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​ = 1.5 kΩβ = 80VCC​ = 10 VRB​ = 820 kΩ

An NPN transistor with β = 80 is biased by a base resistor RB = 820 kΩ from the supply VCC = 10 V. The collector resistor is RC = 1.5 kΩ and the emitter is grounded. Take VBE = 0.7 V and assume the transistor is in the active region. Find the collector–emitter voltage VCE.

VCC = 10 VRB = 820 kΩRC = 1.5 kΩβ = 80VBE = 0.7 V
VCE = V
2.Diodes & transistorsHard
V (V)I (mA)0.736.383Q = ?

A diode is modelled as 0.7 V in series with 10 Ω (it conducts above 0.7 V). It is in series with a 470 Ω resistor across a 3 V supply. Find the operating current ID where the diode line meets the load line.

Vs = 3 VR = 470 ΩV0 = 0.7 Vrd = 10 Ω
ID = mA
3.Op-amp circuitsMedium
−+Vout​Rf​ = 47 kΩR1​ = 22 kΩVin​ = 0.5 VRa​ = 10 kΩRb​ = 22 kΩ

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

Vin = 0.5 VRa = 10 kΩRb = 22 kΩR1 = 22 kΩRf = 47 kΩ
Vout = V
4.Op-amp circuitsHard
−+Vout​Rf​ = 47 kΩV1​ = −0.5 VR1​ = 22 kΩV2​ = 1.4 VR2​ = 47 kΩ

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

V1 = −0.5 VV2 = 1.4 VR1 = 22 kΩR2 = 47 kΩRf = 47 kΩ
Vout = V
5.RC & RL transientsMedium
R = 100 Ωt = 0L220 mHi(t)

The inductor carries a steady current of 2 A. At t = 0 the switch closes the loop through R and the source is removed, so the inductor current decays through R. How long does it take for the current to fall to 1 A? Find t.

i(0) = 2 AR = 100 ΩL = 220 mH
t = ms
6.RC & RL transientsHard
+−Vs​10 Vt = 0R = 6.8 kΩC47 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 15 V? Find t.

Vs = 10 VR = 6.8 kΩC = 47 µFvC(0) = 20 V
t = ms
7.Series & parallel resistorsMedium
R1​ = 8 ΩIR1​R3​ = 12 Ω+−V1​10 VR2​15 ΩAR4​20 ΩB

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

V1 = 10 VR1 = 8 ΩR2 = 15 ΩR3 = 12 ΩR4 = 20 Ω
IR1 = A
8.Series & parallel resistorsHard
R1​ = 10 ΩIR1​R3​ = 8 ΩR5​ = 3 Ω+−V1​9 VR2​12 ΩAR4​6 ΩBR6​6 Ω

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

V1 = 9 VR1 = 10 ΩR2 = 12 ΩR3 = 8 ΩR4 = 6 ΩR5 = 3 ΩR6 = 6 Ω
IR1 = A
9.DC-DC convertersMedium
tiL​Imax​Imin​ΔI = ?DTT2T

An ideal boost converter turns 24 V into 96 V at 25 kHz with L = 330 µH. Find the peak-to-peak inductor ripple current ΔIL.

Vin​ = 24 VVo​ = 96 Vf = 25 kHzL = 330 µH
ΔIL = A
10.DC-DC convertersHard
tiL​Imax​IL​DTT2T

An ideal inverting buck-boost converter turns 24 V into −36 V for a 50 Ω load at 100 kHz. Find the smallest inductance Lcrit for continuous conduction.

Vin​ = 24 VVo​ = −36 Vf = 100 kHzR = 50 Ω
Lcrit = µH
11.Wheatstone bridge & strain gaugesMedium
+−2 VR1​ = 10 ΩR2​ = 300 ΩR3​ = 250 ΩR4​ = 250 ΩabGRg​ = 20 Ω

A galvanometer with a resistance of 20 Ω is connected between a and b of the bridge shown (Vs = 2 V). Find the galvanometer current Ig from a to b, in µA.

Vs = 2 VR1 = 10 ΩR2 = 300 ΩR3 = 250 ΩR4 = 250 ΩRg = 20 Ω
Ig = µA
12.Wheatstone bridge & strain gaugesHard
+−2.5 V350 Ω − ΔR350 Ω + ΔR350 Ω350 Ωab+−Vo​ = ?

A bridge with 350 Ω arms is excited with 2.5 V and has two active gauges in adjacent arms, one in tension and one in compression (half bridge). The gauge factor is 2.05 and the strain is 400 µε. Find the bridge output Vo in mV.

Vs = 2.5 VGF = 2.05ε = 400 µε
Vo = mV
13.Digital logic: gates, K-maps & flip-flopsMedium
MUX0I0​CI1​C′I2​C′I3​ABS1​S0​F

A 4-to-1 multiplexer has its select inputs S₁ = A and S₀ = B, and its data inputs tied to I₀ = 0, I₁ = C, I₂ = C′, I₃ = C′. For how many of the 8 combinations of A, B and C is the output F = 1? Find N.

I₀ = 0I₁ = CI₂ = C′I₃ = C′
N =
14.Digital logic: gates, K-maps & flip-flopsHard
ABCD000111100001111010X1131214051716012013X1511418X9011010

Find the minimal SOP form of F(A, B, C, D) = Σm(0, 2, 3, 4, 6, 7, 8, 14) + d(1, 9, 15), where d marks the don't-care conditions. How many literals L does it contain?

F(A, B, C, D) = Σm(0, 2, 3, 4, 6, 7, 8, 14) + d(1, 9, 15)
L =

3Solutions

1.Diodes & transistors

Answer: VCE = 8.639 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.

Base current

IB = (VCC − VBE)/RB = (10 − 0.7)/820 kΩ = 11.34 µA

Collector current

IC = β·IB = 80·11.34 µA = 0.9073 mA

Collector–emitter voltage

VCE = 10 − 0.9073 mA·1.5 kΩ = 8.639 V

Answer

VCE = 8.639 V
2.Diodes & transistors

Answer: ID = 4.792 mA

LED and diode circuits: a forward-biased LED drops roughly its forward voltage VF (about 2 V for red, 3 V for blue or white), whatever the current. A series resistor sets the current: R = (Vs − n·VF)/I for n LEDs in series. With a more exact diode model V = V₀ + I·rd, the operating point is where the diode line meets the load line I = (Vs − V)/R, so I = (Vs − V₀)/(R + rd).

Combine the two equations

3 = 0.7 + I·(470 + 10)

Operating current

ID = 2.3/480 = 4.792 mA
VD = 0.7 + 0.004792·10 = 0.7479 V

Answer

ID = 4.792 mA
3.Op-amp circuits

Answer: Vout = 1.078 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) = 0.5·22/(10 + 22) = 0.3438 V

Non-inverting gain

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

Vout = V₊·(1 + Rf/R1) = 0.3438·(1 + 47/22) = 1.078 V

Answer

Vout = 1.078 V
4.Op-amp circuits

Answer: Vout = −0.3318 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 = −0.5/22 = −0.02273 mA
I2 = V2/R2 = 1.4/47 = 0.02979 mA
If = I1 + I2 = 0.00706 mA

Output voltage

Vout = −Rf·If = −47·0.00706 = −0.3318 V

Answer

Vout = −0.3318 V
5.RC & RL transients

Answer: t = 1.525 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

τ = L/R = 220 mH / 100 Ω = 2.2 ms

Solve for the time

1 = 2·e−t/τ → t = τ·ln(2/1)
t = 2.2·ln(2) = 1.525 ms

Answer

t = 1.525 ms
6.RC & RL transients

Answer: t = 221.5 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 = 10 V
τ = R·C = 6.8 kΩ · 47 µF = 319.6 ms
vC(t) = 10 + (20 − 10)·e−t/τ

Solve for the time

15 = 10 + (10)·e−t/τ → e−t/τ = (15 − 10)/(20 − 10) = 0.5
t = τ·ln((20 − 10)/(15 − 10)) = 319.6·ln(2) = 221.5 ms

Answer

t = 221.5 ms
7.Series & parallel resistors

Answer: IR1 = 0.5491 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​ = 8 ΩR3​ = 12 Ω+−V1​10 VR2​15 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 = 12 + 20 = 32 Ω
R2 ∥ 32 = 15·32/(15+32) = 10.21 Ω
Req = R1 + 10.21 = 8 + 10.21 = 18.21 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 = 10/18.21 = 0.5491 A

Answer

IR1 = 0.5491 A
8.Series & parallel resistors

Answer: IR1 = 0.5661 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​ = 8 ΩR5​ = 3 Ω+−V1​9 VR2​12 ΩAR4​6 ΩBR6​6 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 = 3 + 6 = 9 Ω
R4 ∥ 9 = 3.6 Ω
R3 + 3.6 = 11.6 Ω
R2 ∥ 11.6 = 5.898 Ω
Req = R1 + 5.898 = 10 + 5.898 = 15.9 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 = 9/15.9 = 0.5661 A

Answer

IR1 = 0.5661 A
9.DC-DC converters

Answer: ΔIL = 2.182 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 − 24/96 = 0.75

Inductor voltage during the on-time

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

VL = 24 V

Ripple current

ΔIL = VL·D/(L·f) = 24·0.75/(330·10⁻⁶·25·10³) = 2.182 A

Answer

ΔIL = 2.182 A
10.DC-DC converters

Answer: Lcrit = 40 µH

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 = 36/(24 + 36) = 0.6

Boundary condition

Set the average inductor current equal to half the ripple current and solve for L.

Lcrit = (1 − D)²·R/(2f)

Critical inductance

Lcrit = (1 − 0.6)²·50/(2100·10³) = 40 µH

Answer

Lcrit = 40 µH
11.Wheatstone bridge & strain gauges

Answer: Ig = 6048 µA

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.

Thévenin voltage

Vth = 2·(300/310 − 250/500) = 0.9355 V

Thévenin resistance

Rth = R₁∥R₂ + R₃∥R₄ = 134.7 Ω

Galvanometer current

Ig = 0.9355/(134.7 + 20) = 6048 µA

Answer

Ig = 6048 µA
12.Wheatstone bridge & strain gauges

Answer: Vo = 1.025 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 = 2.05·400·10⁻⁶ = 0.00082

Bridge output

Vo = Vs·GF·ε/2 = 2.5·0.00082/2 = 1.025 mV

Answer

Vo = 1.025 mV
13.Digital logic: gates, K-maps & flip-flops

Answer: N = 3

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′BC + AB′C′ + ABC′

Rows with F = 1

ABC = 011, 100, 110
N = 3

Answer

N = 3
14.Digital logic: gates, K-maps & flip-flops

Answer: L = 8

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′C′, BC, A′D′, A′C, A′B′
ABCD000111100001111010X1131214051716012013X1511418X9011010

Minimal cover

F = B′C′ + BC + A′D′ + A′C
L = 8

Answer

L = 8

Another grouping of the same size exists; it has the same number of terms and literals.

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