Circuit Analysis 1: cram pack

Formula sheets, the key method steps for every topic and 14 practice problems, with full solutions at the back.

New problems Back to the course

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1Formulas and methods

Series & parallel resistors

Resistors in series: R_eq = R₁ + R₂ + …
Resistors in parallel: 1/R_eq = 1/R₁ + 1/R₂ + …
Two in parallel: R_eq = R₁R₂ / (R₁ + R₂)
Ohm's law: V = I·R
Power: P = V·I = I²R = V²/R

Method

Start at the end of the network furthest from the terminals.
Combine resistors in series by adding them, and resistors in parallel with 1/R = 1/R₁ + 1/R₂ + …
Redraw the circuit after each step.
Repeat until one resistor is left between the terminals.

Nodal analysis

Kirchhoff’s current law: ΣI_in = ΣI_out
Branch current: I = (V_a − V_b)/R
Reference node: V_ground = 0

Method

Choose a reference node (ground) and label the other node voltages.
Write Kirchhoff’s current law at every unknown node: currents leaving through each branch equal the currents entering.
Express every branch current as (V_a − V_b)/R.
Solve the system of equations, then find any current you need.

Mesh analysis

Kirchhoff’s voltage law: ΣV = 0 around every loop
Shared resistor: current = I₁ − I₂
Current source in a mesh: fixes that mesh current

Method

Draw a clockwise current in every mesh (window) of the circuit.
Apply Kirchhoff’s voltage law around each mesh: the sum of voltage drops is zero.
In a resistor shared by two meshes the current is the difference of the two mesh currents.
Solve the equations; a negative result means the current flows the other way.

Superposition

Superposition: x = x₁ + x₂ + … (one source at a time)
Switched-off voltage source: short circuit (0 V)
Switched-off current source: open circuit (0 A)
Voltage divider: V₂ = V·R₂/(R₁ + R₂)
Current divider: I₁ = I·R₂/(R₁ + R₂)

Method

Count the independent sources. You will solve one simpler circuit per source.
Keep one source and switch off the others: a voltage source becomes a short circuit (a wire), a current source becomes an open circuit (a gap).
Solve the simpler circuit for the voltage or current you need, keeping track of its direction.
Repeat for every source, then add the contributions with their signs.

Thévenin & Norton

Thévenin voltage: V_th = V_{open circuit}
Thévenin resistance: R_th: all sources off, seen from a–b
Norton current: I_N = V_th/R_th
Load current: I_L = V_th/(R_th + R_L)
Maximum power transfer: R_L = R_th, P_max = V_th²/(4R_th)

Method

Remove the load and mark the two terminals a and b.
Find the open-circuit voltage between a and b: this is V_th.
Switch off all independent sources and find the resistance seen from a–b: this is R_th.
Put the load back on the equivalent circuit: V_th in series with R_th.
For the Norton equivalent, convert: I_N = V_th/R_th, with R_N = R_th in parallel.

Op-amp circuits

Inverting amplifier: V_out = −(R_f/R_in)·V_in
Non-inverting amplifier: V_out = (1 + R_f/R₁)·V_in
Summing amplifier: V_out = −R_f(V₁/R₁ + V₂/R₂)
Ideal op-amp: V₊ = V₋, I_in = 0

RC & RL transients

Time constant: τ = RC | τ = L/R
Response: x(t) = x(∞) + [x(0) − x(∞)]·e^−t/τ
Capacitor at DC: open circuit; v_C cannot jump
Inductor at DC: short circuit; i_L cannot jump
Settled: t ≈ 5τ

Method

Find the initial value just after switching: a capacitor voltage and an inductor current cannot jump.
Find the final value long after switching: a capacitor acts as an open circuit, an inductor as a short circuit.
Find the time constant: τ = RC or τ = L/R, using the resistance seen by the capacitor or inductor.
Use x(t) = x(∞) + [x(0) − x(∞)]·e^−t/τ.

2Practice problems

1.Series & parallel resistorsMedium

Find the current I_R2 through R₂.

V₁ = 15 VR₁ = 20 ΩR₂ = 10 ΩR₃ = 20 ΩR₄ = 4 Ω

I_R2 = A

2.Series & parallel resistorsHard

Find the current I_R2 through R₂.

V₁ = 6 VR₁ = 3 ΩR₂ = 20 ΩR₃ = 30 ΩR₄ = 6 ΩR₅ = 8 ΩR₆ = 25 Ω

I_R2 = A

3.Nodal analysisMedium

Use nodal analysis to find the power P_Is delivered by the current source I_s.

V₁ = 10 VI_s = 1.5 AR₁ = 15 ΩR₂ = 4 ΩR₃ = 4 ΩR₄ = 15 Ω

P_Is = W

4.Nodal analysisHard

Use nodal analysis to find the node voltage V_B (measured from ground).

V₁ = 18 VI_s = 0.5 AV₂ = 18 VR₁ = 3 ΩR₂ = 12 ΩR₃ = 8 ΩR₄ = 25 ΩR₅ = 2 Ω

V_B = V

5.Mesh analysisMedium

Use mesh analysis to find the mesh current I₂ (clockwise).

V₁ = 6 VV₂ = 24 VR₁ = 5 ΩR₂ = 20 ΩR₃ = 3 Ω

I₂ = A

6.Mesh analysisHard

Use mesh analysis to find the current I_R5 through R₅ in the direction of the arrow.

V₁ = 12 VV₂ = 9 VR₁ = 30 ΩR₂ = 2 ΩR₃ = 8 ΩR₄ = 10 ΩR₅ = 12 Ω

I_R5 = A

7.SuperpositionMedium

Use superposition to find the current I_R2 through R₂ in the direction of the arrow.

V₁ = 30 VI_s = 1 AR₁ = 15 ΩR₂ = 20 ΩR₃ = 15 ΩR₄ = 5 Ω

I_R2 = A

8.SuperpositionHard

Find the value of the voltage source V₂ (polarity as shown) that makes the current I_R3 through R₃ equal to zero.

V₁ = 36 VI_s = 3 AR₁ = 30 ΩR₂ = 3 ΩR₃ = 30 ΩR₄ = 10 Ω

V₂ = V

9.Thévenin & NortonMedium

Find the Thévenin resistance R_th seen from terminals a–b.

V₁ = 6 VR₁ = 5 ΩR₂ = 3 ΩR₃ = 2 Ω

R_th = Ω

10.Thévenin & NortonHard

Find the Thévenin voltage V_th seen from terminals a–b.

V₁ = 30 VI_s = 6 AR₁ = 2 ΩR₂ = 10 ΩR₃ = 25 Ω

V_th = V

11.Op-amp circuitsMedium

The op-amp is ideal and runs from ±15 V supplies. Find the output voltage V_out.

V_in = 0.3 VR₁ = 1 kΩR_f = 10 kΩ

V_out = V

12.Op-amp circuitsHard

The op-amp is ideal and runs from ±15 V supplies. The resistor ratios are not matched. Find the output voltage V_out.

V₁ = 0.9 VV₂ = 0.6 VR₁ = 100 kΩR₂ = 2 kΩR₃ = 10 kΩR₄ = 22 kΩ

V_out = V

13.RC & RL transientsMedium

The inductor carries no current before the switch closes at t = 0. Find the voltage v_L across the inductor at t = 5 ms.

V_s = 5 VR = 100 ΩL = 220 mHt = 5 ms

v_L = V

14.RC & RL transientsHard

A timer starts charging an uncharged capacitor through a resistor from a 9 V supply at t = 0. It must trigger when the capacitor voltage reaches 6.75 V, exactly 200 ms after the start. With R = 4.7 kΩ, find the capacitance C needed.

V_s = 9 VV_th = 6.75 VT = 200 msR = 4.7 kΩ

C = µF

3Solutions

1.Series & parallel resistors

Answer: I_R2 = 0.3913 A

Series and parallel resistors: in series the same current flows through each resistor and R = R₁ + R₂ + …. In parallel each resistor has the same voltage and 1/R = 1/R₁ + 1/R₂ + …. A ladder network is reduced one pair at a time until a single equivalent resistance remains.

Combine resistors from the far end

Start at the end farthest from the source and work back towards it. Resistors carrying the same current are in series; resistors across the same two nodes are in parallel.

R₃ + R₄ = 20 + 4 = 24 Ω

R₂ ∥ 24 = 10·24/(10+24) = 7.059 Ω

R_eq = R₁ + 7.059 = 20 + 7.059 = 27.06 Ω

Current from the source

The source sees only R_eq, so Ohm’s law gives the current it delivers. That current flows through R₁.

I_R1 = V₁/R_eq = 15/27.06 = 0.5543 A

Current through R₂

Subtract the drop across R₁ to get the voltage at node A, which is the voltage across R₂.

V_A = V₁ − I_R1·R₁ = 15 − 0.5543·20 = 3.913 V

I_R2 = V_A/R₂ = 3.913/10 = 0.3913 A

Answer

I_R2 = 0.3913 A

2.Series & parallel resistors

Answer: I_R2 = 0.2428 A

Combine resistors from the far end

Start at the end farthest from the source and work back towards it. Resistors carrying the same current are in series; resistors across the same two nodes are in parallel.

R₅ + R₆ = 8 + 25 = 33 Ω

R₄ ∥ 33 = 5.077 Ω

R₃ + 5.077 = 35.08 Ω

R₂ ∥ 35.08 = 12.74 Ω

R_eq = R₁ + 12.74 = 3 + 12.74 = 15.74 Ω

Current from the source

The source sees only R_eq, so Ohm’s law gives the current it delivers. That current flows through R₁.

I_R1 = V₁/R_eq = 6/15.74 = 0.3813 A

Current through R₂

Subtract the drop across R₁ to get the voltage at node A, which is the voltage across R₂.

V_A = V₁ − I_R1·R₁ = 6 − 0.3813·3 = 4.856 V

I_R2 = V_A/R₂ = 4.856/20 = 0.2428 A

Answer

I_R2 = 0.2428 A

3.Nodal analysis

Answer: P_Is = 13.04 W

Nodal analysis: choose a reference node, label the unknown node voltages, write Kirchhoff’s current law at each unknown node using Ohm’s law (I = ΔV/R), and solve the resulting equations.

KCL at node A

Currents leaving A through the resistors equal the current pushed into A by sources.

V_A/R₂ + (V_A − V₁)/R₁ + (V_A − V_B)/R₃ = 0

V_A/4 + (V_A − 10)/15 + (V_A − V_B)/4 = 0

0.5667·V_A − 0.25·V_B = 0.6667

KCL at node B

Currents leaving B through the resistors equal the current pushed into B by sources.

V_B/R₄ + (V_B − V_A)/R₃ = I_s

V_B/15 + (V_B − V_A)/4 = 1.5

−0.25·V_A + 0.3167·V_B = 1.5

Solve

Δ = (0.5667)(0.3167) − (−0.25)(−0.25) = 0.1169

V_A = Δ₁/Δ = 0.5861/0.1169 = 5.012 V

V_B = Δ₂/Δ = 1.017/0.1169 = 8.694 V

Power delivered by the current source

The source pushes Iₛ up into node B, from ground (0 V) to V_B. A source whose current leaves its + end delivers P = V·I.

P_Is = V_B·I_s = 8.694·1.5 = 13.04 W

Answer

P_Is = 13.04 W

4.Nodal analysis

Answer: V_B = 3.51 V

Nodal analysis: choose a reference node, label the unknown node voltages, write Kirchhoff’s current law at each unknown node using Ohm’s law (I = ΔV/R), and solve the resulting equations.

Set up the nodes

Ground is the bottom wire. Known node voltages come straight from the sources (V₁ = 18 V, V₂ = 18 V). Unknowns: V_A, V_B.

KCL at node A

Currents leaving A through the resistors equal the current pushed into A by sources.

V_A/R₃ + (V_A − V₁)/R₁ + (V_A − V_B)/R₂ = 0

V_A/8 + (V_A − 18)/3 + (V_A − V_B)/12 = 0

0.5417·V_A − 0.08333·V_B = 6

KCL at node B

Currents leaving B through the resistors equal the current pushed into B by sources.

V_B/R₅ + (V_B − V_A)/R₂ + (V_B − V₂)/R₄ = I_s

V_B/2 + (V_B − V_A)/12 + (V_B − 18)/25 = 0.5

−0.08333·V_A + 0.6233·V_B = 1.22

Solve

Δ = (0.5417)(0.6233) − (−0.08333)(−0.08333) = 0.3307

V_A = Δ₁/Δ = 3.842/0.3307 = 11.62 V

V_B = Δ₂/Δ = 1.161/0.3307 = 3.51 V

Answer

V_B = 3.51 V

5.Mesh analysis

Answer: I₂ = −0.9943 A

Mesh analysis: give each window of a planar circuit its own loop current, write Kirchhoff’s voltage law around each loop (sum of drops = sum of rises), and solve. Branch currents are the mesh current, or the difference of two mesh currents on a shared branch.

Assign mesh currents

Draw a clockwise current in each window: I₁, I₂. A resistor shared by two meshes carries the difference of their currents.

KVL around mesh 1

Going clockwise, the voltage drops across resistors equal the source voltage rises (− to + in the direction of travel).

R₁·I₁ + R₃(I₁ − I₂) = V₁

5·I₁ + 3(I₁ − I₂) = 6

8·I₁ − 3·I₂ = 6

KVL around mesh 2

Going clockwise, the voltage drops across resistors equal the source voltage rises (− to + in the direction of travel).

R₂·I₂ + R₃(I₂ − I₁) = −V₂

20·I₂ + 3(I₂ − I₁) = (−24)

−3·I₁ + 23·I₂ = −24

Solve

Δ = (8)(23) − (−3)(−3) = 175

I₁ = Δ₁/Δ = 66/175 = 0.3771 A

I₂ = Δ₂/Δ = −174/175 = −0.9943 A

Answer

I₂ = −0.9943 A

A negative mesh current flows anticlockwise.

6.Mesh analysis

Answer: I_R5 = 0.3829 A

Assign mesh currents

Draw a clockwise current in each window: I₁, I₂, I₃. A resistor shared by two meshes carries the difference of their currents.

KVL around mesh 1

Going clockwise, the voltage drops across resistors equal the source voltage rises (− to + in the direction of travel).

R₁·I₁ + R₄(I₁ − I₂) = V₁

30·I₁ + 10(I₁ − I₂) = 12

40·I₁ − 10·I₂ = 12

KVL around mesh 2

Going clockwise, the voltage drops across resistors equal the source voltage rises (− to + in the direction of travel).

R₂·I₂ + R₄(I₂ − I₁) + R₅(I₂ − I₃) = 0

2·I₂ + 10(I₂ − I₁) + 12(I₂ − I₃) = 0

−10·I₁ + 24·I₂ − 12·I₃ = 0

KVL around mesh 3

Going clockwise, the voltage drops across resistors equal the source voltage rises (− to + in the direction of travel).

R₃·I₃ + R₅(I₃ − I₂) = −V₂

8·I₃ + 12(I₃ − I₂) = (−9)

−12·I₂ + 20·I₃ = −9

Solve

Δ = det of the coefficient matrix = 11440

I₁ = Δ₁/Δ = 2952/11440 = 0.258 A

I₂ = Δ₂/Δ = −1920/11440 = −0.1678 A

I₃ = Δ₃/Δ = −6300/11440 = −0.5507 A

Answer

I_R5 = I₂ − I₃ = 0.3829 A

A negative mesh current flows anticlockwise.

7.Superposition

Answer: I_R2 = 0.675 A

Superposition: in a linear circuit, any voltage or current is the sum of the responses to each independent source acting alone. To switch a source off, replace an ideal voltage source with a short circuit and an ideal current source with an open circuit. Resistors stay where they are.

Case 1 · V₁ acting alone

Iₛ becomes an open circuit, so R₃ and R₄ form one series branch from A to ground, in parallel with R₂.

R₃+R₄ = 15+5 = 20 Ω

R₂ ∥ (R₃+R₄) = 20·20/(20+20) = 10 Ω

V_A = 30·10/(15+10) = 12 V

V_B = V_A·R₄/(R₃+R₄) = 12·5/20 = 3 V

I_R2′ = (V_A − 0)/R₂ = (12 − 0)/20 = 0.6 A

Case 2 · I_s acting alone

V₁ becomes a short, so R₁ is in parallel with R₂. Iₛ splits at B between R₄ and the path through R₃.

R₁ ∥ R₂ = 15·20/(15+20) = 8.571 Ω

R_eq = R₄ ∥ (R₃+R₁∥R₂) = 5 ∥ 23.57 = 4.125 Ω

V_B = I_s·R_eq = 1·4.125 = 4.125 V

V_A = V_B·(R₁∥R₂)/(R₃+R₁∥R₂) = 4.125·8.571/23.57 = 1.5 V

I_R2″ = (V_A − 0)/R₂ = (1.5 − 0)/20 = 0.075 A

Add the contributions

I_R2 = I_R2′ + I_R2″

I_R2 = 0.6 + 0.075 = 0.675 A

A negative result means the real current flows against the arrow.

8.Superposition

Answer: V₂ = 14.4 V

Case 1 · V₁ acting alone

V₂ becomes a short and Iₛ an open circuit. Seen from A, R₃ is in parallel with the series pair R₂+R₄.

R₃ ∥ (R₂+R₄) = 30 ∥ 13 = 9.07 Ω

V_A = 36·9.07/(30+9.07) = 8.357 V

V_B = V_A·R₄/(R₂+R₄) = 8.357·10/13 = 6.429 V

Case 2 · I_s acting alone

Both voltage sources become shorts. Iₛ splits at B between R₄ (now to ground) and R₂ in series with R₁ ∥ R₃. The arrow of Iₛ points down, away from its node, so Iₛ draws current out of that node: its term enters with a minus sign.

R₁ ∥ R₃ = 15 Ω, so the left path is R₂+15 = 18 Ω

R_eq = R₄ ∥ 18 = 6.429 Ω

V_B = −I_s·R_eq = −3·6.429 = −19.29 V

V_A = V_B·15/18 = −16.07 V

Case 3 · V₂ acting alone, per volt

V₁ becomes a short and Iₛ an open circuit. R₁ ∥ R₃ hangs from A, in series with R₂ back to B.

R₁ ∥ R₃ = 15 Ω

V_A‴ = V₂·15/(10 + 3 + 15) = 0.5357·V₂

Set V_A to zero

With V_A = 0 there is no voltage across R₃, so its current is zero.

V_A′ + V_A″ + V_A‴ = 8.357 + (−16.07) + 0.5357·V₂ = 0

V₂ = 7.714/0.5357 = 14.4 V

Answer

V₂ = 14.4 V

9.Thévenin & Norton

Answer: R_th = 3.875 Ω

Thévenin’s theorem: any linear two-terminal network behaves like a single voltage source V_th in series with a resistance R_th. Norton’s theorem gives the same network as a current source I_N = V_th/R_th in parallel with R_th.

Find R_th with every source switched off

Replace voltage sources with shorts and current sources with opens, then look into the circuit from a–b.

R₁ ∥ R₂ = 5·3/(5+3) = 1.875 Ω

R_th = (R₁ ∥ R₂) + R₃ = 1.875 + 2 = 3.875 Ω

10.Thévenin & Norton

Answer: V_th = 185 V

Find R_th with every source switched off

Replace voltage sources with shorts and current sources with opens, then look into the circuit from a–b.

R₁ ∥ R₂ = 2·10/(2+10) = 1.667 Ω

R_th = (R₁ ∥ R₂) + R₃ = 1.667 + 25 = 26.67 Ω

Find V_th, the open-circuit voltage

With a–b open, the only path for Iₛ is through R₃ into node A. Find V_A by superposition of V₁ and Iₛ, then add the drop across R₃.

V_A = V₁·R₂/(R₁+R₂) + I_s·(R₁∥R₂) = 25 + 6·1.667 = 35 V

V_th = V_B = V_A + I_s·R₃ = 35 + 6·25 = 185 V

11.Op-amp circuits

Answer: V_out = 3.3 V

Ideal op-amp rules: with negative feedback, the op-amp drives its output so that its two inputs sit at the same voltage (V₋ = V₊), and no current flows into either input. Writing KCL at the inverting input with these two facts gives the output.

Inverting input follows the input

V₋ = V₊ = 0.3 V

I = V₋/R₁ = 0.3/1 = 0.3 mA

Output voltage

The current through R₁ also flows through R_f.

V_out = V₋ + I·R_f = 0.3 + 0.3·10 = 3.3 V

Answer

V_out = 3.3 V

12.Op-amp circuits

Answer: V_out = 0.4027 V

Voltage at the + input

V₊ = V₂·R₄/(R₃ + R₄) = 0.6·22/(10 + 22) = 0.4125 V

Superpose the two inputs

With V₂ = 0, V₁ sees an inverting amplifier. With V₁ = 0, V₊ is amplified by the non-inverting gain 1 + R₂/R₁.

V_out = −(2/100)·0.9 + (1 + 2/100)·0.4125 = −0.018 + 0.4207 = 0.4027 V

Answer

V_out = 0.4027 V

13.RC & RL transients

Answer: v_L = 0.5152 V

First-order transients: in a circuit with one capacitor or one inductor, every voltage and current moves exponentially from its initial value to its final value: x(t) = x(∞) + [x(0) − x(∞)]·e^−t/τ, with τ = RC or τ = L/R. After about 5τ the circuit has settled.

Time constant and final current

Long after the switch closes the inductor behaves like a short circuit, so the final current is set by R alone.

τ = L/R = 220 mH / 100 Ω = 2.2 ms

i(∞) = V_s/R = 5/100 = 0.05 A

Inductor voltage

At t = 0 the whole supply voltage appears across the inductor; it then decays to zero.

v_L(t) = V_s·e^−t/τ = 5·e^−5/2.2 = 0.5152 V

Answer

v_L = 0.5152 V

14.RC & RL transients

Answer: C = 30.7 µF

Required time constant

6.75 = 9·(1 − e^−200/τ) → τ = 200/ln(9/(9 − 6.75))

τ = 200/1.386 = 144.3 ms

Capacitance

kΩ times µF gives milliseconds.

C = τ/R = 144.3/4.7 = 30.7 µF

Answer

C = 30.7 µF

ExamProblems · examproblems.com/courses/circuit-analysis-1

Circuit Analysis 1: cram pack

1Formulas and methods

Series & parallel resistors

Method

Nodal analysis

Method

Mesh analysis

Method

Superposition

Method

Thévenin & Norton

Method

Op-amp circuits

RC & RL transients

Method

2Practice problems

3Solutions

Combine resistors from the far end

Current from the source

Current through R₂

Answer

Combine resistors from the far end

Current from the source

Current through R₂

Answer

KCL at node A

KCL at node B

Solve

Power delivered by the current source

Answer

Set up the nodes

KCL at node A

KCL at node B

Solve

Answer

Assign mesh currents

KVL around mesh 1

KVL around mesh 2

Solve

Answer

Assign mesh currents

KVL around mesh 1

KVL around mesh 2

KVL around mesh 3

Solve

Answer

Case 1 · V1 acting alone

Case 2 · Is acting alone

Add the contributions

Case 1 · V1 acting alone

Case 2 · Is acting alone

Case 3 · V2 acting alone, per volt

Set VA to zero

Answer

Find Rth with every source switched off

Find Rth with every source switched off

Find Vth, the open-circuit voltage

Inverting input follows the input

Output voltage

Answer

Voltage at the + input

Superpose the two inputs

Answer

Time constant and final current

Inductor voltage

Answer

Required time constant

Capacitance

Answer

Case 1 · V₁ acting alone

Case 2 · I_s acting alone

Case 1 · V₁ acting alone

Case 2 · I_s acting alone

Case 3 · V₂ acting alone, per volt

Set V_A to zero

Find R_th with every source switched off

Find R_th with every source switched off

Find V_th, the open-circuit voltage