written 8.4 years ago by | • modified 8.4 years ago |
Mumbai University > EXTC > Sem 3 > Analog Electronics 1
Marks: 4 M
Year: May 2014
written 8.4 years ago by | • modified 8.4 years ago |
Mumbai University > EXTC > Sem 3 > Analog Electronics 1
Marks: 4 M
Year: May 2014
written 8.4 years ago by | • modified 8.4 years ago |
Fig1 Full hybrid π model of BJT
Capacitance $C_u$ represents the transition or space charge capacitance of base collector junction and Capacitance $C_π$ is the Diffusion capacitance of emitter base junction. Diffusion capacitance of emitter base junction is directly proportional to emitter bias current and forward base transit time. Values of both the capacitors are in the range of picofarad.
$r_B$ is base spreading resistance which represents the bulk resistance of the material between the base terminal and the physical inaccessible internal node of BJT. $r_π$ is Internal base node to emitter resistance it accounts for the increase recombination base current as emitter current increases $r_u$ is Feedback resistance from internal base node to collector node it is included in the model to take in to account early effect.ro is collector to emitter resistance represents the resistance of the material between collector to emitter. $R_C$ is load resistance
High frequency model parameters of a BJT in terms of low frequency hybrid parameters is given below
1.Transconductance $g_m = I_c/V_T$
$I_c$ is the quiescent collector current (also called the collector bias or DC collector current)
$V_T =\frac{kT}{q}$is the thermal voltage calculated at approximately room temperature $(295K, 22°C or 71°F)$
2.$r_π=\frac{V_T}{I_B}$
3.$rO=\frac{V_A +V_{CE}}{I_C}$ , where $V_A$=early voltage
Early effect is the variation of collector-base depletion region width due to variation in applied
Fig1 (a) diode in normal condition (b) early effect