VIPSolutions logo ✨ VIPSolutions

Please convert the below content to rendered equations without any changes and errors.This is a **MOS differential pair with PMOS active loads** and a **resistor (R_1) between the two output nodes**. Let’s solve each part step-by-step. --- # (a) Differential input short-circuit transconductance (G_m) ### Step 1: Differential excitation For differential input [ v_{in1} = +\frac{v_{id}}{2}, \qquad v_{in2} = -\frac{v_{id}}{2} ] Transistors **M1 and M2** form the differential pair. Small-signal drain currents: [ i_{d1} = g_{m1}\frac{v_{id}}{2} ] [ i_{d2} = -g_{m2}\frac{v_{id}}{2} ] Assuming matched devices: [ g_{m1} = g_{m2} = g_m ] --- ### Step 2: Differential output current The differential output current is [ i_{out} = i_{d1} - i_{d2} ] Substitute: [ i_{out} = g_m\frac{v_{id}}{2} ------------------- \left(-g_m\frac{v_{id}}{2}\right) ] [ i_{out} = g_m v_{id} ] --- ### Step 3: Short-circuit transconductance [ G_m = \frac{i_{out}}{v_{id}} ] [ \boxed{G_m = g_m} ] --- # (b) Differential output resistance (neglect (R_1)) In differential mode, the circuit is symmetric. Each output node sees: * (r_{o2}) from **M2** * (r_{o4}) from **M4** Thus single-side resistance: [ r_o = r_{o2} \parallel r_{o4} ] For **differential output resistance** [ R_{out,diff} = 2(r_{o2} \parallel r_{o4}) ] --- ### Final answer [ \boxed{R_{out,diff} = 2(r_{o2} \parallel r_{o4})} ] --- # (c) Differential gain including (R_1) Now (R_1) connects the two output nodes. For differential signals, **the resistor splits into two halves**: [ R_1 \rightarrow \frac{R_1}{2} \text{ to ground (each half circuit)} ] --- ### Step 1: Effective output resistance Single-side resistance becomes [ R_{out,half} = (r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2}) ] --- ### Step 2: Differential gain Differential gain: [ A_{vd} = G_m \cdot R_{out,diff} ] But differential resistance is [ R_{out,diff} = 2(R_{out,half}) ] Substitute: [ A_{vd} ====== g_m \cdot 2\left(r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2}\right) ] --- ### Final result [ \boxed{ A_{vd} ====== 2g_m \left( r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2} \right) } ] --- # Final Answers ### (a) [ \boxed{G_m = g_m} ] ### (b) [ \boxed{R_{out,diff} = 2(r_{o2} \parallel r_{o4})} ] ### (c) [ \boxed{ A_{vd} ====== 2g_m \left( r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2} \right) } ] --- If you'd like, I can also show the **half-circuit method (the trick professors expect in exams)** which makes this problem **10× faster to solve**.

Question:

Please convert the below content to rendered equations without any changes and errors.This is a **MOS differential pair with PMOS active loads** and a **resistor (R_1) between the two output nodes**. Let’s solve each part step-by-step. --- # (a) Differential input short-circuit transconductance (G_m) ### Step 1: Differential excitation For differential input [ v_{in1} = +\frac{v_{id}}{2}, \qquad v_{in2} = -\frac{v_{id}}{2} ] Transistors **M1 and M2** form the differential pair. Small-signal drain currents: [ i_{d1} = g_{m1}\frac{v_{id}}{2} ] [ i_{d2} = -g_{m2}\frac{v_{id}}{2} ] Assuming matched devices: [ g_{m1} = g_{m2} = g_m ] --- ### Step 2: Differential output current The differential output current is [ i_{out} = i_{d1} - i_{d2} ] Substitute: [ i_{out} = g_m\frac{v_{id}}{2} ------------------- \left(-g_m\frac{v_{id}}{2}\right) ] [ i_{out} = g_m v_{id} ] --- ### Step 3: Short-circuit transconductance [ G_m = \frac{i_{out}}{v_{id}} ] [ \boxed{G_m = g_m} ] --- # (b) Differential output resistance (neglect (R_1)) In differential mode, the circuit is symmetric. Each output node sees: * (r_{o2}) from **M2** * (r_{o4}) from **M4** Thus single-side resistance: [ r_o = r_{o2} \parallel r_{o4} ] For **differential output resistance** [ R_{out,diff} = 2(r_{o2} \parallel r_{o4}) ] --- ### Final answer [ \boxed{R_{out,diff} = 2(r_{o2} \parallel r_{o4})} ] --- # (c) Differential gain including (R_1) Now (R_1) connects the two output nodes. For differential signals, **the resistor splits into two halves**: [ R_1 \rightarrow \frac{R_1}{2} \text{ to ground (each half circuit)} ] --- ### Step 1: Effective output resistance Single-side resistance becomes [ R_{out,half} = (r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2}) ] --- ### Step 2: Differential gain Differential gain: [ A_{vd} = G_m \cdot R_{out,diff} ] But differential resistance is [ R_{out,diff} = 2(R_{out,half}) ] Substitute: [ A_{vd} ====== g_m \cdot 2\left(r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2}\right) ] --- ### Final result [ \boxed{ A_{vd} ====== 2g_m \left( r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2} \right) } ] --- # Final Answers ### (a) [ \boxed{G_m = g_m} ] ### (b) [ \boxed{R_{out,diff} = 2(r_{o2} \parallel r_{o4})} ] ### (c) [ \boxed{ A_{vd} ====== 2g_m \left( r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2} \right) } ] --- If you'd like, I can also show the **half-circuit method (the trick professors expect in exams)** which makes this problem **10× faster to solve**.

This is AI generated Response.
Asked by: Salaar
Created at: 2026-03-07 09:08:50

Final Answer:

Rendered Raw Text
Did you like this answer?
# MOS Differential Pair with PMOS Active Loads and Resistor \(R1\) --- ## (a) Differential Short-Circuit Transconductance (\(G_m\)) ### Step 1: Differential Excitation For differential input: \[ v_{in1 = +\frac{v_{id}}{2}, \qquad v_{in2} = -\frac{v_{id}}{2} \] Small-signal drain currents: \[ i_{d1} = g_{m1}\frac{v_{id}}{2} \] \[ i_{d2} = -g_{m2}\frac{v_{id}}{2} \] Assuming matched devices: \[ g_{m1} = g_{m2} = g_m \] --- ### Step 2: Differential Output Current \[ i_{out} = i_{d1} - i_{d2} \] \[ i_{out} = g_m\frac{v_{id}}{2} - \left(-g_m\frac{v_{id}}{2}\right) \] \[ i_{out} = g_m v_{id} \] --- ### Step 3: Short-Circuit Transconductance \[ G_m = \frac{i_{out}}{v_{id}} \] \[ \boxed{G_m = g_m} \] --- ## (b) Differential Output Resistance (Neglect \(R_1\)) In differential mode, the circuit is symmetric. Each output node sees: - \(r_{o2}\) from **M2** - \(r_{o4}\) from **M4** Single-side resistance: \[ r_o = r_{o2} \parallel r_{o4} \] Differential output resistance: \[ R_{out,diff} = 2(r_{o2} \parallel r_{o4}) \] --- ### Final Answer \[ \boxed{R_{out,diff} = 2(r_{o2} \parallel r_{o4})} \] --- ## (c) Differential Gain Including \(R_1\) Now \(R_1\) connects the two output nodes. For differential signals, the resistor splits into two halves: \[ R_1 \rightarrow \frac{R_1}{2} \text{ to ground (each half circuit)} \] --- ### Step 1: Effective Output Resistance Single-side resistance becomes: \[ R_{out,half} = (r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2}) \] --- ### Step 2: Differential Gain Differential gain: \[ A_{vd} = G_m \cdot R_{out,diff} \] But differential resistance is: \[ R_{out,diff} = 2(R_{out,half}) \] Substitute: \[ A_{vd} = g_m \cdot 2\left(r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2}\right) \] --- ### Final Result \[ \boxed{ A_{vd} = 2g_m \left( r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2} \right) } \] --- ## Final Answers ### (a) \[ \boxed{G_m = g_m} \] ### (b) \[ \boxed{R_{out,diff} = 2(r_{o2} \parallel r_{o4})} \] ### (c) \[ \boxed{ A_{vd} = 2g_m \left( r_{o2} \parallel r_{o4} \parallel \frac{R_1}{2} \right) } \]

📢 Instructions:

  • Ask anything relatd to above question only.
  • For new Question goto :

Study Help, Fast Answers

VIPSolutions focuses on clear, step‑by‑step explanations so you can learn quickly. Whether you need an AI‑generated walkthrough or a short hint to get unstuck, each solution is organized for fast reading and easy review later.

Search similar questions, compare approaches, and bookmark the best answers for revision. Our goal is simple: quick, reliable study help that feels natural—not noisy.