Electronics 1: cram pack

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

New problemsBack to the course

In the print window, choose “Save as PDF” to keep a copy on your device.

1Formulas and methods

Diodes & transistors

Diode (constant drop)
VD = 0.7 V when conducting
Active region
VBE = 0.7 V, IC = β·IB, IE = (β + 1)·IB
Fixed bias
IB = (VCC − 0.7)/RB
Divider bias
IB = (VTH − 0.7)/(RTH + (β + 1)RE)
Thévenin of the divider
VTH = VCC·R2/(R1 + R2), RTH = R1∥R2
Collector loop
VCE = VCC − ICRC − IERE
Saturation
IC(sat) = (VCC − VCE(sat))/RC, IB ≥ IC(sat)/β

Op-amp circuits

Inverting amplifier
Vout = −(Rf/Rin)·Vin
Non-inverting amplifier
Vout = (1 + Rf/R1)·Vin
Summing amplifier
Vout = −Rf(V1/R1 + V2/R2)
Ideal op-amp
V+ = V−, Iin = 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; vC cannot jump
Inductor at DC
short circuit; iL cannot jump
Settled
t ≈ 5τ

Method

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

Series & parallel resistors

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

Method

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

DC-DC converters

Buck
Vo = D·Vin
Boost
Vo = Vin/(1 − D)
Inverting buck-boost
|Vo| = Vin·D/(1 − D)
Ideal power balance
VinIin = VoIo
Inductor ripple
ΔIL = VL,on·D/(L·f); buck Vin − Vo, boost and buck-boost Vin
Average inductor current
buck Io; boost and buck-boost Io/(1 − D)
Output ripple
buck ΔIL/(8fC); boost and buck-boost Io·D/(fC)
CCM boundary
buck (1 − D)R/(2f); boost D(1 − D)²R/(2f); buck-boost (1 − D)²R/(2f)

Method

  1. Identify the converter (buck, boost or buck-boost) and the duty cycle D from the voltage ratio.
  2. Use volt-second balance on the inductor: the average inductor voltage over a period is zero.
  3. Find the inductor voltage while the switch is on, then ΔIL = VL·D/(L·f).
  4. For the output ripple, find the charge that flows in and out of the capacitor; for the CCM boundary, set the average inductor current equal to ΔIL/2.

Wheatstone bridge & strain gauges

Divider voltages
Va = VsR2/(R1 + R2), Vb = VsR4/(R3 + R4)
Output
Vab = Va − Vb
Balance
R1/R2 = R3/R4
Slide-wire bridge
R/Rx = l/(100 − l)
Thévenin resistance
Rth = R1∥R2 + R3∥R4
Gauge factor
ΔR/R = GF·ε
Bridge output
quarter Vs·GF·ε/4, half Vs·GF·ε/2, full Vs·GF·ε
Small change, one arm
Vab ≈ Vs·ΔR/(4R)
Stress
σ = E·ε

Method

  1. Treat the bridge as two voltage dividers across the same supply.
  2. For balance, set R₁/R₂ = R₃/R₄ and solve for the unknown resistor.
  3. For an unbalanced bridge, find Va and Vb from the dividers and subtract; use the Thévenin equivalent when a meter loads the output.
  4. For strain gauges, convert strain to ΔR/R = GF·ε and use Vs·GF·ε/4, /2 or ×1 for a quarter, half or full bridge.

Digital logic: gates, K-maps & flip-flops

Basic gates
A·B, A + B, A′, (A·B)′, (A + B)′, A ⊕ B
Boolean rules
X + X′ = 1, X·X′ = 0, X + XY = X, XY + XY′ = X
De Morgan
(X·Y)′ = X′ + Y′, (X + Y)′ = X′·Y′
Karnaugh map order
00, 01, 11, 10 (Gray code)
Group of 2ᵏ cells
loses k variables
4-to-1 multiplexer
F = A′B′I0 + A′BI1 + AB′I2 + ABI3
Flip-flops
D: Q⁺ = D, T: Q⁺ = T ⊕ Q, JK: Q⁺ = JQ′ + K′Q
Counters
n-bit: 2ⁿ states; mod-N: smallest n with 2ⁿ ≥ N; fout = fclk/N
Ripple counter
fmax = 1/(n·tpd)
Ring and Johnson counters
n and 2n states

Method

  1. For a circuit, work from the inputs to the output one gate at a time and write the value on every wire, or write its expression and fill in the truth table.
  2. For simplification, put the 1s (and the don’t-cares as X) into a Karnaugh map with Gray-code rows and columns: 00, 01, 11, 10.
  3. Cover the 1s with as few and as large groups of 1, 2, 4, 8 or 16 cells as possible, wrapping round the edges; each group is one product term made of the variables that stay constant. Group the 0s for the POS form.
  4. For flip-flops and counters, read the inputs at each active clock edge, write the state after every edge, and remember that an n-bit counter wraps round after 2ⁿ states.

2Practice problems

1.Diodes & transistorsMedium
+−15 V100 Ω12 V3300 ΩIZ​ = ?

A 12 V Zener regulator is fed from 15 V through 100 Ω and supplies a 3300 Ω load. Find the Zener current IZ.

Vin = 15 VVZ = 12 VR = 100 ΩRL = 3300 Ω
IZ = mA
2.Diodes & transistorsHard
RC​ = 470 Ωβ = 50IC​ = ?VCC​ = 12 V5 VRB​ = 2.2 kΩ

An NPN transistor with β = 50 switches a 470 Ω load resistor connected between VCC = 12 V and its collector. The emitter is grounded. The base is driven from a 5 V logic output through a base resistor RB = 2.2 kΩ. Take VBE = 0.7 V and VCE(sat) = 0.2 V. Find the collector current IC in mA when the input is high. Decide first whether the transistor is saturated.

VCC = 12 VRC = 470 Ωβ = 50Vin = 5 VVBE = 0.7 VVCE(sat) = 0.2 VRB = 2.2 kΩ
IC = mA
3.Op-amp circuitsMedium
−+Vout​Rf​ = ?R1​ = 100 kΩVin​

Choose the feedback resistor Rf that gives this non-inverting amplifier a voltage gain of 25.

R1 = 100 kΩAv = 25
Rf = kΩ
4.Op-amp circuitsHard
−+Vout​Rf​ = 4.7 kΩV1​ = 0.8 VR1​ = 1 kΩV2​ = −1.3 VR2​ = 22 kΩ

The summing amplifier uses an ideal op-amp with ±15 V supplies. Find the output voltage Vout.

V1 = 0.8 VV2 = −1.3 VR1 = 1 kΩR2 = 22 kΩRf = 4.7 kΩ
Vout = V
5.RC & RL transientsMedium
+−Vs​20 Vt = 0R = 33 ΩL68 mHi(t)

The inductor carries no current before the switch closes at t = 0. How long after the switch closes does the current reach 75% of its final value? Find t.

Vs = 20 VR = 33 ΩL = 68 mH
t = ms
6.RC & RL transientsHard
+−Vs​9 Vt = 0R = ?C22 µF+−vC​

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 8.1 V, exactly 250 ms after the start. With C = 22 µF, find the resistance R needed.

Vs = 9 VVth = 8.1 VT = 250 msC = 22 µF
R = kΩ
7.Series & parallel resistorsMedium
R1​ = 4 ΩR3​ = 8 Ω+−V1​12 VR2​4 ΩIR2​AR4​20 ΩB

Find the current IR2 through R2.

V1 = 12 VR1 = 4 ΩR2 = 4 ΩR3 = 8 ΩR4 = 20 Ω
IR2 = A
8.Series & parallel resistorsHard
R1​ = 15 ΩR3​ = 25 ΩR5​ = 4 Ω+−V1​30 VR2​4 ΩAR4​5 ΩBR6​20 Ω

Find the equivalent resistance Req seen by the source V1.

V1 = 30 VR1 = 15 ΩR2 = 4 ΩR3 = 25 ΩR4 = 5 ΩR5 = 4 ΩR6 = 20 Ω
Req = Ω
9.DC-DC convertersMedium
tiL​Imax​ = ?Imin​Io​DTT2T

A buck converter turns 24 V into 16.8 V for a 4 Ω load. It switches at 500 kHz with L = 47 µH. Find the peak inductor current Imax.

Vin​ = 24 VVo​ = 16.8 Vf = 500 kHzL = 47 µHR = 4 Ω
Imax = A
10.DC-DC convertersHard
tvo​Vo​ΔV = ?DTT2T

A buck converter turns 12 V into 7.2 V for a 25 Ω load at 200 kHz, with L = 68 µH and C = 22 µF. Find the peak-to-peak output voltage ripple ΔVo in mV.

Vin​ = 12 VVo​ = 7.2 Vf = 200 kHzL = 68 µHC = 22 µF
ΔVo = mV
11.Wheatstone bridge & strain gaugesMedium
+−2 VR1​ = 150 ΩR2​ = 60 ΩR3​ = 20 ΩR4​ = 300 Ωab+−Rth​ = ?

Find the Thévenin resistance Rth of the bridge shown, seen from the output terminals a and b.

Vs = 2 VR1 = 150 ΩR2 = 60 ΩR3 = 20 ΩR4 = 300 Ω
Rth = Ω
12.Wheatstone bridge & strain gaugesHard
+−10 V350 Ω − ΔR350 Ω + ΔR350 Ω + ΔR350 Ω − ΔRab+−Vo​ = ?

A bridge with 350 Ω arms is excited with 10 V and has four active gauges, two in tension and two in compression (full bridge). The gauge factor is 2.05 and the strain is 200 µε. Find the bridge output Vo in mV.

Vs = 10 VGF = 2.05ε = 200 µε
Vo = mV
13.Digital logic: gates, K-maps & flip-flopsMedium
MUXC′I0​C′I1​CI2​1I3​ABS1​S0​F

A 4-to-1 multiplexer has its select inputs S₁ = A and S₀ = B, and its data inputs tied to I₀ = C′, I₁ = C′, I₂ = C, I₃ = 1. For how many of the 8 combinations of A, B and C is the output F = 1? Find N.

I₀ = C′I₁ = C′I₂ = CI₃ = 1
N =
14.Digital logic: gates, K-maps & flip-flopsHard
ABCD00011110000111100001X3121405171601201301501408X9111010

For F(A, B, C, D) = Σm(2, 4, 6, 7, 11) + d(3, 9), where d marks the don't-care conditions, find the number N of essential prime implicants.

F(A, B, C, D) = Σm(2, 4, 6, 7, 11) + d(3, 9)
N =

3Solutions

1.Diodes & transistors

Answer: IZ = 26.36 mA

Zener regulator: a reverse-biased Zener diode holds its voltage VZ while its current stays above a minimum IZ,min. The series resistor R takes the difference between input and output: IR = (Vin − VZ)/R. That current splits between the load, IL = VZ/RL, and the Zener: IZ = IR − IL. Design for the worst cases: the lowest input with the largest load must still leave IZ,min, and the highest input with no load gives the largest Zener power PZ = VZ·IZ.

Resistor current

IR = 3/100 = 30 mA

Load current

IL = 12/3300 = 3.636 mA

Zener current

IZ = 30 − 3.636 = 26.36 mA

Answer

IZ = 26.36 mA
2.Diodes & transistors

Answer: IC = 25.11 mA

BJT as a switch: to switch a load fully on, the transistor is driven into saturation, where VCE = VCE(sat) and the collector current is set by the load: IC(sat) = (VCC − VCE(sat))/RC. Saturation needs at least IB = IC(sat)/β. If the base current is smaller, the transistor stays active and IC = β·IB.

Base current

IB = (5 − 0.7)/2.2 kΩ = 1955 µA

Saturated or active?

β·IB is larger than IC(sat), so the transistor saturates.

β·IB = 97.73 mA
IC(sat) = (12 − 0.2)/470 = 25.11 mA

Collector current

IC = IC(sat) = 25.11 mA

Answer

IC = 25.11 mA

The transistor is saturated.

3.Op-amp circuits

Answer: Rf = 2400 kΩ

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.

Gain of a non-inverting amplifier

V₋ = V₊ = Vin, and the current through R₁ also flows through Rf, so Vout = Vin·(1 + Rf/R₁).

Av = 1 + Rf/R1
Rf = (25 − 1)·100 = 2400 kΩ

Answer

Rf = 2400 kΩ
4.Op-amp circuits

Answer: Vout = −3.482 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.

Input currents

V₋ = 0, so each input resistor has its full input voltage across it.

I1 = V1/R1 = 0.8/1 = 0.8 mA
I2 = V2/R2 = −1.3/22 = −0.05909 mA
If = I1 + I2 = 0.7409 mA

Output voltage

Vout = −Rf·If = −4.7·0.7409 = −3.482 V

Answer

Vout = −3.482 V
5.RC & RL transients

Answer: t = 2.857 ms

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 = 68 mH / 33 Ω = 2.061 ms
i(∞) = Vs/R = 20/33 = 0.6061 A

Solve for the time

0.75 = 1 − e−t/τ → t = −τ·ln(1 − 0.75)
t = −2.061·ln(0.25) = 2.857 ms

Answer

t = 2.857 ms
6.RC & RL transients

Answer: R = 4.935 kΩ

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.

Required time constant

8.1 = 9·(1 − e−250/τ) → τ = 250/ln(9/(9 − 8.1))
τ = 250/2.303 = 108.6 ms

Resistance

kΩ times µF gives milliseconds.

R = τ/C = 108.6/22 = 4.935 kΩ

Answer

R = 4.935 kΩ
7.Series & parallel resistors

Answer: IR2 = 1.4 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.

R1​ = 4 ΩR3​ = 8 Ω+−V1​12 VR2​4 ΩAR4​20 ΩB

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 = 8 + 20 = 28 Ω
R2 ∥ 28 = 4·28/(4+28) = 3.5 Ω
Req = R1 + 3.5 = 4 + 3.5 = 7.5 Ω

Current from the source

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

IR1 = V1/Req = 12/7.5 = 1.6 A

Current through R₂

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

VA = V1 − IR1·R1 = 12 − 1.6·4 = 5.6 V
IR2 = VA/R2 = 5.6/4 = 1.4 A

Answer

IR2 = 1.4 A
8.Series & parallel resistors

Answer: Req = 18.52 Ω

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.

R1​ = 15 ΩR3​ = 25 ΩR5​ = 4 Ω+−V1​30 VR2​4 ΩAR4​5 ΩBR6​20 Ω

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 = 4 + 20 = 24 Ω
R4 ∥ 24 = 4.138 Ω
R3 + 4.138 = 29.14 Ω
R2 ∥ 29.14 = 3.517 Ω
Req = R1 + 3.517 = 15 + 3.517 = 18.52 Ω

Answer

Req = 18.52 Ω
9.DC-DC converters

Answer: Imax = 4.307 A

DC-DC converters: a switch S turns on for the fraction D of each period T = 1/f. In steady state the average inductor voltage is zero (volt-second balance), which gives the ideal conversion ratios in continuous conduction: buck Vo = D·Vin, boost Vo = Vin/(1 − D), inverting buck-boost |Vo| = Vin·D/(1 − D). An ideal converter keeps the power: Vin·Iin = Vo·Io. While S is on the inductor current rises by ΔIL = VL·D·T/L, with VL = Vin − Vo for the buck and Vin for the boost and buck-boost. The output ripple is ΔVo = ΔIL/(8fC) for the buck and Io·D/(fC) for the boost and buck-boost. The inductor current just touches zero (the CCM boundary) when the average inductor current equals ΔIL/2.

Duty cycle

D = 16.8/24 = 0.7

Average and ripple current

Io = 16.8/4 = 4.2 A
ΔIL = VL·D/(L·f) = 7.2·0.7/(47·10⁻⁶·500·10³) = 0.2145 A

Peak current

Imax = 4.2 + 0.2145/2 = 4.307 A

Answer

Imax = 4.307 A
10.DC-DC converters

Answer: ΔVo = 6.016 mV

DC-DC converters: a switch S turns on for the fraction D of each period T = 1/f. In steady state the average inductor voltage is zero (volt-second balance), which gives the ideal conversion ratios in continuous conduction: buck Vo = D·Vin, boost Vo = Vin/(1 − D), inverting buck-boost |Vo| = Vin·D/(1 − D). An ideal converter keeps the power: Vin·Iin = Vo·Io. While S is on the inductor current rises by ΔIL = VL·D·T/L, with VL = Vin − Vo for the buck and Vin for the boost and buck-boost. The output ripple is ΔVo = ΔIL/(8fC) for the buck and Io·D/(fC) for the boost and buck-boost. The inductor current just touches zero (the CCM boundary) when the average inductor current equals ΔIL/2.

Duty cycle

D = 7.2/12 = 0.6

Inductor ripple current

ΔIL = (12 − 7.2)·0.6/(68·10⁻⁶·200·10³) = 0.2118 A

Output ripple

ΔVo = 0.2118/(8·200·10³·22·10⁻⁶) = 6.016 mV

Answer

ΔVo = 6.016 mV
11.Wheatstone bridge & strain gauges

Answer: Rth = 61.61 Ω

Wheatstone bridge: two voltage dividers share one supply Vs. The left divider R1–R2 gives Va = Vs·R2/(R1 + R2) and the right divider R3–R4 gives Vb = Vs·R4/(R3 + R4); the output is Vab = Va − Vb. The bridge is balanced (Vab = 0, no current in the meter) when R1/R2 = R3/R4, that is R1·R4 = R2·R3. Seen from the output, the bridge is a Thévenin source with Rth = R1∥R2 + R3∥R4.

Supply shorted

R₁∥R₂ = 150·60/210 = 42.86 Ω
R₃∥R₄ = 20·300/320 = 18.75 Ω

Thévenin resistance

Rth = 61.61 Ω

Answer

Rth = 61.61 Ω
12.Wheatstone bridge & strain gauges

Answer: Vo = 4.1 mV

Strain gauges: a gauge changes its resistance with strain: ΔR/R = GF·ε, where the gauge factor GF is about 2 for metal foil. In a bridge with all arms equal to R, one active gauge (quarter bridge) gives Vo ≈ Vs·GF·ε/4. Two active gauges with opposite strains in adjacent arms (half bridge) give Vs·GF·ε/2, and four (full bridge) give Vs·GF·ε. Stress follows from Hooke’s law, σ = E·ε. Load cells state their sensitivity in mV/V: the output at full load per volt of excitation.

Relative resistance change

ΔR/R = 2.05·200·10⁻⁶ = 0.00041

Bridge output

Vo = Vs·GF·ε = 10·0.00041 = 4.1 mV

Answer

Vo = 4.1 mV
13.Digital logic: gates, K-maps & flip-flops

Answer: N = 5

Multiplexer: a 2ⁿ-to-1 multiplexer passes one of its data inputs to the output; the select lines, read as a binary number, pick which one. For a 4-to-1 MUX with selects S₁S₀ = AB, F = A′B′·I₀ + A′B·I₁ + AB′·I₂ + AB·I₃. Tying the data inputs to 0, 1, C or C′ makes the MUX produce any function of A, B and C, which is a common way to build logic with one chip.

Output expression

F = A′B′C′ + A′BC′ + AB′C + AB

Rows with F = 1

ABC = 000, 010, 101, 110, 111
N = 5

Answer

N = 5
14.Digital logic: gates, K-maps & flip-flops

Answer: N = 2

Karnaugh maps: the cells are ordered in Gray code (00, 01, 11, 10), so neighbouring cells, including the ones across the edges, differ in exactly one variable. Group the 1s in rectangles of 1, 2, 4, 8 or 16 cells, as large as possible and as few as possible, until every 1 is covered. Each group is one product term: the variables that stay constant inside it. A group of 2ᵏ cells loses k variables. Don't-cares (X) may be used to make groups bigger but never have to be covered. Grouping the 0s instead gives the minimal POS form.

Prime implicants

The largest groups that can be formed from 1s and Xs.

B′CD, A′C, A′BD′, AB′D
ABCD00011110000111100001X3121405171601201301501408X9111010

Essential prime implicants

A′C, A′BD′
N = 2

Answer

N = 2

ExamProblems · examproblems.com/courses/electronics-1