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
A 6.2 V Zener regulator is fed from 18 V through 680 Ω and supplies a 2200 Ω load. Find the Zener current IZ.
Vin = 18 VVZ = 6.2 VR = 680 ΩRL = 2200 Ω
IZ = mA
2.Diodes & transistorsHard
A diode is modelled as 0.65 V in series with 20 Ω (it conducts above 0.65 V). It is in series with a 330 Ω resistor across a 6 V supply. Find the operating current ID where the diode line meets the load line.
Vs = 6 VR = 330 ΩV0 = 0.65 Vrd = 20 Ω
ID = mA
3.Op-amp circuitsMedium
Choose the feedback resistor Rf that gives this non-inverting amplifier a voltage gain of 3.
R1 = 1 kΩAv = 3
Rf = kΩ
4.Op-amp circuitsHard
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 VV2 = 0.3 VR1 = 10 kΩR2 = 47 kΩRf = 10 kΩ
If = mA
5.RC & RL transientsMedium
The inductor carries a steady current of 1.5 A. At t = 0 the switch closes the loop through R and the source is removed, so the inductor current decays through R. Find the current i at t = 5 ms.
i(0) = 1.5 AR = 22 ΩL = 47 mHt = 5 ms
i = A
6.RC & RL transientsHard
The switch across R2 has been closed for a long time, so the inductor current is steady. At t = 0 the switch opens. How long after t = 0 does the inductor current reach 0.506 A? Find t.
Vs = 12 VR1 = 20 ΩR2 = 22 ΩL = 33 mH
t = ms
7.Series & parallel resistorsMedium
Find the current IR1 delivered by the source, which flows through R1.
V1 = 9 VR1 = 6 ΩR2 = 6 ΩR3 = 10 ΩR4 = 4 Ω
IR1 = A
8.Series & parallel resistorsHard
Find the equivalent resistance Req seen by the source V1.
An ideal buck converter turns 9 V into 6.3 V at 50 kHz with L = 33 µH. Find the peak-to-peak inductor ripple current ΔIL.
Vin = 9 VVo = 6.3 Vf = 50 kHzL = 33 µH
ΔIL = A
10.DC-DC convertersHard
A buck converter turns 48 V into 19.2 V for a 10 Ω load at 500 kHz, with L = 220 µH and C = 220 µF. Find the peak-to-peak output voltage ripple ΔVo in mV.
A 200 Ω strain gauge is one arm (R₂) of a bridge with four equal 200 Ω arms and an excitation of 10 V. Find the power Pg dissipated in the gauge, in mW. Self-heating limits the excitation.
Vs = 10 VR = 200 Ω
Pg = mW
12.Wheatstone bridge & strain gaugesHard
A quarter bridge (one active gauge, GF = 2.1) is excited with 2.5 V. The largest strain to be measured is 800 µε, and it must give 5 V at the input of an analogue-to-digital converter. Find the amplifier gain G.
A 4-to-1 multiplexer has its select inputs S₁ = A and S₀ = B, and its data inputs tied to I₀ = 0, I₁ = 0, 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 = 0I₂ = C′I₃ = C′
N =
14.Digital logic: gates, K-maps & flip-flopsHard
Find the minimal SOP form of F(A, B, C, D) = Σm(0, 1, 7, 11, 12, 14) + d(4, 5, 8, 9, 15), where d marks the don't-care conditions. How many product terms N does it have?
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.
Resistor current
IR = 11.8/680 = 17.35 mA
Load current
IL = 6.2/2200 = 2.818 mA
Zener current
IZ = 17.35 − 2.818 = 14.53 mA
Answer
IZ = 14.53 mA
2.Diodes & transistors
Answer: ID = 15.29 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
6 = 0.65 + I·(330 + 20)
Operating current
ID = 5.35/350 = 15.29 mA
VD = 0.65 + 0.01529·20 = 0.9557 V
Answer
ID = 15.29 mA
3.Op-amp circuits
Answer: Rf = 2 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 = (3 − 1)·1 = 2 kΩ
Answer
Rf = 2 kΩ
4.Op-amp circuits
Answer: If = 0.1064 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 = 1/10 = 0.1 mA
I2 = V2/R2 = 0.3/47 = 0.006383 mA
If = I1 + I2 = 0.1064 mA
Answer
If = 0.1064 mA
5.RC & RL transients
Answer: i = 0.1444 A
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 = 47 mH / 22 Ω = 2.136 ms
Decay of the current
i(t) = 1.5·e−5/2.136 = 0.1444 A
Answer
i = 0.1444 A
6.RC & RL transients
Answer: t = 0.2792 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
Before t = 0 the closed switch bypasses R₂; afterwards R₁ and R₂ are both in the loop.
i(0) = 12/20 = 0.6 A
i(∞) = 12/(20 + 22) = 0.2857 A
τ = L/R = 33/42 = 0.7857 ms
i(t) = 0.2857 + (0.6 − 0.2857)·e−t/τ
Solve for the time
e−t/τ = (0.506 − 0.2857)/(0.6 − 0.2857) = 0.7009
t = 0.7857·ln(1.427) = 0.2792 ms
Answer
t = 0.2792 ms
7.Series & parallel resistors
Answer: IR1 = 0.8824 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 + 4 = 14 Ω
R2 ∥ 14 = 6·14/(6+14) = 4.2 Ω
Req = R1 + 4.2 = 6 + 4.2 = 10.2 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 = 9/10.2 = 0.8824 A
Answer
IR1 = 0.8824 A
8.Series & parallel resistors
Answer: Req = 8.396 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 = 30 + 5 = 35 Ω
R4 ∥ 35 = 10.5 Ω
R3 + 10.5 = 22.5 Ω
R2 ∥ 22.5 = 3.396 Ω
Req = R1 + 3.396 = 5 + 3.396 = 8.396 Ω
Answer
Req = 8.396 Ω
9.DC-DC converters
Answer: ΔIL = 1.145 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 = 6.3/9 = 0.7
Inductor voltage during the on-time
While S is on, the inductor sits between Vin and Vo.
VL = 9 − 6.3 = 2.7 V
Ripple current
ΔIL = VL·D/(L·f) = 2.7·0.7/(33·10⁻⁶·50·10³) = 1.145 A
Answer
ΔIL = 1.145 A
10.DC-DC converters
Answer: ΔVo = 0.119 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 = 19.2/48 = 0.4
Inductor ripple current
ΔIL = (48 − 19.2)·0.4/(220·10⁻⁶·500·10³) = 0.1047 A
Output ripple
ΔVo = 0.1047/(8·500·10³·220·10⁻⁶) = 0.119 mV
Answer
ΔVo = 0.119 mV
11.Wheatstone bridge & strain gauges
Answer: Pg = 125 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 = 10/2 = 5 V
Power
Pg = 5²/200 = 125 mW
Answer
Pg = 125 mW
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 = 1.05 mV
Gain
G = 5/0.00105 = 4762
Answer
G = 4762
13.Digital logic: gates, K-maps & flip-flops
Answer: N = 2
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 = AB′C′ + ABC′
Rows with F = 1
ABC = 100, 110
N = 2
Answer
N = 2
14.Digital logic: gates, K-maps & flip-flops
Answer: N = 4
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.
C′D′, B′C′, BCD, A′C′, ACD, A′BD, AB′D, ABD′, ABC
Minimal cover
F = B′C′ + BCD + ACD + ABD′
N = 4
Answer
N = 4
Another grouping of the same size exists; it has the same number of terms and literals.