NivaarExam PrepOfficial exam papers ↗

22-Elec-B5 Advanced Electronics · December 2013

Question 3 of 5: Series Voltage Regulator — Output, Ripple and Efficiency

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams December 2013, 07‑Elec‑B5 Advanced Electronics — 3 hours, CLOSED BOOK, any non‑communicating calculator permitted. Answer all FIVE (5) questions; all questions are worth 20 marks each. Op‑amps may be assumed ideal and supply voltages ±15 V unless stated otherwise; ground and chassis are common in every schematic.

Reference texts. A. S. Sedra and K. C. Smith, Microelectronic Circuits, 8th ed. (Oxford) — Ch. 8 (differential and multistage amplifiers), Ch. 10 (frequency response), Ch. 13 (signal generators and waveform shaping), Ch. 17 (power amplifiers and regulators); B. Razavi, Design of Analog CMOS Integrated Circuits, 2nd ed. (McGraw‑Hill) — Ch. 4 (differential amplifiers) and Ch. 6 (frequency response). Both are on the Engineers Canada / EGBC reading list for this examination code.

Question 3: Series Voltage Regulator — Output, Ripple and Efficiency (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. A series regulator in which $R_1$ and the zener $D_1$ form the reference, the ideal op‑amp $A_1$ compares that reference with the output through a unity‑gain feedback path, and a Darlington pair $Q_1$–$Q_2$ passes the load current from $V_{DD}$.

Given data
Raw supply $V_{DD}$$10\ \text{V}$Zener knee $V_Z$ at $I_Z$$6.7\ \text{V}$ at $1\ \text{mA}$
Zener dynamic resistance $R_Z$$10\ \text{k}\Omega$Reference feed $R_1$$3.3\ \text{k}\Omega$
Load resistance $R_L$$4\ \Omega$Transistor current gain $\beta$$100$
Base‑emitter drop $V_{BE}$$0.7\ \text{V}$Supply ripple (part b)$1\ \text{V}$ peak‑to‑peak

Find. The nominal regulated output, the peak‑to‑peak ripple that survives at the output, and the power efficiency of the regulator.

+VDDR1VZD1+−A1Q1Q2+VDDRL+−Vout
Question 3 — series regulator. R1 and D1 set the reference at the non‑inverting input; the output is fed back directly to the inverting input, so the loop forces Vout = VZ. Q1 and Q2 form a Darlington pass element.

Approach. Locate the zener on its piecewise‑linear characteristic to get the reference, propagate that through the unity‑gain loop for both the d.c. level and the ripple, then account for every ampere drawn from $V_{DD}$ to form the efficiency.

  1. Part (a) — place the zener on its own load line. Model the diode as a battery in series with $R_Z$: from the quoted point, $V_{Z0}=V_Z-I_ZR_Z=6.7-(1\times10^{-3})(10\times10^{3})=-3.3\ \text{V}$, so $V_z=V_{Z0}+I R_Z$ with $I=(V_{DD}-V_z)/R_1$. Solving the two together, $$V_z=\frac{V_{Z0}+R_ZV_{DD}/R_1}{1+R_Z/R_1}=6.70\ \text{V},\qquad I=\frac{10-6.70}{3300}=1.00\ \text{mA}$$ The bias lands exactly on the quoted 1 mA test point, confirming that $R_1$ was chosen for it.
  2. Close the loop. The op‑amp is ideal and the output is returned undivided to its inverting input, so the loop drives $V_-\to V_+$: $$V_{OUT}=V_z=\boxed{6.70\ \text{V}}$$ The Darlington sits inside the loop, so neither $V_{BE1}$ nor $V_{BE2}$ appears in the answer — the op‑amp simply raises its output by 1.4 V to cover them.
  3. Part (b) — ask where ripple can enter. Ripple on $V_{DD}$ reaches the output by two routes: through the pass transistors, and through the reference. The first is killed by the loop — with an ideal op‑amp the loop gain is infinite, so the output is pinned to whatever the non‑inverting input says, independent of the collector supply. Only the reference route survives.
  4. Divide the ripple between $R_1$ and the zener. To small signals the diode is just $R_Z$, so $R_1$ and $R_Z$ form a divider: $$\frac{v_z}{v_{dd}}=\frac{R_Z}{R_1+R_Z}=\frac{10}{3.3+10}=0.752$$ and since the output follows $v_z$ one for one, $$v_{OUT,\text{ripple}}=0.752\times1\ \text{V}_{pp}=\boxed{0.75\ \text{V}_{pp}}$$
  5. Read what that means. Three quarters of the line ripple appears at the output; the regulator regulates against load changes but barely at all against the line. The culprit is the printed $R_Z=10\ \text{k}\Omega$, which is two to three orders of magnitude larger than a real zener’s dynamic resistance. Were $r_z$ a realistic $20\ \Omega$ the divider would give $20/3320=0.6\ \%$, i.e. about $6\ \text{mV}_{pp}$; the standard cure is to bootstrap the reference feed off the regulated output instead of off $V_{DD}$.
  6. Part (c) — useful power out. The load draws $I_L=V_{OUT}/R_L=6.70/4=1.675\ \text{A}$, so $$P_{out}=V_{OUT}I_L=\frac{V_{OUT}^{2}}{R_L}=\frac{6.70^{2}}{4}=11.22\ \text{W}$$
  7. Account for every path from the supply. The load current is the emitter current of $Q_2$, so $I_{B2}=I_L/(\beta+1)=1.675/101=16.58\ \text{mA}$ and $I_{C2}=1.658\ \text{A}$. That base current is in turn the emitter current of $Q_1$, giving $I_{C1}=16.58\times(100/101)=16.42\ \text{mA}$. Adding the 1.00 mA reference branch, $$I_{DD}=I_{C1}+I_{C2}+I_{R1}=0.01642+1.6584+0.001=1.676\ \text{A}$$
  8. Form the efficiency. $$\eta=\frac{P_{out}}{P_{in}}=\frac{11.22}{(10)(1.676)}=\frac{11.22}{16.76}=\boxed{67.0\ \%}$$ The simple estimate $\eta\approx V_{OUT}/V_{DD}=67.0\ \%$ is indistinguishable, because the base and reference currents together amount to only 1 % of the load current. The missing 5.54 W is dropped across the Darlington as heat, which is the defining limitation of every linear series regulator and the reason a switching pre‑regulator is used when the raw supply sits far above the regulated rail.
Final results
QuantitySymbolValue
Reference operating point$V_z$, $I_Z$$6.70\ \text{V}$ at $1.00\ \text{mA}$
(a) Nominal output voltage$V_{OUT}$$6.70\ \text{V}$
(b) Line‑ripple transfer$R_Z/(R_1+R_Z)$$0.752$
(b) Output ripple$v_{OUT,pp}$$0.75\ \text{V}$ peak‑to‑peak
Load current and output power$I_L$, $P_{out}$$1.675\ \text{A}$, $11.22\ \text{W}$
Total supply current and input power$I_{DD}$, $P_{in}$$1.676\ \text{A}$, $16.76\ \text{W}$
(c) Power efficiency$\eta$$67.0\ \%$
Heat in the pass pair$P_{diss}$$5.54\ \text{W}$

Check — the zener dynamic resistance is used exactly as printed ($R_Z=10\ \text{k}\Omega$), even though a 6.7 V zener at 1 mA would normally show 10–100 Ω. The op‑amp’s own quiescent supply current is neglected, as instruction 7 and the “ideal” label allow.