Question 1 of 5: Design of a CMOS Differential Amplifier
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Exams, December 2018 — 16-Elec-B5
Advanced Electronics. Three hours; CLOSED BOOK, an approved Casio or Sharp
calculator permitted. Five questions, all to be answered, 20 marks each. Op-amps are
ideal and supplies are ±15 V unless a question says otherwise; in schematics
ground and chassis are common.
Reference texts. A. S. Sedra and K. C. Smith,
Microelectronic Circuits, 8th ed. (the paper cites it by name for Question 3)
— Ch. 8 differential and multistage amplifiers, Ch. 10 output stages and power
amplifiers, Ch. 11 frequency response and compensation, Ch. 12 feedback, Ch. 17 tuned
amplifiers. B. Razavi, Design of Analog CMOS Integrated Circuits, 2nd ed.,
Ch. 4 (differential amplifiers) and Ch. 10 (stability and frequency compensation).
P. Gray, P. Hurst, S. Lewis and R. Meyer, Analysis and Design of Analog Integrated
Circuits, 5th ed., Ch. 4 (current mirrors) and Ch. 9 (frequency response of
feedback amplifiers).
Check: figure readings taken from the printed schematics. Three of the five figures need careful reading, and two of them contradict a plain
reading of the accompanying prose. In Question 1 the input pair M1/M2
is a p-channel pair whose common source node is fed by M5, with
M3/M4 as n-channel current-source loads — M6
and M7 are the two diode-connected devices of the reference string, not
signal-path loads. In Question 4 the input vIN drives the source of
M1 and the gate is tied to the R1/R2 tap, so the
forward path is a common-gate stage; were the input on the gate, part (a)'s RIN
would be infinite and its 8 marks unearnable. Both readings are stated where they are
used.
Question 1: Design of a CMOS Differential Amplifier (20 marks)
Given. A single-stage CMOS differential amplifier on
±1.5 V rails, biased from one reference string, with every threshold magnitude
equal and the two mobility-oxide products in a fixed ratio.
Design data, Question 1
Quantity
Symbol
Value
Supply rails
$V_{DD} = |V_{SS}|$
1.5 V
Threshold magnitude
$|V_{TH}|$
0.5 V
n-channel process constant
$\mu_n C_{ox}$
250 µA/V2
p-channel process constant
$\mu_p C_{ox}$
100 µA/V2
Channel-length modulation
$\lambda$
0.1 V−1
Required differential gain
$A_d$
50 V/V
Reference and bias currents
$I_{ref} = I_{bias}$
200 µA
PMOS mirror gate voltage
$V_{G5} = V_{G6}$
+0.8 V
NMOS mirror gate voltage
$V_{G3} = V_{G4} = V_{G7}$
−0.8 V
Find. The reference resistor $R$, and for each of M1 to
M7 the drain current $|I_{DS}|$, the gate-source voltage $|V_{GS}|$ and the
aspect ratio $W/L$ that together meet all four specifications.
[Figure not reproduced: Figure 1.1 — The amplifier as printed, redrawn with the branch currents this design establishes. M 6 , R and M 7 form the reference string; M 5 mirrors it as the tail; M 1 /M 2 are the PMOS input pair and M 3 /M 4 are the NMOS current-source loads. See the official exam paper.]
Approach. Read the bias string first — it fixes every
overdrive except that of the input pair — then take the pair's overdrive from the
gain specification, and finally invert the saturation square law once per device.
Identify what each device does. M6 (diode-connected
PMOS), $R$ and M7 (diode-connected NMOS) form a series string from
$+V_{DD}$ to $-V_{SS}$ carrying $I_{ref}$. M5 takes its gate from
M6 and therefore mirrors $I_{ref}$ into the amplifier as the tail current
$I_{bias}$; M3 and M4 take their gates from M7 and act
as current-source loads. M1 and M2 are the p-channel
input pair: their sources meet at the tail node, their drains are sunk by M3
and M4, and the output $v_{do}$ is taken differentially between the
two drains. Nothing in the signal path is diode-connected, so both drain nodes are high
impedance.
Convert the specified gate voltages into overdrives. For the
p-channel mirror devices the source sits on $+V_{DD}$, so
$$\begin{aligned}|V_{GS5}| &= |V_{GS6}| = V_{DD} - V_{G5} = 1.5 - 0.8 = 0.7\ \text{V} \\ |V_{ov5}| &= |V_{GS5}| - |V_{TH}| = 0.2\ \text{V}.\end{aligned}$$
For the n-channel mirror devices the source sits on $-V_{SS}$, so
$V_{GS3} = V_{G3} - (-V_{SS}) = -0.8 + 1.5 = 0.7$ V and $V_{ov3} = 0.2$ V as well. The
paper has chosen the two gate voltages so that every bias device runs at the
same 0.2 V overdrive.
Assign the branch currents. The reference string carries
$I_{ref} = 200\ \mu\text{A}$ through both M6 and M7. M5
mirrors it, so the tail current is $I_{bias} = 200\ \mu\text{A}$; a balanced pair splits
that equally, and each load must sink exactly what its half of the pair delivers:
$$\boxed{\begin{aligned}|I_{D1}| &= |I_{D2}| = I_{D3} = I_{D4} = 100\ \mu\text{A} \\ |I_{D5}| &= |I_{D6}| = I_{D7} = 200\ \mu\text{A}\end{aligned}}$$
Size the reference resistor from the two diode drops. A
diode-connected device holds its drain at its own gate voltage, so the top of $R$ sits
at $V_{D6} = V_{G6} = +0.8$ V and the bottom at $V_{D7} = V_{G7} = -0.8$ V. The whole
1.6 V appears across $R$ at $I_{ref}$:
$$R = \frac{V_{G6} - V_{G7}}{I_{ref}} = \frac{0.8 - (-0.8)}{200 \times 10^{-6}}
= \boxed{8.0\ \text{k}\Omega}$$
This single resistor is what sets the whole bias point of the amplifier.
Find the output resistance the gain must work against. Channel-length
modulation is neglected for the d.c. bias but is exactly what gives the loads their finite
output resistance. With $\lambda = 0.1\ \text{V}^{-1}$ at 100 µA,
$$\begin{aligned}r_{o2} &= r_{o4} = \frac{1}{\lambda I_D} = \frac{1}{0.1 \times 100 \times 10^{-6}}
= 100\ \text{k}\Omega \\ r_{o2}\,\|\,r_{o4} &= 50\ \text{k}\Omega.\end{aligned}$$
Turn the gain specification into a transconductance. For a
differential output taken between the two drains the differential half-circuit gives
$A_d = g_{m1}(r_{o2}\,\|\,r_{o4})$, so
$$g_{m1} = \frac{A_d}{r_{o2}\,\|\,r_{o4}} = \frac{50}{50 \times 10^{3}}
= \boxed{1.0\ \text{mA/V}}$$
Recover the input pair's overdrive and gate drive. Using
$g_m = 2 I_D / |V_{ov}|$ at the 100 µA found in step 3,
$$\begin{aligned}|V_{ov1}| &= \frac{2 I_{D1}}{g_{m1}} = \frac{2(100 \times 10^{-6})}{1.0 \times 10^{-3}}
= 0.20\ \text{V} \\ |V_{GS1}| &= |V_{TH}| + |V_{ov1}| = 0.70\ \text{V}.\end{aligned}$$
The input pair therefore also lands at a 0.2 V overdrive — a pleasant consequence
of the numbers chosen, not something imposed.
Invert the square law once per device. In saturation
$I_D = \tfrac{1}{2}\mu C_{ox}(W/L)V_{ov}^{2}$, hence $W/L = 2 I_D / (\mu C_{ox} V_{ov}^{2})$
with $\mu_p C_{ox} = \mu_n C_{ox}/2.5 = 100\ \mu\text{A/V}^2$. Every overdrive is 0.2 V,
so $V_{ov}^2 = 0.04\ \text{V}^2$ throughout and the ratios follow directly:
$$\begin{aligned}\left(\frac{W}{L}\right)_{1,2} &= \frac{2(100\,\mu)}{(100\,\mu)(0.04)} = 50 \\ \left(\frac{W}{L}\right)_{3,4} &= \frac{2(100\,\mu)}{(250\,\mu)(0.04)} = 20\end{aligned}$$
$$\begin{aligned}\left(\frac{W}{L}\right)_{5,6} &= \frac{2(200\,\mu)}{(100\,\mu)(0.04)} = 100 \\ \left(\frac{W}{L}\right)_{7} &= \frac{2(200\,\mu)}{(250\,\mu)(0.04)} = 40.\end{aligned}$$
The mirror ratios fall out as they must: M5:M6 is 1:1 because
$I_{bias} = I_{ref}$, while M3:M7 and M4:M7
are 1:2 because each load carries half the tail.
Confirm the operating point is legal. With the input gates at
0 V d.c. the pair's common source node sits at $|V_{GS1}| = +0.70$ V, leaving
M5 with $|V_{DS5}| = 1.5 - 0.7 = 0.8\ \text{V} \gg 0.2$ V of headroom. The
output d.c. level may sit anywhere between $-V_{SS} + V_{ov3} = -1.30$ V (below which the
loads leave saturation) and $V_{S1} - |V_{ov1}| = +0.50$ V (above which the pair does),
a comfortable 1.8 V window on a 3 V total supply.
Every specification is now met simultaneously, and the design is described completely
by one resistor and seven aspect ratios.
Final results, Question 1
Device
Type
Role
$|I_{DS}|$
$|V_{GS}|$
$|V_{ov}|$
$W/L$
M1
PMOS
input pair
100 µA
0.70 V
0.20 V
50
M2
PMOS
input pair
100 µA
0.70 V
0.20 V
50
M3
NMOS
current-source load
100 µA
0.70 V
0.20 V
20
M4
NMOS
current-source load
100 µA
0.70 V
0.20 V
20
M5
PMOS
tail current source
200 µA
0.70 V
0.20 V
100
M6
PMOS
mirror reference (diode)
200 µA
0.70 V
0.20 V
100
M7
NMOS
mirror reference (diode)
200 µA
0.70 V
0.20 V
40
$R$
—
sets $I_{ref}$
8.0 kΩ
$g_{m1}$
—
pair transconductance
1.0 mA/V
$A_d$
—
achieved differential gain
50 V/V
Check: the gain is set by the overdrive alone.
Substituting $g_m = 2I_D/|V_{ov}|$ and $r_o = 1/(\lambda I_D)$ into
$A_d = g_m(r_o\,\|\,r_o)$ collapses every current out of the expression and leaves
$A_d = V_A/|V_{ov}| = 10/0.2 = 50$, with $V_A = 1/\lambda = 10$ V. The design is
therefore independent of the bias current: had the paper asked for the same gain
at 400 µA the aspect ratios would double and the gain would not move. Note also
that the problem asks for channel-length modulation to be ignored for the d.c.
calculations while retaining $\lambda$ in $r_o$ — the two uses are not in conflict,
and dropping $\lambda$ from $r_o$ as well would make the gain infinite.