Electronics 1: cram pack

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

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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
RC​ = 4.7 kΩβ = 200RE​ = 1.5 kΩVCC​ = 12 VR1​ = 22 kΩR2​ = 6.8 kΩ

An NPN transistor with β = 200 has voltage-divider bias from VCC = 12 V: R₁ = 22 kΩ from VCC to the base and R₂ = 6.8 kΩ from the base to ground. The collector resistor is RC = 4.7 kΩ and the emitter resistor is RE = 1.5 kΩ. Take VBE = 0.7 V and use the Thévenin equivalent of the divider (do not neglect the base current). Find the collector–emitter voltage VCE.

VCC = 12 VR1 = 22 kΩR2 = 6.8 kΩRC = 4.7 kΩRE = 1.5 kΩβ = 200
VCE = V
2.Diodes & transistorsHard
+−≥ 24 VR = ?6.2 V≤ 20 mA

A 6.2 V Zener regulator must supply up to 20 mA to a load. The input can drop to 24 V, and the Zener needs at least 1 mA to regulate. Find the largest series resistance Rmax that keeps it regulating.

Vin,min = 24 VVZ = 6.2 VIL,max = 20 mAIZ,min = 1 mA
Rmax = Ω
3.Op-amp circuitsMedium
−+Vout​Rf​ = ?R1​ = 47 kΩVin​

Choose the feedback resistor Rf that gives this non-inverting amplifier a voltage gain of 5.

R1 = 47 kΩAv = 5
Rf = kΩ
4.Op-amp circuitsHard
−+Vout​Rf​ = 100 kΩV1​ = 0.1 VR1​ = 4.7 kΩV2​ = 1.2 VR2​ = 22 kΩIf​

The summing amplifier uses an ideal op-amp with ±15 V supplies. Find the current If through the feedback resistor, flowing towards the output.

V1 = 0.1 VV2 = 1.2 VR1 = 4.7 kΩR2 = 22 kΩRf = 100 kΩ
If = mA
5.RC & RL transientsMedium
+−Vs​15 Vt = 0R = 100 ΩL68 mHi(t)

The inductor carries no current before the switch closes at t = 0. Find the voltage vL across the inductor at t = 1 ms.

Vs = 15 VR = 100 ΩL = 68 mHt = 1 ms
vL = V
6.RC & RL transientsHard
+−Vs​6 Vt = 0R = 1 kΩC68 µF+−vC​vC​(0) = 20 V

Just before the switch closes at t = 0, the capacitor holds 20 V with the polarity shown. How long does it take for vC to reach 8.8 V? Find t.

Vs = 6 VR = 1 kΩC = 68 µFvC(0) = 20 V
t = ms
7.Series & parallel resistorsMedium
R1​ = 8 ΩR3​ = 3 Ω+−V1​30 VR2​2 ΩAR4​15 ΩB

Find the equivalent resistance Req seen by the source V1.

V1 = 30 VR1 = 8 ΩR2 = 2 ΩR3 = 3 ΩR4 = 15 Ω
Req = Ω
8.Series & parallel resistorsHard
R1​ = 6 ΩIR1​R3​ = 12 ΩR5​ = 30 Ω+−V1​5 VR2​15 ΩAR4​15 ΩBR6​2 Ω

Find the current IR1 delivered by the source, which flows through R1.

V1 = 5 VR1 = 6 ΩR2 = 15 ΩR3 = 12 ΩR4 = 15 ΩR5 = 30 ΩR6 = 2 Ω
IR1 = A
9.DC-DC convertersMedium
tiL​Imax​Imin​ΔI = ?DTT2T

An ideal boost converter turns 12 V into 24 V at 20 kHz with L = 220 µH. Find the peak-to-peak inductor ripple current ΔIL.

Vin​ = 12 VVo​ = 24 Vf = 20 kHzL = 220 µH
ΔIL = A
10.DC-DC convertersHard
+−9 VSL = 47 µHC = ?R+−2.7 V

A buck converter turns 9 V into 2.7 V at 250 kHz with L = 47 µH. Find the output capacitance C that limits the peak-to-peak output ripple to 10 mV.

Vin​ = 9 VVo​ = 2.7 Vf = 250 kHzL = 47 µHΔVo = 10 mV
C = µF
11.Wheatstone bridge & strain gaugesMedium
+−15 V350 Ω350 Ω + ΔR350 Ω350 Ωab+−182.9 mV

A bridge with four 350 Ω arms is supplied with 15 V. When the sensor R₂ changes, the output reads Vab = 182.9 mV. Find the exact change ΔR of R₂.

Vs = 15 VR = 350 ΩVab = 182.9 mV
ΔR = Ω
12.Wheatstone bridge & strain gaugesHard
+−5 V1000 Ω1000 Ω + ΔR1000 Ω1000 Ωab+−Vo​

A quarter bridge (one active gauge, GF = 2.1) is excited with 5 V. The largest strain to be measured is 200 µε, and it must give 2.5 V at the input of an analogue-to-digital converter. Find the amplifier gain G.

Vs = 5 VGF = 2.1εmax = 200 µεVFS = 2.5 V
G =
13.Digital logic: gates, K-maps & flip-flopsMedium
MUXC′I0​C′I1​C′I2​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 = C′I₃ = 1
N =
14.Digital logic: gates, K-maps & flip-flopsHard
TQ0​Q0​TQ1​Q1​TQ2​Q2​TQ3​Q3​CLKUP

A 4-bit binary up counter starts at 4 (decimal, Q = 0100). Which count Q (in decimal) does it show after 48 clock pulses?

Q0 = 448n = 4
Q =

3Solutions

1.Diodes & transistors

Answer: VCE = 3.364 V

BJT bias point: in the active region VBE = 0.7 V, IC = β·IB and IE = (β + 1)·IB. Find IB from the base loop with KVL, then IC, then VCE from the collector–emitter loop. A voltage divider at the base is replaced by its Thévenin equivalent VTH = VCC·R₂/(R₁ + R₂), RTH = R₁∥R₂; an emitter resistor appears (β + 1) times larger in the base loop.

Thévenin equivalent of the divider

VTH = 12·6.8/(22 + 6.8) = 2.833 V
RTH = 22·6.8/(22 + 6.8) = 5.194 kΩ

Base current

KVL around the base loop; the emitter current is (β + 1)·IB.

IB = (2.833 − 0.7)/(5.194 + 201·1.5) = 6.956 µA

Collector current

IC = 200·6.956 µA = 1.391 mA
IE = 201·6.956 µA = 1.398 mA

Collector–emitter voltage

VCE = 12 − 1.391·4.7 − 1.398·1.5 = 3.364 V

Answer

VCE = 3.364 V
2.Diodes & transistors

Answer: Rmax = 847.6 Ω

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.

Worst-case current

IR = 20 + 1 = 21 mA

Largest resistance

Rmax = 17.8/0.021 = 847.6 Ω

Answer

Rmax = 847.6 Ω
3.Op-amp circuits

Answer: Rf = 188 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 = (5 − 1)·47 = 188 kΩ

Answer

Rf = 188 kΩ
4.Op-amp circuits

Answer: If = 0.07582 mA

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 = 0.1/4.7 = 0.02128 mA
I2 = V2/R2 = 1.2/22 = 0.05455 mA
If = I1 + I2 = 0.07582 mA

Answer

If = 0.07582 mA
5.RC & RL transients

Answer: vL = 3.447 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 = 68 mH / 100 Ω = 0.68 ms
i(∞) = Vs/R = 15/100 = 0.15 A

Inductor voltage

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

vL(t) = Vs·e−t/τ = 15·e−1/0.68 = 3.447 V

Answer

vL = 3.447 V
6.RC & RL transients

Answer: t = 109.4 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.

Initial value, final value, time constant

The capacitor voltage cannot jump, so it starts at its stored value and heads for the source voltage.

vC(0) = 20 V, vC(∞) = Vs = 6 V
τ = R·C = 1 kΩ · 68 µF = 68 ms
vC(t) = 6 + (20 − 6)·e−t/τ

Solve for the time

8.8 = 6 + (14)·e−t/τ → e−t/τ = (8.8 − 6)/(20 − 6) = 0.2
t = τ·ln((20 − 6)/(8.8 − 6)) = 68·ln(5) = 109.4 ms

Answer

t = 109.4 ms
7.Series & parallel resistors

Answer: Req = 9.8 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​ = 8 ΩR3​ = 3 Ω+−V1​30 VR2​2 ΩAR4​15 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 = 3 + 15 = 18 Ω
R2 ∥ 18 = 2·18/(2+18) = 1.8 Ω
Req = R1 + 1.8 = 8 + 1.8 = 9.8 Ω

Answer

Req = 9.8 Ω
8.Series & parallel resistors

Answer: IR1 = 0.3344 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​ = 6 ΩR3​ = 12 ΩR5​ = 30 Ω+−V1​5 VR2​15 ΩAR4​15 ΩBR6​2 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 = 30 + 2 = 32 Ω
R4 ∥ 32 = 10.21 Ω
R3 + 10.21 = 22.21 Ω
R2 ∥ 22.21 = 8.954 Ω
Req = R1 + 8.954 = 6 + 8.954 = 14.95 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 = 5/14.95 = 0.3344 A

Answer

IR1 = 0.3344 A
9.DC-DC converters

Answer: ΔIL = 1.364 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 = 1 − 12/24 = 0.5

Inductor voltage during the on-time

While S is on, the inductor sits directly across Vin.

VL = 12 V

Ripple current

ΔIL = VL·D/(L·f) = 12·0.5/(220·10⁻⁶·20·10³) = 1.364 A

Answer

ΔIL = 1.364 A
10.DC-DC converters

Answer: C = 8.043 µF

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 = 2.7/9 = 0.3

Inductor ripple current

ΔIL = (9 − 2.7)·0.3/(47·10⁻⁶·250·10³) = 0.1609 A

Capacitance

C = 0.1609/(8·250·10³·10·10⁻³) = 8.043 µF

Answer

C = 8.043 µF
11.Wheatstone bridge & strain gauges

Answer: ΔR = 17.5 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.

Node voltage

Va = 7.5 + 0.1829 = 7.683 V

Solve the divider

R₂ = 350·7.683/(15 − 7.683) = 367.5 Ω
ΔR = 367.5 − 350 = 17.5 Ω

Answer

ΔR = 17.5 Ω
12.Wheatstone bridge & strain gauges

Answer: G = 4762

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.

Bridge output at full scale

Vo = 0.525 mV

Gain

G = 2.5/0.000525 = 4762

Answer

G = 4762
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, 100, 110, 111
N = 5

Answer

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

Answer: Q = 4

Flip-flops and counters: a flip-flop changes only at the active clock edge. D copies its input (Q⁺ = D); T toggles when T = 1; JK holds for 00, resets for 01, sets for 10 and toggles for 11. An n-bit binary counter has 2ⁿ states and counts modulo 2ⁿ; a mod-N counter goes 0, 1, …, N − 1 and back to 0, and needs the smallest n with 2ⁿ ≥ N flip-flops. Each stage of a ripple counter halves the frequency, so the last output of a mod-N counter runs at fclk/N. A Johnson counter of n flip-flops has 2n states, a ring counter n.

Full cycles

Every 16 pulses bring the counter back to the same state.

48 = 3·16 + 0

Count after the remaining pulses

Q = (4 + 0) mod 16 = 4
Q = 0100₂

Answer

Q = 4

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