Transcript Ohm`s Law

Current Electricity,
Ohm’s Law & Circuits
Current (I)
• The rate of flow of charges through a
conductor
• Needs a complete closed conducting
path to flow
• Must have a potential difference
(voltage)
• Measured with an “ammeter” in amps
(A) named for Ampere – French
scientist
• I = current, A
Q = charge, C
Coulomb
t = time, s
So: 1 Amp = 1 sec ond
Q
I
t
Voltage (V)
• Electric potential difference between 2 points on a
conductor. Equal to the electric potential energy
per charge.
PE
V 
q
• Sometimes described as “electric pressure” that
makes current flow
• Supplies the energy of the circuit
• Measured in Volts (V) using a voltmeter
• 1 Volt = 1 Joule / Coulomb
Resistance (R)
• The “electrical friction” encountered by
the charges moving through a material.
• Depends on material, length, and crosssectional area of conductor
• Measured in Ohms (Ω)
R

A
Where: R = resistance,  = length
of conductor, A = cross-sectional
area of conductor, ρ = resistivity
of conducting material
Resistivity (ρ)
• Property of material that resists the
flow of charges (resistivity, ρ, in Ωm)
• The inverse property of conductivity
• Resistivity is temperature
dependent…as temperature increases,
then resistivity increases, and so
resistance increases.
Ohm’s Law
• A relationship between voltage, current,
and resistance in an electric circuit
• used to make calculations in all circuit
problems
• V = potential difference (voltage) in volts
• I = electric current in amperes (amps , A)
• R = resistance in ohms (  )
V  IR
Electric Power (Watts)
Energy
Power 
time
2
V
P  IV  I R 
• Used for thermal energy R
2
Electric Energy
• Electric energy can be measured in
Joules (J) or Kilowatt hours ( kWh )
• for Joules use Power in watts and time
in seconds
• for kWh use Power in kilowatts and
time in hours
E  Pt
Series Circuits
• Current can only travel through one path
• Current is the same through all parts of the circuit.
• The sum of the voltages of each component of the
circuit must equal the battery.
• The equivalent resistance of a series circuit is the
sum of the individual resistances.
Req  R1  R2  R3 ...
VBattery  V1  V2  V3 ...
I T  I1  I 2  I 3 ...
R1
V
I
R3
R2
Solving a Series Circuit
R1=1 Ω
IT
6V
R2=1 Ω
Step 1: Find the equivalent
(total) resistance of the circuit
RT  R1  R2
RT  1  1  2
Step 2: Find the total current
supplied by the battery
Step 3: Find Voltage Drop
across each resistor.
VBatt 6V
IT 

 3amps
RT
2
V1  I  R  3A 1  3V
Note: Since both resistors are the same, they use the same voltage. Voltage
adds in series and voltage drops should add to the battery voltage, 3V+3V=6V
Parallel Circuits
• Current splits into “branches” so there is more
than one path that current can take
• Voltage is the same across each branch
• Currents in each branch add to equal the total
current through the battery
1
1
1
1



...
Req
R1 R2 R3
I T  I1  I 2  I 3 ...
V
VBattery  V1  V2  V3  ...
R1
R2
R3
Solving a Parallel Circuit
Step 1: Find the total resistance of the circuit.
1
RT

1
R1

1
R2
1
RT

1
1

1
2

1
R3

so... R 
1
3


11
6
6
T
11
Step 2: Find the total current from the battery.
IT 
VT
RT

12V
6 
11
 22 A
Step 3: Find the current through
each resistor. Remember, voltage is
the same on each branch.
I1 
V1
R1
 121V  12 A
I2 
V2
R2
 122 V  6 A
I3 
V3
R3
 123V  4 A
Step 4: Check currents to see if the
answers follow the pattern for current.
I T  I1  I 2  I 3
R2=2Ω
12V
R1=1Ω
I T  12 A  6 A  4 A  22 A
R3=3Ω
The total of the branches should be equal
to the sum of the individual branches.
Combo Circuits with Ohm’s Law
What’s in series and what is in parallel?
A
3Ω
B
5Ω
15V
1Ω
6Ω
4Ω
7Ω
D
2Ω C
6Ω
4Ω
B
1Ω
3Ω
It is often easier to answer this
question if we redraw the circuit.
Let’s label the junctions (where
current splits or comes together)
as reference points.
A
5Ω
15V
C
2Ω
D
7Ω
Combo Circuits with Ohm’s Law
Now…again…what’s in series and what’s in parallel?
6Ω
4Ω
B
3Ω
1Ω
A
C
2Ω
D
7Ω
5Ω
15V
The 6Ω and the 4Ω resistors are in series with each other, the
branch they are on is parallel to the 1Ω resistor. The parallel
branches between B & C are in series with the 2Ω resistor.
The 5Ω resistor is on a branch that is parallel with the BC
parallel group and its series 2Ω buddy. The total resistance
between A & D is in series with the 3Ω and the 7Ω resistors.
Combo Circuits with Ohm’s Law
Finding total (equivalent) resistance
6Ω
4Ω
B
3Ω
C
2Ω
1Ω
A
D
7Ω
5Ω
15V
To find RT work from the inside out.
Start with the 6+4 = 10Ω series branch.
So, 10Ω is in parallel with 1Ω between
B&C…
1
RBC
11
 101  11  10
so... RBC  10
11  0.91
Then, RBC + 2Ω=2.91Ω and this
value is in parallel with the 5Ω
branch, so… 1  1  1
R AD
2.91
5
so... RAD  1.84
Finally RT = RAD +3 + 7 = 1.84 + 3 + 7
RT = 11.84Ω
Combo Circuits with Ohm’s Law
Solving for current and voltage drops in each resistor
RT = 11.84Ω
6Ω
4Ω
IT 
C
 1115.84V  1.27 A
2Ω
B
1Ω
3Ω
VT
RT
D
A
7Ω
5Ω
IT=1.27A
IT=1.27A
15V
The total current IT goes through the 3Ω
and the 7Ω and since those are in series,
they must get their chunk of the 15V
input before we can know how much is
left for the parallel. So…
IT  I 3  I 7   1.27 A
Then… V3  I 3  R  1.27 A  3  3.81V
V7   I 7   R  1.27 A  7  8.89V
So… VP  15V  3.81V  8.89V  2.3V
AD
Since parallel branches have the same
current, that means the voltage across
the 5Ω resistor V5Ω=4.84V and the
voltage across the parallel section
between B&C plus the 2Ω is also 4.84V
Combo Circuits with Ohm’s Law
Solving for current and voltage drops in each resistor (continued)
6Ω
4Ω
B
1Ω
3Ω
A
C
2Ω
I2Ω=0.81A
D
7Ω
5Ω
IT=1.27A
Known values from
previous slide.
RT  11.84
I T  1.27 A
V3  3.81V
V5  8.89V
VPAD  2.3V
15V
To calculate the current
through the 5Ω resistor…
I 5  VR5  25.3V  0.46 A
IT=1.27A
To calculate the top branch of the
parallel circuit between points A &
D we need to find the current and
voltage for the series 2 Ω resistor.
Since the current through the
resistor plus the 0.92A for the
bottom branch must equal 1.3A.
So… I 2  1.27 A  0.46 A  0.81A
V2  I 2  R  0.81A  2  1.62V
Combo Circuits with Ohm’s Law
Solving for current and voltage drops in each resistor (continued)
I6Ω=I4Ω =0.068A
C
B
6Ω
I1Ω=0.68A
A
2Ω
4Ω
1Ω
3Ω
Known values from
previous slide.
I2Ω=0.81A
D
RT  11.84
7Ω
V3  3.81V
5Ω
IT=1.27A
IT=1.27A
15V
Next we need to calculate
quantities for the parallel bunch
between points B&C. The
voltage that is left to operate this
parallel bunch is the voltage for
the 5Ω minus what is used by
the series 2Ω resistor. The 1Ω
resistor gets all of this voltage.
I T  1.27 A
Finally we need to calculate the
current through the 6Ω and 4Ω
resistors and the voltage used by each.
I 6  I 4 
0.68V
( 6 4) 
 0.068 A
All we need now is the voltage
drop across the 6Ω and 4Ω
resistors. So…
V7   8.89V
VPAD  V5  2.3V
I 5  0.46 A
I 2   0.81A
V2   1.62V
VPBC  V1  0.68V
I1  0.68 A
VPBC  V1  2.3V  1.62V  0.68V V6  I 6  R  0.068 A  6  0.41V
I1 
V1
R

0.68V
1
 0.68 A
V4  I 4  R  0.068 A  4  0.27V
THE END!
Voltmeter and Ammeter
• Ammeter
– Measures current in amps
– Placed in series where current is to be measured
• Voltmeter
– Measures voltage in Volts
– Placed in parallel across whatever is being
measured