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 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 10 mA.
Vs = 9 VVF = 2.2 Vn = 2I = 10 mA
R = Ω
2.Diodes & transistorsHard
An NPN transistor with β = 150 switches a 100 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.
The inductor carries no current before the switch closes at t = 0. Find the current i at t = 1 ms.
Vs = 9 VR = 22 ΩL = 22 mHt = 1 ms
i = A
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 = 100 ms.
Vs = 10 VR1 = 10 kΩR2 = 10 kΩC = 33 µFt = 100 ms
i2 = mA
7.Series & parallel resistorsMedium
Find the current IR2 through R2.
V1 = 10 VR1 = 12 ΩR2 = 2 ΩR3 = 5 ΩR4 = 3 Ω
IR2 = A
8.Series & parallel resistorsHard
Find the current IR1 delivered by the source, which flows through R1.
An ideal buck converter turns 9 V into 2.7 V at 20 kHz with L = 47 µH. Find the peak-to-peak inductor ripple current ΔIL.
Vin = 9 VVo = 2.7 Vf = 20 kHzL = 47 µH
ΔIL = A
10.DC-DC convertersHard
An ideal boost converter turns 36 V into 90 V for a 25 Ω load at 20 kHz. Find the smallest inductance Lcrit for continuous conduction.
Vin = 36 VVo = 90 Vf = 20 kHzR = 25 Ω
Lcrit = µH
11.Wheatstone bridge & strain gaugesMedium
Find the Thévenin resistance Rth of the bridge shown, seen from the output terminals a and b.
Vs = 6 VR1 = 250 ΩR2 = 40 ΩR3 = 1000 ΩR4 = 20 Ω
Rth = Ω
12.Wheatstone bridge & strain gaugesHard
A bridge with 1000 Ω arms is excited with 3 V and has two active gauges in adjacent arms, one in tension and one in compression (half bridge). The gauge factor is 2.12 and the strain is 1200 µε. Find the bridge output Vo in mV.
A 4-to-1 multiplexer has its select inputs S₁ = A and S₀ = B, and its data inputs tied to I₀ = C′, 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 = C′I₁ = 0I₂ = CI₃ = C′
N =
14.Digital logic: gates, K-maps & flip-flopsHard
A 4-bit shift register Q₃Q₂Q₁Q₀ holds 1010. At every clock edge the bits shift one place to the right (Q₃ → Q₂ → Q₁ → Q₀, Q₀ is lost) and the serial input enters Q₃. The serial input is 1, 0, 0, 1, 0, 1 at the 6 edges. Give the final state Q = Q₃Q₂Q₁Q₀ as a decimal number.
Q₃Q₂Q₁Q₀ = 10101, 0, 0, 1, 0, 1
Q =
3Solutions
1.Diodes & transistors
Answer: R = 460 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 = 4.6/0.01 = 460 Ω
Answer
R = 460 Ω
The resistor dissipates 46 mW.
2.Diodes & transistors
Answer: IC = 2.932 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 = 2.932 mA
IC(sat) = (9 − 0.2)/100 = 88 mA
Collector current
IC = β·IB = 2.932 mA
Answer
IC = 2.932 mA
The transistor is active, so the load is not fully switched on.
3.Op-amp circuits
Answer: Vout = 8.55 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.
Inverting input follows the input
V₋ = V₊ = 1.5 V
I = V₋/R1 = 1.5/10 = 0.15 mA
Output voltage
The current through R₁ also flows through Rf.
Vout = V₋ + I·Rf = 1.5 + 0.15·47 = 8.55 V
Answer
Vout = 8.55 V
4.Op-amp circuits
Answer: Vout = −2.604 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 = 1.1/2 = 0.55 mA
I2 = V2/R2 = 0.4/100 = 0.004 mA
If = I1 + I2 = 0.554 mA
Output voltage
Vout = −Rf·If = −4.7·0.554 = −2.604 V
Answer
Vout = −2.604 V
5.RC & RL transients
Answer: i = 0.2586 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 and final current
Long after the switch closes the inductor behaves like a short circuit, so the final current is set by R alone.
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) = 10·10/(10 + 10) = 5 V
Time constant after the switch opens
τ = R2·C = 10·33 = 330 ms
Discharge
vC(t) = 5·e−100/330 = 3.693 V
i2 = vC/R2 = 3.693/10 = 0.3693 mA
Answer
i2 = 0.3693 mA
7.Series & parallel resistors
Answer: IR2 = 0.5882 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 = 5 + 3 = 8 Ω
R2 ∥ 8 = 2·8/(2+8) = 1.6 Ω
Req = R1 + 1.6 = 12 + 1.6 = 13.6 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 = 10/13.6 = 0.7353 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 = 10 − 0.7353·12 = 1.176 V
IR2 = VA/R2 = 1.176/2 = 0.5882 A
Answer
IR2 = 0.5882 A
8.Series & parallel resistors
Answer: IR1 = 0.2777 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.
R5 + R6 = 2 + 10 = 12 Ω
R4 ∥ 12 = 3 Ω
R3 + 3 = 28 Ω
R2 ∥ 28 = 13.21 Ω
Req = R1 + 13.21 = 30 + 13.21 = 43.21 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 = 12/43.21 = 0.2777 A
Answer
IR1 = 0.2777 A
9.DC-DC converters
Answer: ΔIL = 2.011 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 = 2.7/9 = 0.3
Inductor voltage during the on-time
While S is on, the inductor sits between Vin and Vo.
VL = 9 − 2.7 = 6.3 V
Ripple current
ΔIL = VL·D/(L·f) = 6.3·0.3/(47·10⁻⁶·20·10³) = 2.011 A
Answer
ΔIL = 2.011 A
10.DC-DC converters
Answer: Lcrit = 60 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 = 1 − 36/90 = 0.6
Boundary condition
Set the average inductor current equal to half the ripple current and solve for L.
Lcrit = D(1 − D)²·R/(2f)
Critical inductance
Lcrit = 0.6(1 − 0.6)²·25/(220·10³) = 60 µH
Answer
Lcrit = 60 µH
11.Wheatstone bridge & strain gauges
Answer: Rth = 54.09 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.
Supply shorted
R₁∥R₂ = 250·40/290 = 34.48 Ω
R₃∥R₄ = 1000·20/1020 = 19.61 Ω
Thévenin resistance
Rth = 54.09 Ω
Answer
Rth = 54.09 Ω
12.Wheatstone bridge & strain gauges
Answer: Vo = 3.816 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 = 2.12·1200·10⁻⁶ = 0.002544
Bridge output
Vo = Vs·GF·ε/2 = 3·0.002544/2 = 3.816 mV
Answer
Vo = 3.816 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′B′C′ + AB′C + ABC′
Rows with F = 1
ABC = 000, 101, 110
N = 3
Answer
N = 3
14.Digital logic: gates, K-maps & flip-flops
Answer: Q = 10
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.