This section describes BJT capacitances.
The base-emitter capacitance contains a complex diffusion term with the standard depletion capacitance formula. The diffusion capacitance is modified by model parameters TF, XTF, ITF, and VTF.
Determine the base-emitter capacitance cbe by the following formula:
where cbediff and cbedep are the base-emitter diffusion and depletion capacitances, respectively.
Determine diffusion capacitance as follows:
The forward part of the collector-emitter branch current is determined as follows:
There are two different equations for modeling the depletion capacitance. Select the proper equation by specifying option DCAP in an OPTIONS statement.
The base-emitter depletion capacitance is determined as follows:
The base-emitter depletion capacitance is determined as follows:
Limits peak depletion capacitance to FC · CJCeff or FC · CJEeff, with proper fall-off when forward bias exceeds PB (FC >= 1).
Determine the base collector capacitance cbc as follows:
where cbcdiff and cbcdep are the base-collector diffusion and depletion capacitances, respectively.
where the internal base-collector current ibc is:
There are two different equations for modeling the depletion capacitance. Select the proper equation by specifying option DCAP in an .OPTIONS statement.
Specify DCAP=1 to select one of the following equations:
Specify DCAP=2 to select one of the following equations:
The base-collector capacitance is modeled as a distributed capacitance when the model parameter XCJC is set. Since the default setting of XCJC is one, the entire base-collector capacitance is on the internal base node cbc.
Specify DCAP=1 to select one of the following equations:
Specify DCAP=2 to select one of the following equations:
where vbcx is the voltage between the external base node and the internal collector node.
The function of substrate capacitance is similar to that of the substrate diode. Switch it from the collector to the base by setting the model parameter, SUBS.
The model parameter, PTF, models excess phase. It is defined as extra degrees of phase delay (introduced by the BJT) at any frequency and is determined by the equation:
where f is in Hertz, and you can set PTF and TF. The excess phase is a delay (linear phase) in the transconductance generator for AC analysis. Use it also in transient analysis.
Star-Hspice Manual - Release 2001.2 - June 2001