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Ways to Wire Circuits
There are 2 basic ways to wire a circuit.
Series – One after another
Parallel – between a set of junctions and
parallel to each other
Series Circuit
In in series circuit, the resistors
are wired one after another.
Since they are all part of the
SAME LOOP they each
experience the SAME
AMOUNT of current. In
figure, however, you see
that they all exist
BETWEEN the terminals of
the battery, meaning they
SHARE the potential
(voltage).
3
2
1
)
(
3
2
1
)
(
V
V
V
V
I
I
I
I
Total
series
Total
series






Series Circuit
3
2
1
)
(
3
2
1
)
(
V
V
V
V
I
I
I
I
Total
series
Total
series






As the current goes through the circuit, the charges must USE ENERGY to get
through the resistor. So each individual resistor will get its own individual potential
voltage). We call this VOLTAGE DROP.













i
s
series
series
T
T
Total
series
R
R
R
R
R
R
R
I
R
I
R
I
R
I
IR
V
V
V
V
V
3
2
1
3
3
2
2
1
1
3
2
1
)
(
)
(
;
Note: They may use the
terms “effective” or
“equivalent” to mean
TOTAL!
Example A series circuit is shown to the left.
a) What is the total resistance?
b) What is the total current?
c) What is the current across EACH
resistor?
d) What is the voltage drop across
each resistor?( Apply Ohm's law
to each resistor separately)
R(series) = 1 + 2 + 3 = 6W
V=IR 12=I(6) I = 2A
They EACH get 2 amps!
V1W(2)(1) 2 V V3W=(2)(3)= 6V V2W=(2)(2)= 4V
Notice that the individual VOLTAGE DROPS add up to the TOTAL!!
Parallel Circuit
In a parallel circuit, we have
multiple loops. So the
current splits up among
the loops with the
individual loop currents
adding to the total
current
It is important to understand that parallel
circuits will all have some position
where the current splits and comes back
together. We call these JUNCTIONS.
The current going IN to a junction will
always equal the current going OUT of a
junction.
Junctions OUT
IN
Total
parallel
I
I
I
I
I
I




:
Junctions
Regarding
3
2
1
)
(
Parallel Circuit Notice that the JUNCTIONS both touch the
POSTIVE and NEGATIVE terminals of the
battery. That means you have the SAME
potential difference down EACH individual
branch of the parallel circuit. This means
that the individual voltages drops are equal.
This junction
touches the
POSITIVE
terminal
This junction
touches the
NEGATIVE
terminal
V
















i
P
P
Parallel
T
T
Total
parallel
Total
parallel
R
R
R
R
R
R
R
V
R
V
R
V
R
V
IR
V
I
I
I
I
V
V
V
V
1
1
1
1
1
1
)
(
;
3
2
1
3
3
2
2
1
1
3
2
1
)
(
3
2
1
)
(
Example







454
.
0
1
454
.
0
1
9
1
7
1
5
1
1
P
p
P
R
R
R




)
(
8 R
I
IR
V
To the left is an example of a parallel circuit.
a) What is the total resistance?
b) What is the total current?
c) What is the voltage across EACH resistor?
d) What is the current through each resistor?
(Apply Ohm's law to each resistor separately)
2.20 W
3.64 A
8 V each!








W
W
W
9
8
7
8
5
8
9
7
5 I
I
I
IR
V
1.6 A 1.14 A 0.90 A
Notice that the
individual currents
ADD to the total.

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Series and parallel circuits.ppt

  • 1. Ways to Wire Circuits There are 2 basic ways to wire a circuit. Series – One after another Parallel – between a set of junctions and parallel to each other
  • 2. Series Circuit In in series circuit, the resistors are wired one after another. Since they are all part of the SAME LOOP they each experience the SAME AMOUNT of current. In figure, however, you see that they all exist BETWEEN the terminals of the battery, meaning they SHARE the potential (voltage). 3 2 1 ) ( 3 2 1 ) ( V V V V I I I I Total series Total series      
  • 3. Series Circuit 3 2 1 ) ( 3 2 1 ) ( V V V V I I I I Total series Total series       As the current goes through the circuit, the charges must USE ENERGY to get through the resistor. So each individual resistor will get its own individual potential voltage). We call this VOLTAGE DROP.              i s series series T T Total series R R R R R R R I R I R I R I IR V V V V V 3 2 1 3 3 2 2 1 1 3 2 1 ) ( ) ( ; Note: They may use the terms “effective” or “equivalent” to mean TOTAL!
  • 4. Example A series circuit is shown to the left. a) What is the total resistance? b) What is the total current? c) What is the current across EACH resistor? d) What is the voltage drop across each resistor?( Apply Ohm's law to each resistor separately) R(series) = 1 + 2 + 3 = 6W V=IR 12=I(6) I = 2A They EACH get 2 amps! V1W(2)(1) 2 V V3W=(2)(3)= 6V V2W=(2)(2)= 4V Notice that the individual VOLTAGE DROPS add up to the TOTAL!!
  • 5. Parallel Circuit In a parallel circuit, we have multiple loops. So the current splits up among the loops with the individual loop currents adding to the total current It is important to understand that parallel circuits will all have some position where the current splits and comes back together. We call these JUNCTIONS. The current going IN to a junction will always equal the current going OUT of a junction. Junctions OUT IN Total parallel I I I I I I     : Junctions Regarding 3 2 1 ) (
  • 6. Parallel Circuit Notice that the JUNCTIONS both touch the POSTIVE and NEGATIVE terminals of the battery. That means you have the SAME potential difference down EACH individual branch of the parallel circuit. This means that the individual voltages drops are equal. This junction touches the POSITIVE terminal This junction touches the NEGATIVE terminal V                 i P P Parallel T T Total parallel Total parallel R R R R R R R V R V R V R V IR V I I I I V V V V 1 1 1 1 1 1 ) ( ; 3 2 1 3 3 2 2 1 1 3 2 1 ) ( 3 2 1 ) (
  • 7. Example        454 . 0 1 454 . 0 1 9 1 7 1 5 1 1 P p P R R R     ) ( 8 R I IR V To the left is an example of a parallel circuit. a) What is the total resistance? b) What is the total current? c) What is the voltage across EACH resistor? d) What is the current through each resistor? (Apply Ohm's law to each resistor separately) 2.20 W 3.64 A 8 V each!         W W W 9 8 7 8 5 8 9 7 5 I I I IR V 1.6 A 1.14 A 0.90 A Notice that the individual currents ADD to the total.