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UNIT 2
Electric Circuits
AGORA International School
Technology
3 ESO
SERIES AND PARALLEL CIRCUITS
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
οƒ˜ Step 4. Reconstruct the circuit step-by-step while analyzing individual resistors finding voltage
(V) and current (I).
Most circuits are not in a basic series or parallel configuration, but rather consist of a complex
combination of series and parallel resistances. The key to simplifying circuits is to combine complex
arrangements of resistors into one main resistor. The general rules for solving these types of problems
are as follows:
Tip: Redraw the schematic after every step so you don't miss
an opportunity to simplify
SOLVING SERIES-PARALLEL COMBINATION CIRCUITS
R4
R2
R3
R1
ProblemBPart 1: Break it out
ProblemB
R4
R2
R3
R1
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
R2 R1
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R2 R1
We can the equivalent resistance:
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
2) Resistors 3 and 4 are in series.
R3 R4
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
2) Resistors 3 and 4 are in series.
R3 R4
RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω
We can the equivalent resistance:
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
2) Resistors 3 and 4 are in series.
R3 R4
RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω
We can the equivalent resistance:
Redraw the simplified circuit:
RE 1-2
RE 3-4
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
2) Resistors 3 and 4 are in series.
R3 R4
RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω
We can the equivalent resistance:
Redraw the simplified circuit:
RE 1-2
RE 3-4
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
2) Resistors 3 and 4 are in series. 3) Resistors E1-2 and E2-3 are in parallel.
R3 R4
RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω
We can the equivalent resistance:
Redraw the simplified circuit:
RE 1-2
RE 3-4
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
2) Resistors 3 and 4 are in series. 3) Resistors E1-2 and E2-3 are in parallel.
R3 R4
RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω
We can the equivalent resistance:
Redraw the simplified circuit:
RE 1-2
RE 3-4
We can the equivalent resistance:
1
𝑅 𝑇
=
1
𝑅 𝐸1βˆ’2
+
1
𝑅 𝐸3βˆ’4
=
1
4Ξ©
+
1
9Ξ©
1
𝑅 𝑇
= 0,36
1
Ξ©
β†’ RT =
1
0,36
1
Ξ©
= 2,8 𝜴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
2) Resistors 3 and 4 are in series. 3) Resistors E1-2 and E2-3 are in parallel.
R3 R4
RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω
We can the equivalent resistance:
Redraw the simplified circuit:
RE 1-2
RE 3-4
We can the equivalent resistance:
1
𝑅 𝑇
=
1
𝑅 𝐸1βˆ’2
+
1
𝑅 𝐸3βˆ’4
=
1
4Ξ©
+
1
9Ξ©
1
𝑅 𝑇
= 0,36
1
Ξ©
β†’ RT =
1
0,36
1
Ξ©
= 2,8 𝜴
RT
Redraw the simplified circuit:
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
ProblemB
R4
R2
R3
R1
1) Resistors 1 and 2 are in series.
οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or
parallel.
οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE).
οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω
R4
RE 1-2
R3
R2 R1
We can the equivalent resistance:
Redraw the simplified circuit:
2) Resistors 3 and 4 are in series. 3) Resistors E1-2 and E2-3 are in parallel.
R3 R4
RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω
We can the equivalent resistance:
Redraw the simplified circuit:
RE 1-2
RE 3-4
We can the equivalent resistance:
1
𝑅 𝑇
=
1
𝑅 𝐸1βˆ’2
+
1
𝑅 𝐸3βˆ’4
=
1
4Ξ©
+
1
9Ξ©
1
𝑅 𝑇
= 0,36
1
Ξ©
β†’ RT =
1
0,36
1
Ξ©
= 2,8 𝜴
RT
Redraw the simplified circuit:
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
R1 = 2Ω
R2 = 2Ω
R3 = 4Ω
R4 = 5Ω
VT = 6 V
R4
R2
R3
R1
ProblemBPart 2: Build it up
οƒ˜ Step 4. Reconstruct the circuit step-by-step while analyzing
individual resistors finding voltage (V) and current (I).
ProblemB
R4
R2
R3
R1
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 4
R4 5
Total 6 2,8
R1-2 4
R3-4 9
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 4
R4 5
Total 6 2,8
R1-2 4
R3-4 9
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 4
R4 5
Total 6 2,1 2,8
R1-2 4
R3-4 9
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 4
R4 5
Total 6 2,1 2,8
R1-2 4
R3-4 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 4
R4 5
Total 6 2,1 2,8
R1-2 6 4
R3-4 6 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 4
R4 5
Total 6 2,1 2,8
R1-2 6 4
R3-4 6 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 4
R4 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 4
R4 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
R4
RE 1-2
R3
3) Resistors 𝑅3 and 𝑅4
are in series.
Same I’s
Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 0,7 4
R4 0,7 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
R4
RE 1-2
R3
3) Resistors 𝑅3 and 𝑅4
are in series.
Same I’s
Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 0,7 4
R4 0,7 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
R4
RE 1-2
R3
3) Resistors 𝑅3 and 𝑅4
are in series.
Same I’s
Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
To find 𝑉3and 𝑉4I use
Ohm’s law.
𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉
𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 2,8 0,7 4
R4 3,5 0,7 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
R4
RE 1-2
R3
3) Resistors 𝑅3 and 𝑅4
are in series.
Same I’s
Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
To find 𝑉3and 𝑉4I use
Ohm’s law.
𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉
𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 2
R2 2
R3 2,8 0,7 4
R4 3,5 0,7 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
R4
RE 1-2
R3
3) Resistors 𝑅3 and 𝑅4
are in series.
Same I’s
Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
To find 𝑉3and 𝑉4I use
Ohm’s law.
𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉
𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉
R4
R2
R3
R1
4) Resistors 𝑅1 and 𝑅2 are
in series.
Same I’s
Diff V’s
𝐼1 = 1,5 𝐴
𝐼2 = 1,5 𝐴
𝑉1 + 𝑉2 = 6 𝑉
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 1,5 2
R2 1,5 2
R3 2,8 0,7 4
R4 3,5 0,7 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
R4
RE 1-2
R3
3) Resistors 𝑅3 and 𝑅4
are in series.
Same I’s
Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
To find 𝑉3and 𝑉4I use
Ohm’s law.
𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉
𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉
R4
R2
R3
R1
4) Resistors 𝑅1 and 𝑅2 are
in series.
Same I’s
Diff V’s
𝐼1 = 1,5 𝐴
𝐼2 = 1,5 𝐴
𝑉1 + 𝑉2 = 6 𝑉
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 1,5 2
R2 1,5 2
R3 2,8 0,7 4
R4 3,5 0,7 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
R4
RE 1-2
R3
3) Resistors 𝑅3 and 𝑅4
are in series.
Same I’s
Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
To find 𝑉3and 𝑉4I use
Ohm’s law.
𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉
𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉
R4
R2
R3
R1
4) Resistors 𝑅1 and 𝑅2 are
in series.
Same I’s
Diff V’s
𝐼1 = 1,5 𝐴
𝐼2 = 1,5 𝐴
𝑉1 + 𝑉2 = 6 𝑉
To find 𝑉1and 𝑉2I use
Ohm’s law.
𝑉1 = 𝑅1 βˆ™ 𝐼1 = 2 Ω βˆ™ 1,5 A = 3 𝑉
𝑉2 = 𝑅2 βˆ™ 𝐼2 = 2 Ω βˆ™ 1,5 A = 3 𝑉
ProblemB
R4
R2
R3
R1
1) Find total current using Ohm’s law.
𝐼 𝑇 =
𝑉𝑇
𝑅 𝑇
=
6 𝑉
2,8 Ξ©
= 2,1 𝐴RT
Voltage (V) Current (A) Resistance (Ω)
R1 3 1,5 2
R2 3 1,5 2
R3 2,8 0,7 4
R4 3,5 0,7 5
Total 6 2,1 2,8
R1-2 6 1,5 4
R3-4 6 0,7 9
2) Resistors 𝑅 𝐸1βˆ’2
and 𝑅 𝐸3βˆ’4
are in
parallel.
Diff I’s
Same V’s
𝑉𝐸1βˆ’2
= 6 𝑉
𝑉𝐸3βˆ’4
= 6 𝑉
𝐼 𝐸1βˆ’2
+ 𝐼 𝐸3βˆ’4
= 2,1 𝐴
𝑅 𝐸1βˆ’2
𝑅 𝐸3βˆ’4
To find 𝐼 𝐸1βˆ’2
and 𝐼 𝐸3βˆ’4
I use Ohm’s law.
𝐼 𝐸1βˆ’2
=
𝑉𝐸1βˆ’2
𝑅 𝐸1βˆ’2
=
6 𝑉
4 Ξ©
= 1,5 𝐴 𝐼 𝐸3βˆ’4
=
𝑉𝐸3βˆ’4
𝑅 𝐸3βˆ’4
=
6 𝑉
9 Ξ©
= 0,7 𝐴
R4
RE 1-2
R3
3) Resistors 𝑅3 and 𝑅4
are in series.
Same I’s
Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
To find 𝑉3and 𝑉4I use
Ohm’s law.
𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉
𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉
R4
R2
R3
R1
4) Resistors 𝑅1 and 𝑅2 are
in series.
Same I’s
Diff V’s
𝐼1 = 1,5 𝐴
𝐼2 = 1,5 𝐴
𝑉1 + 𝑉2 = 6 𝑉
To find 𝑉1and 𝑉2I use
Ohm’s law.
𝑉1 = 𝑅1 βˆ™ 𝐼1 = 2 Ω βˆ™ 1,5 A = 3 𝑉
𝑉2 = 𝑅2 βˆ™ 𝐼2 = 2 Ω βˆ™ 1,5 A = 3 𝑉

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Simplifying circuits electric circuits presentation buid it up

  • 1. UNIT 2 Electric Circuits AGORA International School Technology 3 ESO
  • 2. SERIES AND PARALLEL CIRCUITS οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. οƒ˜ Step 4. Reconstruct the circuit step-by-step while analyzing individual resistors finding voltage (V) and current (I). Most circuits are not in a basic series or parallel configuration, but rather consist of a complex combination of series and parallel resistances. The key to simplifying circuits is to combine complex arrangements of resistors into one main resistor. The general rules for solving these types of problems are as follows: Tip: Redraw the schematic after every step so you don't miss an opportunity to simplify SOLVING SERIES-PARALLEL COMBINATION CIRCUITS
  • 4. ProblemB R4 R2 R3 R1 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains.
  • 5. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. R2 R1 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 6. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R2 R1 We can the equivalent resistance: R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 7. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 8. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 9. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: 2) Resistors 3 and 4 are in series. R3 R4 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 10. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: 2) Resistors 3 and 4 are in series. R3 R4 RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω We can the equivalent resistance: R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 11. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: 2) Resistors 3 and 4 are in series. R3 R4 RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω We can the equivalent resistance: Redraw the simplified circuit: RE 1-2 RE 3-4 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 12. ProblemB R4 R2 R3 R1 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: 2) Resistors 3 and 4 are in series. R3 R4 RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω We can the equivalent resistance: Redraw the simplified circuit: RE 1-2 RE 3-4
  • 13. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: 2) Resistors 3 and 4 are in series. 3) Resistors E1-2 and E2-3 are in parallel. R3 R4 RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω We can the equivalent resistance: Redraw the simplified circuit: RE 1-2 RE 3-4 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 14. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: 2) Resistors 3 and 4 are in series. 3) Resistors E1-2 and E2-3 are in parallel. R3 R4 RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω We can the equivalent resistance: Redraw the simplified circuit: RE 1-2 RE 3-4 We can the equivalent resistance: 1 𝑅 𝑇 = 1 𝑅 𝐸1βˆ’2 + 1 𝑅 𝐸3βˆ’4 = 1 4Ξ© + 1 9Ξ© 1 𝑅 𝑇 = 0,36 1 Ξ© β†’ RT = 1 0,36 1 Ξ© = 2,8 𝜴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 15. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: 2) Resistors 3 and 4 are in series. 3) Resistors E1-2 and E2-3 are in parallel. R3 R4 RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω We can the equivalent resistance: Redraw the simplified circuit: RE 1-2 RE 3-4 We can the equivalent resistance: 1 𝑅 𝑇 = 1 𝑅 𝐸1βˆ’2 + 1 𝑅 𝐸3βˆ’4 = 1 4Ξ© + 1 9Ξ© 1 𝑅 𝑇 = 0,36 1 Ξ© β†’ RT = 1 0,36 1 Ξ© = 2,8 𝜴 RT Redraw the simplified circuit: 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 16. ProblemB R4 R2 R3 R1 1) Resistors 1 and 2 are in series. οƒ˜ Step 1. Analyze the circuit to find a section in which all resistors are either series or parallel. οƒ˜ Step 2. Reduce series and parallel configurations into equivalent resistances (RE). οƒ˜ Step 3. Continue combining resistors until one, total resistance (RT) remains. RE 1-2 = R1 + R2 = 2 Ω + 2 Ω = 4 Ω R4 RE 1-2 R3 R2 R1 We can the equivalent resistance: Redraw the simplified circuit: 2) Resistors 3 and 4 are in series. 3) Resistors E1-2 and E2-3 are in parallel. R3 R4 RE 3-4 = R3+ R4 = 4 Ω + 5 Ω = 9 Ω We can the equivalent resistance: Redraw the simplified circuit: RE 1-2 RE 3-4 We can the equivalent resistance: 1 𝑅 𝑇 = 1 𝑅 𝐸1βˆ’2 + 1 𝑅 𝐸3βˆ’4 = 1 4Ξ© + 1 9Ξ© 1 𝑅 𝑇 = 0,36 1 Ξ© β†’ RT = 1 0,36 1 Ξ© = 2,8 𝜴 RT Redraw the simplified circuit: 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 R1 = 2Ω R2 = 2Ω R3 = 4Ω R4 = 5Ω VT = 6 V
  • 17. R4 R2 R3 R1 ProblemBPart 2: Build it up οƒ˜ Step 4. Reconstruct the circuit step-by-step while analyzing individual resistors finding voltage (V) and current (I).
  • 18. ProblemB R4 R2 R3 R1 Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 4 R4 5 Total 6 2,8 R1-2 4 R3-4 9
  • 19. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 4 R4 5 Total 6 2,8 R1-2 4 R3-4 9
  • 20. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 4 R4 5 Total 6 2,1 2,8 R1-2 4 R3-4 9
  • 21. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 4 R4 5 Total 6 2,1 2,8 R1-2 4 R3-4 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4
  • 22. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 4 R4 5 Total 6 2,1 2,8 R1-2 6 4 R3-4 6 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4
  • 23. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 4 R4 5 Total 6 2,1 2,8 R1-2 6 4 R3-4 6 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴
  • 24. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 4 R4 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴
  • 25. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 4 R4 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴 R4 RE 1-2 R3 3) Resistors 𝑅3 and 𝑅4 are in series. Same I’s Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
  • 26. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 0,7 4 R4 0,7 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴 R4 RE 1-2 R3 3) Resistors 𝑅3 and 𝑅4 are in series. Same I’s Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉
  • 27. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 0,7 4 R4 0,7 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴 R4 RE 1-2 R3 3) Resistors 𝑅3 and 𝑅4 are in series. Same I’s Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉 To find 𝑉3and 𝑉4I use Ohm’s law. 𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉 𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉
  • 28. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 2,8 0,7 4 R4 3,5 0,7 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴 R4 RE 1-2 R3 3) Resistors 𝑅3 and 𝑅4 are in series. Same I’s Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉 To find 𝑉3and 𝑉4I use Ohm’s law. 𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉 𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉
  • 29. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 2 R2 2 R3 2,8 0,7 4 R4 3,5 0,7 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴 R4 RE 1-2 R3 3) Resistors 𝑅3 and 𝑅4 are in series. Same I’s Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉 To find 𝑉3and 𝑉4I use Ohm’s law. 𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉 𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉 R4 R2 R3 R1 4) Resistors 𝑅1 and 𝑅2 are in series. Same I’s Diff V’s 𝐼1 = 1,5 𝐴 𝐼2 = 1,5 𝐴 𝑉1 + 𝑉2 = 6 𝑉
  • 30. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 1,5 2 R2 1,5 2 R3 2,8 0,7 4 R4 3,5 0,7 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴 R4 RE 1-2 R3 3) Resistors 𝑅3 and 𝑅4 are in series. Same I’s Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉 To find 𝑉3and 𝑉4I use Ohm’s law. 𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉 𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉 R4 R2 R3 R1 4) Resistors 𝑅1 and 𝑅2 are in series. Same I’s Diff V’s 𝐼1 = 1,5 𝐴 𝐼2 = 1,5 𝐴 𝑉1 + 𝑉2 = 6 𝑉
  • 31. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 1,5 2 R2 1,5 2 R3 2,8 0,7 4 R4 3,5 0,7 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴 R4 RE 1-2 R3 3) Resistors 𝑅3 and 𝑅4 are in series. Same I’s Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉 To find 𝑉3and 𝑉4I use Ohm’s law. 𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉 𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉 R4 R2 R3 R1 4) Resistors 𝑅1 and 𝑅2 are in series. Same I’s Diff V’s 𝐼1 = 1,5 𝐴 𝐼2 = 1,5 𝐴 𝑉1 + 𝑉2 = 6 𝑉 To find 𝑉1and 𝑉2I use Ohm’s law. 𝑉1 = 𝑅1 βˆ™ 𝐼1 = 2 Ω βˆ™ 1,5 A = 3 𝑉 𝑉2 = 𝑅2 βˆ™ 𝐼2 = 2 Ω βˆ™ 1,5 A = 3 𝑉
  • 32. ProblemB R4 R2 R3 R1 1) Find total current using Ohm’s law. 𝐼 𝑇 = 𝑉𝑇 𝑅 𝑇 = 6 𝑉 2,8 Ξ© = 2,1 𝐴RT Voltage (V) Current (A) Resistance (Ω) R1 3 1,5 2 R2 3 1,5 2 R3 2,8 0,7 4 R4 3,5 0,7 5 Total 6 2,1 2,8 R1-2 6 1,5 4 R3-4 6 0,7 9 2) Resistors 𝑅 𝐸1βˆ’2 and 𝑅 𝐸3βˆ’4 are in parallel. Diff I’s Same V’s 𝑉𝐸1βˆ’2 = 6 𝑉 𝑉𝐸3βˆ’4 = 6 𝑉 𝐼 𝐸1βˆ’2 + 𝐼 𝐸3βˆ’4 = 2,1 𝐴 𝑅 𝐸1βˆ’2 𝑅 𝐸3βˆ’4 To find 𝐼 𝐸1βˆ’2 and 𝐼 𝐸3βˆ’4 I use Ohm’s law. 𝐼 𝐸1βˆ’2 = 𝑉𝐸1βˆ’2 𝑅 𝐸1βˆ’2 = 6 𝑉 4 Ξ© = 1,5 𝐴 𝐼 𝐸3βˆ’4 = 𝑉𝐸3βˆ’4 𝑅 𝐸3βˆ’4 = 6 𝑉 9 Ξ© = 0,7 𝐴 R4 RE 1-2 R3 3) Resistors 𝑅3 and 𝑅4 are in series. Same I’s Diff V’s𝐼3 = 0,7 𝐴 𝐼4 = 0,7 𝐴 𝑉3 + 𝑉4 = 6 𝑉 To find 𝑉3and 𝑉4I use Ohm’s law. 𝑉3 = 𝑅3 βˆ™ 𝐼3 = 4 Ω βˆ™ 0,7 A = 2,8 𝑉 𝑉4 = 𝑅4 βˆ™ 𝐼4 = 5 Ω βˆ™ 0,7 A = 3,5 𝑉 R4 R2 R3 R1 4) Resistors 𝑅1 and 𝑅2 are in series. Same I’s Diff V’s 𝐼1 = 1,5 𝐴 𝐼2 = 1,5 𝐴 𝑉1 + 𝑉2 = 6 𝑉 To find 𝑉1and 𝑉2I use Ohm’s law. 𝑉1 = 𝑅1 βˆ™ 𝐼1 = 2 Ω βˆ™ 1,5 A = 3 𝑉 𝑉2 = 𝑅2 βˆ™ 𝐼2 = 2 Ω βˆ™ 1,5 A = 3 𝑉