SmallSignal Modeling Dr David W Graham West Virginia

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Small-Signal Modeling Dr. David W. Graham West Virginia University Lane Department of Computer Science

Small-Signal Modeling Dr. David W. Graham West Virginia University Lane Department of Computer Science and Electrical Engineering © 2010 David W. Graham 1

Small-Signal Modeling • An approximation to the large-signal model around an operating point •

Small-Signal Modeling • An approximation to the large-signal model around an operating point • Assumes perturbations in the bias conditions are small • Can use a linearized model for small changes 2

Small-Signal Modeling • Assumptions – Transistor is biased at some current level – Saturated

Small-Signal Modeling • Assumptions – Transistor is biased at some current level – Saturated operation (typically) – Only small potential changes at the terminals (G, S, D, B) • Consequences – DC bias levels (currents & voltages) can be ignored – Any voltage change at any terminal will modify the channel current 3

Different Small-Signal Models • Bulk-referred model • Source-referred model • T model 4

Different Small-Signal Models • Bulk-referred model • Source-referred model • T model 4

Bulk-Referred Small-Signal Model (Low Frequency) 5

Bulk-Referred Small-Signal Model (Low Frequency) 5

Bulk Referred Small-Signal Model • Every potential is with respect to (wrt) the bulk

Bulk Referred Small-Signal Model • Every potential is with respect to (wrt) the bulk • Use VCCS to model changes in current from DC • No gate current • Increases in the gate & drain wrt the bulk increase the channel current (drain-to-source) • Increases in the source wrt the bulk decrease the channel current Total Current (centered around IBIAS) 6

Transconductance, gm Changes in the gate voltage (ΔVg) produce changes in the channel current

Transconductance, gm Changes in the gate voltage (ΔVg) produce changes in the channel current Changes in Vg change the current by gm transconductance creates a conductance at other terminals (not including the gate terminal) 7

Bulk-Referred Small-Signal Model • Derive the small signal parameters for subthreshold operation – gm

Bulk-Referred Small-Signal Model • Derive the small signal parameters for subthreshold operation – gm – gs – gd • Bulk-referred model is typically used for subthreshold modeling • (Source-referred model is typically used for above threshold modeling) 8

Source Conductance, gs Changes in the source voltage (ΔVs) produce changes in the channel

Source Conductance, gs Changes in the source voltage (ΔVs) produce changes in the channel current Changes in Vs change the current by gs source conductance creates a conductance at its own terminal 9

Drain Conductance, gd Changes in the drain voltage (ΔVd) produce changes in the channel

Drain Conductance, gd Changes in the drain voltage (ΔVd) produce changes in the channel current gd drain conductance Changes in Vd change the current by Output Resistance 10

Total Small-Signal Current (Bulk-Referred Model) 11

Total Small-Signal Current (Bulk-Referred Model) 11

Source-Referred Small-Signal Model (Low Frequency) 12

Source-Referred Small-Signal Model (Low Frequency) 12

Source-Referred Small-Signal Model • Use κ ≈ 1 Approximation • All voltages referenced to

Source-Referred Small-Signal Model • Use κ ≈ 1 Approximation • All voltages referenced to the source instead of the bulk • Traditional small-signal model for Above VT operation κ ≈ 1 Approximation 13

Source-Referred Small-Signal Model 14

Source-Referred Small-Signal Model 14

κ ≈ 1 Sub VT Parameters 15

κ ≈ 1 Sub VT Parameters 15

Simplification to the Small-Signal Models g 0 Vds is a current whose value linearly

Simplification to the Small-Signal Models g 0 Vds is a current whose value linearly depends on the voltage across it Resistor Typically use this simplification in both the source-referred and bulk referred models 16

Source-Referred Bulk-Referred Small Signal Models 17

Source-Referred Bulk-Referred Small Signal Models 17

Above VT Small-Signal Parameters, gm Typically use the source-referred model K is often referred

Above VT Small-Signal Parameters, gm Typically use the source-referred model K is often referred to as the transconductance parameter 18

Above VT Small-Signal Parameters, gmb • No Vbs terms in the current expression •

Above VT Small-Signal Parameters, gmb • No Vbs terms in the current expression • However, VT depends on Vbs λ = 1/VA 19

Above VT Small-Signal Parameters, r 0 20

Above VT Small-Signal Parameters, r 0 20

Similarities Between Small-Signal Models Bulk-Referred Model Source-Referred Model Comparison – KCL at the source

Similarities Between Small-Signal Models Bulk-Referred Model Source-Referred Model Comparison – KCL at the source for both cases Comparison 21

Consequences • Therefore, you can use either model (bulkreferred or source-referred) for any analysis

Consequences • Therefore, you can use either model (bulkreferred or source-referred) for any analysis • Use whichever model provides a simpler analysis • Typically, we use |gs| for subthreshold and (gm+gmb) for above threshold – Simply plug in the appropriate values at the end of the analysis 22

“Unified” Bulk-Referred Model Let gx = |gs| = gm + gmb (whichever is appropriate)

“Unified” Bulk-Referred Model Let gx = |gs| = gm + gmb (whichever is appropriate) 23

T Model • Useful for specific situations • For the derivation – Start from

T Model • Useful for specific situations • For the derivation – Start from the source-referred model – Assume no body effect (can be added later) • No current flows into the gate ig = 0 (KCL) vertical gmvgs is a “resistor” Two current sources in series do not add 24

Exploring the Small-Signal Parameters 25

Exploring the Small-Signal Parameters 25

Transconductance Efficiency • Transconductance for a given bias current, gm/ID • Sub VT has

Transconductance Efficiency • Transconductance for a given bias current, gm/ID • Sub VT has a constant, large transconductance efficiency • This is related to the “inversion coefficient” Holds true for n. FETs and p. FETs of various processes and sizes 26

Maximum Intrinsic Gain • Largest gain that can be achieved by a single transistor

Maximum Intrinsic Gain • Largest gain that can be achieved by a single transistor • g mr 0 gmr 0 Sub VT Above VT • Higher gain in sub VT • Faster operation in above VT Example Configuration 27