Identify the converter (buck, boost or buck-boost) and the duty cycle D from the voltage ratio.
Use volt-second balance on the inductor: the average inductor voltage over a period is zero.
Find the inductor voltage while the switch is on, then ΔIL = VL·D/(L·f).
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
Treat the bridge as two voltage dividers across the same supply.
For balance, set R₁/R₂ = R₃/R₄ and solve for the unknown resistor.
For an unbalanced bridge, find Va and Vb from the dividers and subtract; use the Thévenin equivalent when a meter loads the output.
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
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.
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.
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.
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
2 blue LEDs (forward voltage 3.2 V each) are connected in series with a resistor to a 24 V supply. Find the resistance R that sets the current to 5 mA.
Vs = 24 VVF = 3.2 Vn = 2I = 5 mA
R = Ω
2.Diodes & transistorsHard
An NPN transistor with β = 150 switches a 470 Ω load resistor connected between VCC = 5 V and its collector. The emitter is grounded. The base is driven from a 3.3 V logic output through a base resistor RB. Take VBE = 0.7 V and VCE(sat) = 0.2 V. For reliable switching, design for a base current 4 times the minimum needed for saturation. Find RB in kΩ.
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 = 5 ms.
Vs = 12 VR1 = 6.8 kΩR2 = 1 kΩC = 22 µFt = 5 ms
vC = V
6.RC & RL transientsHard
The switch has been closed for a long time, so the circuit is in steady state. At t = 0 the switch opens. Find the current i2 through R2 at t = 1000 ms.
Vs = 15 VR1 = 3.3 kΩR2 = 10 kΩC = 47 µFt = 1000 ms
i2 = mA
7.Series & parallel resistorsMedium
Find the current IR1 delivered by the source, which flows through R1.
V1 = 30 VR1 = 10 ΩR2 = 20 ΩR3 = 10 ΩR4 = 10 Ω
IR1 = A
8.Series & parallel resistorsHard
Find the equivalent resistance Req seen by the source V1.
A bridge with four 470 Ω arms is supplied with 9 V. When the sensor R₂ changes, the output reads Vab = 173.1 mV. Find the exact change ΔR of R₂.
Vs = 9 VR = 470 ΩVab = 173.1 mV
ΔR = Ω
12.Wheatstone bridge & strain gaugesHard
A load cell (a full bridge of strain gauges) has a rated output of 2.5 mV/V at its rated load of 200 kg. It is excited with 12 V. Find its output Vo under a load of 80 kg.
A 4-to-1 multiplexer has its select inputs S₁ = A and S₀ = B, and its data inputs tied to I₀ = 1, I₁ = C′, I₂ = 1, I₃ = C′. For how many of the 8 combinations of A, B and C is the output F = 1? Find N.
I₀ = 1I₁ = C′I₂ = 1I₃ = C′
N =
14.Digital logic: gates, K-maps & flip-flopsHard
A synchronous mod-11 counter counts 0, 1, …, 10 and then returns to 0. It starts at 3. Which count Q (in decimal) does it show after 37 clock pulses?
Q0 = 337N = 11
Q =
3Solutions
1.Diodes & transistors
Answer: R = 3520 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 = 24 − 2·3.2 = 17.6 V
Resistance
R = 17.6/0.005 = 3520 Ω
Answer
R = 3520 Ω
The resistor dissipates 88 mW.
2.Diodes & transistors
Answer: RB = 9.547 kΩ
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.
Collector current in saturation
IC(sat) = (5 − 0.2)/470 = 10.21 mA
Minimum base current
IB(min) = IC(sat)/β = 10.21/150 = 68.09 µA
Design base current
IB = 4·68.09 µA = 272.3 µA
Base resistor
RB = (3.3 − 0.7)/IB = 2.6 V/0.2723 mA = 9.547 kΩ
Answer
RB = 9.547 kΩ
3.Op-amp circuits
Answer: V− = 0.6667 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) = 1·2/(1 + 2) = 0.6667 V
V₋ = V₊
Answer
V− = 0.6667 V
4.Op-amp circuits
Answer: Vout = 2.444 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 = −0.6/1 = −0.6 mA
I2 = V2/R2 = 0.8/10 = 0.08 mA
If = I1 + I2 = −0.52 mA
Output voltage
Vout = −Rf·If = −4.7·(−0.52) = 2.444 V
Answer
Vout = 2.444 V
5.RC & RL transients
Answer: vC = 0.3531 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 = 6.8·1/(6.8 + 1) = 0.8718 kΩ
vC(∞) = 12·1/(6.8 + 1) = 1.538 V
Time constant
τ = Rth·C = 0.8718·22 = 19.18 ms
Charging curve
vC(t) = 1.538·(1 − e−5/19.18) = 0.3531 V
Answer
vC = 0.3531 V
6.RC & RL transients
Answer: i2 = 0.1343 mA
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 capacitor voltage
In steady state the capacitor is an open circuit, so R₁ and R₂ form a voltage divider. The capacitor voltage cannot jump when the switch opens.
vC(0) = 15·10/(3.3 + 10) = 11.28 V
Time constant after the switch opens
τ = R2·C = 10·47 = 470 ms
Discharge
vC(t) = 11.28·e−1000/470 = 1.343 V
i2 = vC/R2 = 1.343/10 = 0.1343 mA
Answer
i2 = 0.1343 mA
7.Series & parallel resistors
Answer: IR1 = 1.5 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.
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 + 10 = 20 Ω
R2 ∥ 20 = 20·20/(20+20) = 10 Ω
Req = R1 + 10 = 10 + 10 = 20 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 = 30/20 = 1.5 A
Answer
IR1 = 1.5 A
8.Series & parallel resistors
Answer: Req = 13.39 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.
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 + 8 = 12 Ω
R4 ∥ 12 = 2.4 Ω
R3 + 2.4 = 22.4 Ω
R2 ∥ 22.4 = 3.394 Ω
Req = R1 + 3.394 = 10 + 3.394 = 13.39 Ω
Answer
Req = 13.39 Ω
9.DC-DC converters
Answer: Imax = 5.573 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 = 21.6/36 = 0.6
Average and ripple current
Io = 21.6/4 = 5.4 A
ΔIL = VL·D/(L·f) = 14.4·0.6/(100·10⁻⁶·250·10³) = 0.3456 A
Peak current
Imax = 5.4 + 0.3456/2 = 5.573 A
Answer
Imax = 5.573 A
10.DC-DC converters
Answer: C = 3.273 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 = 28.8/48 = 0.6
Inductor ripple current
ΔIL = (48 − 28.8)·0.6/(220·10⁻⁶·200·10³) = 0.2618 A
Capacitance
C = 0.2618/(8·200·10³·50·10⁻³) = 3.273 µF
Answer
C = 3.273 µF
11.Wheatstone bridge & strain gauges
Answer: ΔR = 37.6 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 = 4.5 + 0.1731 = 4.673 V
Solve the divider
R₂ = 470·4.673/(9 − 4.673) = 507.6 Ω
ΔR = 507.6 − 470 = 37.6 Ω
Answer
ΔR = 37.6 Ω
12.Wheatstone bridge & strain gauges
Answer: Vo = 12 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.
Full-scale output
2.5·12 = 30 mV
Output at this load
Vo = 30·80/200 = 12 mV
Answer
Vo = 12 mV
13.Digital logic: gates, K-maps & flip-flops
Answer: N = 6
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′ + A′BC′ + AB′ + ABC′
Rows with F = 1
ABC = 000, 001, 010, 100, 101, 110
N = 6
Answer
N = 6
14.Digital logic: gates, K-maps & flip-flops
Answer: Q = 7
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 11 pulses bring the counter back to the same state.