 2.5 A
- Voltage _______
67OHMS LAW EXAMPLES
- Resistance 10 k?
- Current 4 mA
- Voltage ______
V ? V
I 4mA
R 10kO
68OHMS LAW EXAMPLES
- Current 15 mA
- Voltage 15 V
- Resistance _______
V 15V
I 15mA
R ?O
69OHMS LAW EXAMPLES
- Current 4 mA
- Voltage 60 V
- Resistance _______
70BASIC CIRCUIT EXAMPLES
- R 10 k?, I 10 mA, V _____
- V 100 V
- V 50 V, I 2 mA, R ______
- R 25 k?
- V 75 V, R 10 k?, I ______
- I 7.5 mA
71Example
- Series circuit comprised of resistors
- To calculate out the total resistance we use the
formula RT R1 R2 R3 etc. - The total resistance for the figure is
- RT 10O 20O 30O 60 OHMS
72Replace The Resistors
IT VT/RT 120V / 60kO 2 mA
73Summary
- In a pure series circuit, the current in every
resistor is the same the same as the current
that leaves the battery - The effective resistance of the pure series
circuit is the sum of all resistors in series
74Replace The Resistors II
IT VT/RT 9V / 30kO 300 µA
75Replace The Resistors III
-
-
V 11V
I ?mA
R 4.27kO
IT VT/RT 11V / 4.27kO 2.58mA
76Series Circuit Review
- There is just one path for the current
- The current is the same in every component in a
series circuit - Total resistance is the sum of the resistors
77Parallel Circuits
- There are two or more paths for current flow.
- The voltage is the same across all parallel
branches. - The total current entering any point is equal to
the current leaving the point
78Parallel Combination of Resistances
- When all the resistors in a circuit are connected
in parallel, the circuit is called a parallel
circuit.
79Voltage Drop in Parallel Resistive Circuit
- The voltage drop across each component in a
parallel circuit is the same, since all the
resistances are connected in parallel. Thus, the
voltage across each connection is equal to the
supply voltage. - The voltage drop in a parallel circuit is
where, V is the
supply voltage.
80A Practical Example
- Car circuits (and house circuits) are all
parallel - You can run the radio without the horn being
turned on an advantage
81OHMS LAW EXAMPLES
- Voltage 25 V
- Find the total Current_______
- Find the equivalent Resistance ______
V 25V
R2 50O I2 ?
R1 25O I1 ?
82Calculations
- I1 V1/R1 25V/25O 1 A
- I2 V2/R2 25V/50O .5A (500mA)
- IT I1I2 1 A 500 mA 1.5 A
- RT VT/IT 25V/ 1.5 A 16.7 O
- Notice that the total resistance is LESS than any
one resistor in the circuit.
83TOTAL RESISTANCE
84Parallel Circuit Current
- Current leaving the () terminal is the same
current entering the () terminal. - This is referred to as total current (IT).
- Individual electrons may follow a variety of
paths, but every electron that leaves the battery
is balanced by an electron entering the battery
85Parallel Circuit Current
- Since the total current in the individual
resistors is equal to the current supplied by the
source, the total current can be stated as - IT IR1 IR2 IRn
86Sample Problems
R12kO
R36kO
R24kO
VT 36V
87Sample Problems
R12kO
R36kO
R24kO
VT 36V
88Finding Total Series Resistance
- Finding the total resistance for resistors in
SERIES is easy - In SERIES, just add up the all the resistors
89Finding Total Parallel Resistance
- Every resistor you add in parallel actually
REDUCES the equivalent resistance in the circuit - Each resistor you add in parallel increases the
current, which makes the resistance appear lower - Simple addition does NOT work for resistors in
parallel
90Finding Total Parallel Resistance
91Equation
- The reciprocal of the total resistance is equal
to the sum of the reciprocals of the resistors in
parallel - 1/RT 1/1kO 1/2kO 1/3kO
R11kO
R33kO
R22kO
VT 24V
A
B
C
92Calculations
- 1/RT 1/1kO 1/2kO 1/3kO
- 1/1 1/2 1/3 6/6 3/6 2/6 11/6 1/RT
- RT 6/11 .545 kO 545 O
- RT 545 O
- To check on a calculator
- 1 EXP 3 INV 2 EXP 3 INV 3 EXP 3 INV
EQUALS INV
93Practice
R12kO
R36kO
R24kO
VT 36V
94Series-Parallel Combination of Resistances
- This type of circuit consists of a combination of
resistances in series and parallel. - Series-parallel combination of resistances can be
classified as - Simple series-parallel circuits
- Complex series-parallel circuits
95Parallel Resistors
- For resistors to be in parallel, both ends of
each resistor must be in direct electrical
contact with each other with no resistance
between the ends - Parallel Not Parallel (blue)
96Recognizing Series Components
97Series-Parallel Circuits
- Pure series-parallel circuits can be reduced to a
single equivalent resistor - Example
98Example
- Another simple series-parallel circuit
99Example - Simple
100Voltage Drop in Series-Parallel Resistive Circuit
- To find the equivalent resistance of a
series-parallel resistive circuit - Identify the resistance combinations as either
series or parallel. - Simplify, combine and recombine series and
parallel combinations - Find the value of the total resistance of the
circuit. - Once you know the equivalent resistance, you can
calculate voltage or current
101Circuit Analysis
- Combine the two parallel resistors to one
equivalent resistor - 1/R23 1/20O 1/30O 3/60O 2/60O
- 1/R23 5/60O
- R23 12 O
R1 10O
R1 10O
V 25V
R3 30O
R23 12O
V 25V
R2 20O
102Analysis
- Combine the series resistors
- R123 10 O 12 O 22 O
R123 22O
R1 10O
V 25V
V 25V
R23 12O
103Analysis
- V 25 V, RT 22O,
- IT V/R 25V/22 O
- IT 1.14 A
R1 10O
R3 30O
V 25V
R2 20O
104Class Activity
- What is the equivalent resistance of the
following circuit?
R1 5.6kO
V 30V
R2 10kO
R5 3.3kO
R3 4.7kO
R4 2.2kO
105Current Analysis
- Combine resistors in series
- R23 10kO 4.7kO 14.7kO
R1 5.6kO
V 30V
R5 3.3kO
R23 14.7kO
R4 2.2kO
106Current Analysis
- Combine parallel resistors
- 1/R235 1/14.7 kO 1/3.3kO
- (Use your calculator!)
- R235 2.70 kO
V 30V
R1 5.6kO
R235 2.7 kO
R4 2.2kO
107Current Analysis
- Combine series resistors
- R12345 5.6 kO 2.7kO 2.2 kO 10.5 kO
R12345 10.5kO
V 30V
108More Analysis
- IT VT/RT 30V / 10.5 KO
- IT 2.85 mA
R1 5.6kO
V 30V
R2 10kO
R3 4.7kO
R4 2.2kO
109Ready for Thought Projects
- You are now ready to tackle Electronics Projects
1 2 on pages 135 - 146