// BJT Bias Specifications
V
mA
V
V
MHz
// Voltage Divider Bias Circuit
Vₚₛ RC NPN BJT C / B / E R1 R2 RE CE RF OUT CB
// BJT Bias Results
Q-Point Verification
Collector current ICQ
Base current IBQ
Emitter current IEQ
VCEQ (calculated)
Stability factor S
Resistor Values
Emitter resistor RE
Collector resistor RC
Divider R1 (to VCC)
Divider R2 (to GND)
Nearest E24 R1
Nearest E24 R2
Bypass Capacitors
Emitter bypass CE (at f)
Coupling cap CB (at f)
DC supply bypass Csupply
// Design Equations
Stability factor S: S = (1 + RB/RE) / (1 + RB/(RE·β))
where RB = R1∥R2
Target S ≤ 10 for good thermal stability

Voltage divider: VB = VCC·R2/(R1+R2)
VE = VB − VBE  ·  RE = VE/ICQ
Rule: Idivider ≈ 10×IBQ for good stability

Bypass cap: XCE = RE/10 at f → CE = 10/(2πf·RE)
Coupling cap: XCB = Zin/10 at f
// FET / HEMT Bias Specifications
V
mA
V
V
mA
MHz
// FET Bias Results
Q-Point
Gate-source voltage VGSQ
Drain current IDQ
VDSQ (verified)
Transconductance gm
Bias Resistors
Source resistor RS
Drain resistor RD
Gate resistor RG
Nearest E24 RS
Bypass Capacitors
Source bypass CS
RF choke on gate (if needed)
// FET Self-Bias Equations
JFET/depletion MOSFET self-bias:
ID = IDSS × (1 − VGS/VP
VGS = −ID × RS (source degeneration)
Solve iteratively: VGS = VP(1 − √(ID/IDSS))
→ RS = |VGS| / IDQ

pHEMT gate bias: Typically VGS = −0.5 to −0.8 V
Use negative supply or resistor divider from VDD
gm = 2√(ID·IDSS) / |VP|
// Active Bias Network

An active bias circuit uses a second transistor (or op-amp) to hold the collector/drain current constant regardless of temperature and β variation. Far more stable than passive voltage divider bias.

V
mA
V
mA
// Active Bias Results
Rset (sets reference current)
Nearest E24 Rset
Emitter degeneration RE
Tempco improvement vs passive
IC variation over β range
Mirror current ratio: IC/Iref = emitter area ratio
Rset = (VCC − VBE) / Iref
Advantage: IC tracks VBE with temperature (both VBE change at −2 mV/°C), so IC is nearly constant
IC variation with β: ΔIC/IC ≈ 2/(β+2) — very small for β≥50