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​ = 1.2 kΩβ = 50IC​ = ?VCC​ = 12 VRB​ = 330 kΩ

An NPN transistor with β = 50 is biased by a base resistor RB = 330 kΩ from the supply VCC = 12 V. The collector resistor is RC = 1.2 kΩ and the emitter is grounded. Take VBE = 0.7 V and assume the transistor is in the active region. Find the collector current IC in mA.

VCC = 12 VRB = 330 kΩRC = 1.2 kΩβ = 50VBE = 0.7 V
IC = mA
2.Diodes & transistorsHard
RC​ = 680 Ωβ = 200IC​ = ?VCC​ = 9 V5 VRB​ = 220 kΩ

An NPN transistor with β = 200 switches a 680 Ω load resistor connected between VCC = 9 V and its collector. The emitter is grounded. The base is driven from a 5 V logic output through a base resistor RB = 220 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 = 9 VRC = 680 Ωβ = 200Vin = 5 VVBE = 0.7 VVCE(sat) = 0.2 VRB = 220 kΩ
IC = mA
3.Op-amp circuitsMedium
−+Vout​Rf​ = 10 kΩR1​ = 4.7 kΩVin​ = 5 VRa​ = 22 kΩRb​ = 100 kΩ

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

Vin = 5 VRa = 22 kΩRb = 100 kΩR1 = 4.7 kΩRf = 10 kΩ
Vout = V
4.Op-amp circuitsHard
−+Vout​Rf​ = 2 kΩV1​ = 2 VR1​ = 2 kΩV2​ = 1.7 VR2​ = 47 kΩ

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

V1 = 2 VV2 = 1.7 VR1 = 2 kΩR2 = 47 kΩRf = 2 kΩ
Vout = V
5.RC & RL transientsMedium
+−Vs​6 Vt = 0R1​ = 1 kΩR2​ = 6.8 kΩC33 µF+−vC​

The source Vₛ charges the capacitor through R₁, and R₂ is connected in parallel with C. The capacitor is uncharged when the switch closes at t = 0. Find the capacitor voltage vC at t = 75 ms.

Vs = 6 VR1 = 1 kΩR2 = 6.8 kΩC = 33 µFt = 75 ms
vC = V
6.RC & RL transientsHard
+−Vs​10 Vt = 0R = 6.8 kΩC100 µF+−vC​vC​(0) = 24 V

Just before the switch closes at t = 0, the capacitor holds 24 V with the polarity shown. How long does it take for vC to reach 18.4 V? Find t.

Vs = 10 VR = 6.8 kΩC = 100 µFvC(0) = 24 V
t = ms
7.Series & parallel resistorsMedium
R1​ = 10 ΩR3​ = 10 Ω+−V1​18 VR2​6 ΩIR2​AR4​6 ΩB

Find the current IR2 through R2.

V1 = 18 VR1 = 10 ΩR2 = 6 ΩR3 = 10 ΩR4 = 6 Ω
IR2 = A
8.Series & parallel resistorsHard
R1​ = 25 ΩR3​ = 8 ΩR5​ = 15 Ω+−V1​30 VR2​5 ΩAR4​30 ΩBR6​20 Ω

Find the equivalent resistance Req seen by the source V1.

V1 = 30 VR1 = 25 ΩR2 = 5 ΩR3 = 8 ΩR4 = 30 ΩR5 = 15 ΩR6 = 20 Ω
Req = Ω
9.DC-DC convertersMedium
+−12 VLSCR = 5 Ω+−24 V

An ideal boost converter turns 12 V into 24 V for a 5 Ω load. Find the average inductor current IL.

Vin​ = 12 VVo​ = 24 VR = 5 Ω
IL = A
10.DC-DC convertersHard
+−24 VLSC = 470 µFR = 20 Ω+−60 V

An ideal boost converter turns 24 V into 60 V for a 20 Ω load at 40 kHz. The output capacitor is 470 µF. Find the peak-to-peak output voltage ripple ΔVo in mV.

Vin​ = 24 VVo​ = 60 Vf = 40 kHzC = 470 µFR = 20 Ω
ΔVo = mV
11.Wheatstone bridge & strain gaugesMedium
+−3 V1000 Ω1000 Ω1000 Ω1000 Ωab+−

A 1000 Ω strain gauge is one arm (R₂) of a bridge with four equal 1000 Ω arms and an excitation of 3 V. Find the power Pg dissipated in the gauge, in mW. Self-heating limits the excitation.

Vs = 3 VR = 1000 Ω
Pg = mW
12.Wheatstone bridge & strain gaugesHard
+−2.5 V1000 Ω1000 Ω + ΔR1000 Ω1000 Ωab+−Vo​

A quarter bridge (one active gauge, GF = 2.12) is excited with 2.5 V. The largest strain to be measured is 1200 µε, and it must give 5 V at the input of an analogue-to-digital converter. Find the amplifier gain G.

Vs = 2.5 VGF = 2.12εmax = 1200 µεVFS = 5 V
G =
13.Digital logic: gates, K-maps & flip-flopsMedium
ABCD0001111000011110111111

In this Karnaugh map exactly one 1 has no neighbouring 1, so it stays a group of one cell (a full minterm of four literals) in the minimal SOP form. Neighbours across the map edges count. Click that cell.

F = Σm(0, 1, 3, 4, 11, 13)
  1. 1AB = 00, CD = 00
  2. 2AB = 00, CD = 01
  3. 3AB = 00, CD = 11
  4. 4AB = 00, CD = 10
  5. 5AB = 01, CD = 00
  6. 6AB = 01, CD = 01
  7. 7AB = 01, CD = 11
  8. 8AB = 01, CD = 10
  9. 9AB = 11, CD = 00
  10. 10AB = 11, CD = 01
  11. 11AB = 11, CD = 11
  12. 12AB = 11, CD = 10
  13. 13AB = 10, CD = 00
  14. 14AB = 10, CD = 01
  15. 15AB = 10, CD = 11
  16. 16AB = 10, CD = 10
14.Digital logic: gates, K-maps & flip-flopsHard
TQ0​Q0​TQ1​Q1​TQ2​Q2​CLK

A 3-bit ripple (asynchronous) counter is built from flip-flops with a propagation delay of 25 ns each. All outputs must have settled before the next clock edge. Find the maximum clock frequency fmax.

n = 3tpd = 25 ns
fmax = MHz

3Solutions

1.Diodes & transistors

Answer: IC = 1.712 mA

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.

Base current

IB = (VCC − VBE)/RB = (12 − 0.7)/330 kΩ = 34.24 µA

Collector current

IC = β·IB = 50·34.24 µA = 1.712 mA

Answer

IC = 1.712 mA

Check: VCE = 9.945 V is well above 0.2 V, so the transistor is indeed active.

2.Diodes & transistors

Answer: IC = 3.909 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)/220 kΩ = 19.55 µA

Saturated or active?

β·IB is smaller than IC(sat), so the transistor stays active.

β·IB = 3.909 mA
IC(sat) = (9 − 0.2)/680 = 12.94 mA

Collector current

IC = β·IB = 3.909 mA

Answer

IC = 3.909 mA

The transistor is active, so the load is not fully switched on.

3.Op-amp circuits

Answer: Vout = 12.82 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.

Voltage at the + input

V₊ = Vin·Rb/(Ra + Rb) = 5·100/(22 + 100) = 4.098 V

Non-inverting gain

V₋ = V₊, and the current through R₁ also flows through Rf.

Vout = V₊·(1 + Rf/R1) = 4.098·(1 + 10/4.7) = 12.82 V

Answer

Vout = 12.82 V
4.Op-amp circuits

Answer: Vout = −2.072 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 = 2/2 = 1 mA
I2 = V2/R2 = 1.7/47 = 0.03617 mA
If = I1 + I2 = 1.036 mA

Output voltage

Vout = −Rf·If = −2·1.036 = −2.072 V

Answer

Vout = −2.072 V
5.RC & RL transients

Answer: vC = 4.845 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.

Thévenin equivalent seen by the capacitor

Short the source to find Rth; open the capacitor to find the voltage it will settle at.

Rth = R1 ∥ R2 = 1·6.8/(1 + 6.8) = 0.8718 kΩ
vC(∞) = 6·6.8/(1 + 6.8) = 5.231 V

Time constant

τ = Rth·C = 0.8718·33 = 28.77 ms

Charging curve

vC(t) = 5.231·(1 − e−75/28.77) = 4.845 V

Answer

vC = 4.845 V
6.RC & RL transients

Answer: t = 347.4 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) = 24 V, vC(∞) = Vs = 10 V
τ = R·C = 6.8 kΩ · 100 µF = 680 ms
vC(t) = 10 + (24 − 10)·e−t/τ

Solve for the time

18.4 = 10 + (14)·e−t/τ → e−t/τ = (18.4 − 10)/(24 − 10) = 0.6
t = τ·ln((24 − 10)/(18.4 − 10)) = 680·ln(1.667) = 347.4 ms

Answer

t = 347.4 ms
7.Series & parallel resistors

Answer: IR2 = 0.9114 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​ = 10 ΩR3​ = 10 Ω+−V1​18 VR2​6 ΩAR4​6 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 = 10 + 6 = 16 Ω
R2 ∥ 16 = 6·16/(6+16) = 4.364 Ω
Req = R1 + 4.364 = 10 + 4.364 = 14.36 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 = 18/14.36 = 1.253 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 = 18 − 1.253·10 = 5.468 V
IR2 = VA/R2 = 5.468/6 = 0.9114 A

Answer

IR2 = 0.9114 A
8.Series & parallel resistors

Answer: Req = 29.14 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​ = 25 ΩR3​ = 8 ΩR5​ = 15 Ω+−V1​30 VR2​5 ΩAR4​30 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 = 15 + 20 = 35 Ω
R4 ∥ 35 = 16.15 Ω
R3 + 16.15 = 24.15 Ω
R2 ∥ 24.15 = 4.142 Ω
Req = R1 + 4.142 = 25 + 4.142 = 29.14 Ω

Answer

Req = 29.14 Ω
9.DC-DC converters

Answer: IL = 9.6 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

Load current

Io = 24/5 = 4.8 A

Inductor current

IL = Io/(1 − D) = 4.8/0.5 = 9.6 A

Answer

IL = 9.6 A
10.DC-DC converters

Answer: ΔVo = 95.74 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 = 1 − 24/60 = 0.6

Load current

Io = 60/20 = 3 A

Output ripple

ΔVo = 3·0.6/(40·10³·470·10⁻⁶) = 95.74 mV

Answer

ΔVo = 95.74 mV
11.Wheatstone bridge & strain gauges

Answer: Pg = 2.25 mW

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.

Voltage across the gauge

V = 3/2 = 1.5 V

Power

Pg = 1.5²/1000 = 2.25 mW

Answer

Pg = 2.25 mW
12.Wheatstone bridge & strain gauges

Answer: G = 3145

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 = 1.59 mV

Gain

G = 5/0.00159 = 3145

Answer

G = 3145
13.Digital logic: gates, K-maps & flip-flops

Answer: AB = 11, CD = 01

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.

Neighbours of each 1

A 1 with a neighbouring 1 can join a group of two or more.

m13: m12, m15, m9, m5 → 0
ABCD0001111000011110111111

The isolated 1

m13 = ABC′D → AB = 11, CD = 01

Answer

AB = 11, CD = 01
14.Digital logic: gates, K-maps & flip-flops

Answer: fmax = 13.33 MHz

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.

Worst-case settling time

T = 3·25 ns = 75 ns

Maximum frequency

fmax = 1/75 ns = 13.33 MHz

Answer

fmax = 13.33 MHz

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