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
+−9 VR = ?2 × 2.2 V20 mA

2 green LEDs (forward voltage 2.2 V each) are connected in series with a resistor to a 9 V supply. Find the resistance R that sets the current to 20 mA.

Vs = 9 VVF = 2.2 Vn = 2I = 20 mA
R = Ω
2.Diodes & transistorsHard
RC​ = 220 Ωβ = 150IC​ = ?VCC​ = 9 V5 VRB​ = 10 kΩ

An NPN transistor with β = 150 switches a 220 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 = 10 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 = 220 Ωβ = 150Vin = 5 VVBE = 0.7 VVCE(sat) = 0.2 VRB = 10 kΩ
IC = mA
3.Op-amp circuitsMedium
−+Vout​R2​ = 47 kΩV1​ = −0.9 VR1​ = 22 kΩV2​ = 1.4 VR3​ = 22 kΩR4​ = 47 kΩ

The difference amplifier uses an ideal op-amp with ±15 V supplies, with R3 = R1 and R4 = R2. Find the voltage V− at the inverting input.

V1 = −0.9 VV2 = 1.4 VR1 = R3 = 22 kΩR2 = R4 = 47 kΩ
V− = V
4.Op-amp circuitsHard
−+Vout​Rf​ = 4.7 kΩV1​ = −1.7 VR1​ = 1 kΩV2​ = 1.5 VR2​ = 10 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 = −1.7 VV2 = 1.5 VR1 = 1 kΩR2 = 10 kΩRf = 4.7 kΩ
If = mA
5.RC & RL transientsMedium
+−Vs​5 Vt = 0R = 10 ΩL47 mHi(t)

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

Vs = 5 VR = 10 ΩL = 47 mHt = 5 ms
vL = V
6.RC & RL transientsHard
+−Vs​15 Vt = 0R = 1 kΩC?+−vC​

A timer starts charging an uncharged capacitor through a resistor from a 15 V supply at t = 0. It must trigger when the capacitor voltage reaches 9 V, exactly 10 ms after the start. With R = 1 kΩ, find the capacitance C needed.

Vs = 15 VVth = 9 VT = 10 msR = 1 kΩ
C = µF
7.Series & parallel resistorsMedium
R1​ = 15 ΩR3​ = 4 Ω+−V1​24 VR2​4 ΩAR4​3 ΩB

Find the equivalent resistance Req seen by the source V1.

V1 = 24 VR1 = 15 ΩR2 = 4 ΩR3 = 4 ΩR4 = 3 Ω
Req = Ω
8.Series & parallel resistorsHard
R1​ = 4 ΩR3​ = 4 ΩR5​ = 2 Ω+−V1​6 VR2​20 ΩIR2​AR4​3 ΩBR6​10 Ω

Find the current IR2 through R2.

V1 = 6 VR1 = 4 ΩR2 = 20 ΩR3 = 4 ΩR4 = 3 ΩR5 = 2 ΩR6 = 10 Ω
IR2 = A
9.DC-DC convertersMedium
tiL​Imax​Imin​ΔI = ?DTT2T

An ideal inverting buck-boost converter turns 12 V into −12 V at 500 kHz with L = 47 µH. Find the peak-to-peak inductor ripple current ΔIL.

Vin​ = 12 VVo​ = −12 Vf = 500 kHzL = 47 µH
ΔIL = A
10.DC-DC convertersHard
tiL​Imax​IL​DTT2T

An ideal inverting buck-boost converter turns 9 V into −13.5 V for a 2 Ω load at 250 kHz. Find the smallest inductance Lcrit for continuous conduction.

Vin​ = 9 VVo​ = −13.5 Vf = 250 kHzR = 2 Ω
Lcrit = µH
11.Wheatstone bridge & strain gaugesMedium
+−9 VR1​ = 200 ΩR2​ = 250 ΩR3​ = 300 ΩR4​ = 40 ΩabGRg​ = 100 Ω

A galvanometer with a resistance of 100 Ω is connected between a and b of the bridge shown (Vs = 9 V). Find the galvanometer current Ig from a to b, in µA.

Vs = 9 VR1 = 200 ΩR2 = 250 ΩR3 = 300 ΩR4 = 40 ΩRg = 100 Ω
Ig = µA
12.Wheatstone bridge & strain gaugesHard
+−3 V350 Ω350 Ω + ΔR350 Ω350 Ωab+−1.125 mV

A strain gauge (GF = 2) on a member with E = 70 GPa forms a quarter bridge excited with 3 V. The output reads 1.125 mV. Find the axial stress σ in MPa.

Vs = 3 VGF = 2Vo = 1.125 mVE = 70 GPa
σ = MPa
13.Digital logic: gates, K-maps & flip-flopsMedium
ABCD00011110000111101111

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(4, 9, 11, 15)
  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
ABCD00011110000111100011130204051706X12113X150140809X11X10

Find the minimal SOP form of F(A, B, C, D) = Σm(1, 3, 7, 13) + d(10, 11, 12, 15), where d marks the don't-care conditions. How many product terms N does it have?

F(A, B, C, D) = Σm(1, 3, 7, 13) + d(10, 11, 12, 15)
N =

3Solutions

1.Diodes & transistors

Answer: R = 230 Ω

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).

Voltage across the resistor

VR = 9 − 2·2.2 = 4.6 V

Resistance

R = 4.6/0.02 = 230 Ω

Answer

R = 230 Ω

The resistor dissipates 92 mW.

2.Diodes & transistors

Answer: IC = 40 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)/10 kΩ = 430 µA

Saturated or active?

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

β·IB = 64.5 mA
IC(sat) = (9 − 0.2)/220 = 40 mA

Collector current

IC = IC(sat) = 40 mA

Answer

IC = 40 mA

The transistor is saturated.

3.Op-amp circuits

Answer: V− = 0.9536 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 inputs

R₃ and R₄ carry the same current, so they form a voltage divider; feedback makes V₋ = V₊.

V₊ = V2·R4/(R3 + R4) = 1.4·47/(22 + 47) = 0.9536 V
V₋ = V₊

Answer

V− = 0.9536 V
4.Op-amp circuits

Answer: If = −1.55 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 = −1.7/1 = −1.7 mA
I2 = V2/R2 = 1.5/10 = 0.15 mA
If = I1 + I2 = −1.55 mA

Answer

If = −1.55 mA
5.RC & RL transients

Answer: vL = 1.726 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 = 47 mH / 10 Ω = 4.7 ms
i(∞) = Vs/R = 5/10 = 0.5 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 = 5·e−5/4.7 = 1.726 V

Answer

vL = 1.726 V
6.RC & RL transients

Answer: C = 10.91 µF

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

9 = 15·(1 − e−10/τ) → τ = 10/ln(15/(15 − 9))
τ = 10/0.9163 = 10.91 ms

Capacitance

kΩ times µF gives milliseconds.

C = τ/R = 10.91/1 = 10.91 µF

Answer

C = 10.91 µF
7.Series & parallel resistors

Answer: Req = 17.55 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​ = 4 Ω+−V1​24 VR2​4 ΩAR4​3 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 = 4 + 3 = 7 Ω
R2 ∥ 7 = 4·7/(4+7) = 2.545 Ω
Req = R1 + 2.545 = 15 + 2.545 = 17.55 Ω

Answer

Req = 17.55 Ω
8.Series & parallel resistors

Answer: IR2 = 0.1644 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​ = 4 ΩR5​ = 2 Ω+−V1​6 VR2​20 ΩAR4​3 ΩBR6​10 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 = 2 + 10 = 12 Ω
R4 ∥ 12 = 2.4 Ω
R3 + 2.4 = 6.4 Ω
R2 ∥ 6.4 = 4.848 Ω
Req = R1 + 4.848 = 4 + 4.848 = 8.848 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 = 6/8.848 = 0.6781 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 = 6 − 0.6781·4 = 3.288 V
IR2 = VA/R2 = 3.288/20 = 0.1644 A

Answer

IR2 = 0.1644 A
9.DC-DC converters

Answer: ΔIL = 0.2553 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 = 12/(12 + 12) = 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/(47·10⁻⁶·500·10³) = 0.2553 A

Answer

ΔIL = 0.2553 A
10.DC-DC converters

Answer: Lcrit = 0.64 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 = 13.5/(9 + 13.5) = 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)²·2/(2250·10³) = 0.64 µH

Answer

Lcrit = 0.64 µH
11.Wheatstone bridge & strain gauges

Answer: Ig = 15995 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 = 9·(250/450 − 40/340) = 3.941 V

Thévenin resistance

Rth = R₁∥R₂ + R₃∥R₄ = 146.4 Ω

Galvanometer current

Ig = 3.941/(146.4 + 100) = 15995 µA

Answer

Ig = 15995 µA
12.Wheatstone bridge & strain gauges

Answer: σ = 52.5 MPa

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.

Strain

ε = 4·0.001125/(3·2) = 0.00075

Stress

σ = 70·10³ MPa·0.00075 = 52.5 MPa

Answer

σ = 52.5 MPa
13.Digital logic: gates, K-maps & flip-flops

Answer: AB = 01, CD = 00

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.

m4: m5, m6, m0, m12 → 0
ABCD00011110000111101111

The isolated 1

m4 = A′BC′D′ → AB = 01, CD = 00

Answer

AB = 01, CD = 00
14.Digital logic: gates, K-maps & flip-flops

Answer: N = 3

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.

CD, A′B′D, ABD, ABC′
ABCD00011110000111100011130204051706X12113X150140809X11X10

Minimal cover

F = CD + A′B′D + ABD
N = 3

Answer

N = 3

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

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