# 幸运飞艇超稳计划群

MacSpice > User's Guide > Analyses and Output Control

# MacSpice User's Guide

## 4 ANALYSES AND OUTPUT CONTROL

Most of the commands described in this section are deprecated but are retained to allow MacSpice to run Spice 2 'batch-mode' netlists. Where such backwards compatibility is not required, use the newer Spice 3 commands listed in section 5 within a .CONTROL / .ENDC block. Commands such as .IC and .NODESET that specify the circuit, as opposed to control the simulator, are exceptions to this rule.

The following command lines are for specifying analyses or plots within the circuit description file. Parallel commands exist in the interactive command interpreter (detailed in section 5). Specifying analyses and plots (or tables) in the input file is useful for batch runs. Batch mode is invoked with the run command. If this is given a rawfile argument then all data generated is written to a Spice 3 rawfile. In batch mode, the analyses specified by the control lines in the input file (e.g. '.AC', '.TRAN', etc.) are executed in a standard order. The rawfile may be read and subsequently analysed by using the MacSpice load command. Batch mode is entered when either the -b option is given or when the default input source is redirected from a file. In batch mode, the analyses specified by the control lines in the input file (e.g. ".AC", ".TRAN", etc.) are immediately executed (unless ".CONTROL" lines exists; see the section on the interactive command interpreter). If the -r rawfile option is given then all data generated is written to a Spice 3 rawfile. The rawfile may be read by either the interactive mode of Spice 3 or by nutmeg; see the previous section for details. In this case, the .SAVE line (see below) may be used to record the value of internal device variables (see Appendix B).

If a rawfile is not specified, then output plots (in "line-printer" form) and tables can be printed according to the .PRINT, .PLOT, and .FOUR control lines, described next.

### 4.1 SIMULATOR VARIABLES (.OPTIONS)

Various parameters of the simulations available in Spice 3 can be altered to control the accuracy, speed, or default values for some devices. These parameters may be changed via the set command (described later in the section on the interactive front-end) or via the ".OPTIONS" line:

General form:

     .OPTIONS OPT1 OPT2 ... (or OPT=OPTVAL ...)

Examples:
     .OPTIONS RELTOL=.005 TRTOL=1.2TRTOL=8


The options line allows the user to reset program control and user options for specific simulation purposes. Additional options for Nutmeg may be specified as well and take effect when Nutmeg reads the input file. Options specified to Nutmeg via the 'set' command are also passed on to Spice 3 as if specified on a .OPTIONS line. See the following section on the interactive command interpreter for the parameters which may be set with a .OPTIONS line and the format of the 'set' command. Any combination of the following options may be included, in any order. In the following table, 'x' and 'n' represent positive real and integer values respectively.

OptionEffect
abstol = xResets the absolute current error tolerance of the program. The default value is 1 picoamp.
badmos3Use the older version of the MOS3 model with the "kappa" discontinuity.
bypass = x[*] Controls whether bypass code is [1], or is not [0], used when evaluating device models. Bypassing takes shortcuts if device conditions have changed little since the last full evaluation — it helps speed, but may occasionally cause convergence problems. The default is 1.
chgtol = xResets the charge tolerance (in coulomb) of the program. The default value is 1.0e-14. It is recommended that chgtol is set to Cmin×vntol where Cmin is the smallest capacitor of interest.
defad = xResets the value for MOS drain diffusion area; the default is 0.0.
defas = xResets the value for MOS source diffusion area; the default is 0.0.
defl = xResets the value for MOS channel length; the default is 100.0 micrometer.
defw = xResets the value for MOS channel width; the default is 100.0 micrometer.
gmin = xResets the value of gmin, the minimum conductance allowed by the program. The default value is 1.0e-12.
gminsteps = n [*] Sets number of Gmin steps to be attempted when seeking a solution. The default value is 10. Setting gminsteps = 1 invokes an adaptive algorithm appropriate for cases when convergence is problematic.
itl1 = nResets the DC iteration limit. The default is 100.
itl2 = nResets the DC transfer curve (including the gmin- and source-stepping algorithms) iteration limit. The default is 50.
itl3 = nResets the lower transient analysis iteration limit. The default value is 4. (Note: not implemented in Spice 3).
itl4 = nResets the transient analysis timepoint iteration limit. The default is 10.
itl5 = nResets the transient analysis total iteration limit. The default is 5000. Set itl5 = 0 to omit this test. (Note: not implemented in Spice 3).
itl6 = n [*] Synonym for srcsteps.
keepopinfoRetain the operating point information when either an AC, Distortion, or Pole-Zero analysis is run. This is particularly useful if the circuit is large and you do not want to run a (redundant) ".OP analysis.
method = nameSets the numerical integration method used by SPICE. Possible names are "Gear" or "trapezoidal" (or just "trap"). The default is trapezoidal. [The 'trap' method is relatively fast and accurate, but tends to oscillate in switching circuits and/or long-time transient simulations. Gear tends to be more stable, but at the expense of speed. CDHW.]
maxord = n [*] Specifies the maximum order for the numerical integration method used by SPICE. Possible values for the Gear method are from 2 (the default) to 6. Using the value 1 with the trapezoidal method specifies Euler integration.
minbreak = xResets minimum time between breakpoints. The default is 5×10−5 times the maximum timestep.
pivrel = xResets the relative ratio between the largest column entry and an acceptable pivot value. The default value is 1.0e-3. In the numerical pivoting algorithm the allowed minimum pivot value is determined by epsrel = max(pivrel×maxval, pivtol) where maxval is the maximum element in the column where a pivot is sought (partial pivoting).
pivtol = xResets the absolute minimum value for a matrix entry to be accepted as a pivot. The default value is 1.0e-13.
reltol = xResets the relative error tolerance of the program. The default value is 0.001 (0.1%).
srcsteps = n [*] A non-zero value causes SPICE to use a source-stepping method to find the DC operating point. Its value specifies the number of steps. The default value is 10. Setting srcsteps = 1 invokes an adaptive algorithm appropriate for cases when convergence is problematic.
temp = xResets the operating temperature of the circuit. The default value is 27°C. The value of temp can be overridden by a temperature specification on any temperature dependent instance.
tnom = xResets the nominal temperature at which device parameters are measured. The default value is 27°C. The value of tnom can be overridden by a specification on any temperature dependent device model.
trtol = xResets the transient error tolerance. The default value is 1.0. The default value is 7.0. This parameter is an estimate of the factor by which Spice overestimates the actual truncation error.
trytocompactApplicable only to the LTRA model. When specified, the simulator tries to condense LTRA transmission lines' past history of input voltages and currents.
vntol = xResets the absolute voltage error tolerance of the program. The default value is 1 microvolt.

items marked with an asterisk '*' in the above table are in the berkeley source code but not listed in the original documentation. parameters must be lowercase but for backwards-compatibility .options lines are converted during processing.

OptionEffect
acctcauses accounting and run time statistics to be printed.
listcauses the summary listing of the input data to be printed.
nomodsuppresses the printout of the model parameters.
nopagesuppresses page ejects.
nodecauses the printing of the node table.
optscauses the option values to be printed.

### 4.2 INITIAL CONDITIONS

#### 4.2.1 .NODESET: Specify Initial Node Voltage Guesses

General form:
     .NODESET V(NODNUM)=VAL V(NODNUM)=VAL ...

Examples:
     .NODESET V(12)=4.5 V(4)=2.23


the .nodeset line helps the program find the dc or initial transient solution by making a preliminary pass with the specified nodes held to the given voltages. the restriction is then released and the iteration continues to the true solution. the .nodeset line may be necessary for convergence on bistable or a-stable circuits. in general, this line should not be necessary.

#### 4.2.2 .IC: Set Initial Conditions

General form:

     .IC V(NODNUM)=VAL V(NODNUM)=VAL ...


Examples:

     .IC V(11)=5 V(4)=-5 V(2)=2.2


The .IC line is for setting transient initial conditions. It has two different interpretations, depending on whether the UIC parameter is specified on the .TRAN control line. Also, one should not confuse this line with the .NODESET line. The .NODESET line is only to help DC convergence, and does not affect final bias solution (except for multi-stable circuits). The two interpretations of this line are as follows:

1. When the UIC parameter is specified on the .TRAN line, then the node voltages specified on the .IC control line are used to compute the capacitor, diode, BJT, JFET, and MOSFET initial conditions. This is equivalent to specifying the IC=... parameter on each device line, but is much more convenient. The IC=... parameter can still be specified and takes precedence over the .IC values. Since no DC bias (initial transient) solution is computed before the transient analysis, one should take care to specify all DC node voltages on the .IC control line if they are to be used to compute device initial conditions.

2. When the UIC parameter is not specified on the .TRAN control line, the DC bias (initial transient) solution is computed before the transient analysis. In this case, the node voltages specified on the .IC control line are forced to the desired initial values during the bias solution. During transient analysis, the constraint on these node voltages is removed. This is the preferred method since it allows SPICE to compute a consistent DC solution.

### 4.3 ANALYSES

#### 4.3.1 .AC: Small-Signal AC Analysis

General form:

     .AC DEC ND FSTART FSTOP
.AC OCT NO FSTART FSTOP
.AC LIN NP FSTART FSTOP


Examples:

     .AC DEC 10 1 10K
.AC DEC 10 1K 100MEG
.AC LIN 100 1 100HZ


DEC stands for decade variation, and ND is the number of points per decade. OCT stands for octave variation, and NO is the number of points per octave. LIN stands for linear variation, and NP is the number of points. FSTART is the starting frequency, and FSTOP is the final frequency. If this line is included in the input file, SPICE performs an AC analysis of the circuit over the specified frequency range. Note that in order for this analysis to be meaningful, at least one independent source must have been specified with an ac value.

#### 4.3.2 .DC: DC Transfer Function

General form:
     .DC SRCNAM START STOP INCR [ SRC2 START2 STOP2 INCR2 ]

Examples:
     .DC VIN 0.25 5.0 0.25
.DC VDS 0 10 .5 VGS 0 5 1
.DC VCE 0 10 .25 IB 0 10U 1U


The inclusion of this line in an input file directs SPICE to perform a DC analysis of the circuit. The DC line defines the DC transfer curve source and sweep limits (again with capacitors open and inductors shorted). SRCNAM is the name of an independent voltage or current source. The sweep parameters START, STOP, and INCR are the starting, final, and incrementing values respectively. The first example causes the value of the voltage source VIN to be swept from 0.25 volts to 5.0 volts in increments of 0.25 volts. A second source (SRC2) may optionally be specified with associated sweep parameters. In this case, the first source is swept over its range for each value of the second source. This option can be useful for obtaining semiconductor device output characteristics. See the second example circuit description in Appendix A.

macspice accepts the names of resistors and temp, representing the temperature, as sources for sweep variables. the sweep parameters are as defined above, for example:

     .DC R3 10 100 5
.DC TEMP -60 90 5


[Note: when two sources are used the transpose and reshape commands are needed to convert the results into a form suitable for plotting.]

#### 4.3.3 .DISTO: Distortion Analysis

General form:
     .DISTO DEC ND FSTART FSTOP [ F2OVERF1 ]
.DISTO OCT NO FSTART FSTOP [ F2OVERF1 ]
.DISTO LIN NP FSTART FSTOP [ F2OVERF1 ]

Examples:
     .DISTO DEC 10 1kHz 100MegHz
.DISTO DEC 10 1kHz 100MegHz 0.9


The .DISTO line performs a small-signal distortion analysis of the circuit. A multi-dimensional Volterra series幸运飞艇超稳计划群 analysis is performed using multi-dimensional Taylor series to represent the nonlinearities at the operating point. Terms of up to third order are used in the series expansions.

If the optional parameter F2OVERF1 is not specified, .DISTO does a harmonic analysis, i.e. it analyses distortion in the circuit using only a single input frequency F1, which is swept as specified by arguments of the .DISTO command exactly as in the .AC command. Inputs at this frequency may be present at more than one input source, and their magnitudes and phases are specified by the arguments of the DISTOF1 keyword in the input file lines for the input sources (see the description for independent sources). (The arguments of the DISTOF2 keyword are not relevant in this case). The analysis produces information about the AC values of all node voltages and branch currents at the harmonic frequencies 2F1 and 3F1, vs the input frequency F1 as it is swept. (A value of 1 (as a complex distortion output) signifies cos(2π(2F1)t) at 2F1 and cos(2π(3F1)t) at 3F1, using the convention that 1 at the input fundamental frequency is equivalent to cos(2πF1t).) The distortion component desired (2F1 or 3F1) can be selected using commands in nutmeg, and then printed or plotted. (Normally, one is interested primarily in the magnitude of the harmonic components, so the magnitude of the AC distortion value is looked at). It should be noted that these are the A.C. values of the actual harmonic components, and are not equal to HD2 and HD3. To obtain HD2 and HD3, one must divide by the corresponding AC values at F1, obtained from an .AC幸运飞艇超稳计划群 line. This division can be done using nutmeg commands.

If the optional F2OVERF1 parameter is specified, it should be a real number between (and not equal to) 0.0 and 1.0; in this case, .DISTO does a spectral analysis. It considers the circuit with sinusoidal inputs at two different frequencies F1 and F2. F1 is swept according to the .DISTO control line options exactly as in the .AC control line. F2 is kept fixed at a single frequency as F1 sweeps — the value at which it is kept fixed is equal to F2OVERF1 times FSTART. Each independent source in the circuit may potentially have two (superimposed) sinusoidal inputs for distortion, at the frequencies F1 and F2. The magnitude and phase of the F1 component are specified by the arguments of the DISTOF1 keyword in the source's input line (see the description of independent sources); the magnitude and phase of the F2 component are specified by the arguments of the DISTOF2 keyword. The analysis produces plots of all node voltages/branch currents at the intermodulation product frequencies F1+F2, F1F2, and (2 F1)−F2, vs the swept frequency F1. The IM product of interest may be selected using the setplot command, and displayed with the print and plot commands. It is to be noted as in the harmonic analysis case, the results are the actual AC voltages and currents at the intermodulation frequencies, and need to be normalized with respect to .AC幸运飞艇超稳计划群 values to obtain the IM parameters.

It should be carefully noted that the number F2OVERF1 should ideally be an irrational number, and that since this is not possible in practice, efforts should be made to keep the denominator in its fractional representation as large as possible, certainly above 3, for accurate results (i.e. if F2OVERF1 is represented as a fraction A/B, where A and B are integers with no common factors, B should be as large as possible; note that A<B because F2OVERF1 is constrained to be less than one). To illustrate why, consider the cases where F2OVERF1 is 49/100 and 1/2. In a spectral analysis, the outputs produced are at F1+F2, F1F2 and 2 F1F2. In the latter case, F1F2 = F2, so the result at the F1F2 component is erroneous because there is the strong fundamental F2 component at the same frequency. Also, F1+F2 = 2 F1F2 in the latter case, and each result is erroneous individually. This problem is not there in the case where F2OVERF1 = 49/100, because F1F2 = 51/100 F1 is not equal to 49/100 F1 = F2. In this case, there are two very closely spaced frequency components at F2 and F1F2. One of the advantages of the Volterra series technique is that it computes distortions at mix frequencies expressed symbolically (i.e. nF1+m F2幸运飞艇超稳计划群), therefore one is able to obtain the strengths of distortion components accurately even if the separation between them is very small, as opposed to transient analysis for example. The disadvantage is of course that if two of the mix frequencies coincide, the results are not merged together and presented (though this could presumably be done as a postprocessing step). Currently, the interested user should keep track of the mix frequencies themself and add the distortions at coinciding mix frequencies together, should it be necessary.

#### 4.3.4 .NOISE: Noise Analysis

General form:

     .NOISE V(OUTPUT [ , REF ] ) SRC [ DEC | LIN | OCT ] PTS FSTART FSTOP
+ [ PTS_PER_SUMMARY ]


Examples:

     .NOISE V(5) VIN DEC 10 1kHZ 100Mhz
.NOISE V(5,3) V1 OCT 8 1.0 1.0e6 1


The Noise line does a noise analysis of the circuit. OUTPUT is the node at which the total output noise is desired; if REF is specified, then the noise voltage V(OUTPUT)−V(REF) is calculated. By default, REF is assumed to be ground. SRC is the name of an independent voltage or current source to which input noise is referred with a non-zero AC magnitude (use 1.0 for conventional scaling). PTS, FSTART and FSTOP are .AC type parameters that specify the frequency range over which plots are desired. PTS_PER_SUMMARY is an optional integer; if specified, the noise contributions of each noise generator is produced every PTS_PER_SUMMARY幸运飞艇超稳计划群 frequency points.

The .NOISE control line produces two plots - one for the Noise Spectral Density curves and one for the total Integrated Noise over the specified frequency range. All noise voltages/currents are in squared units (V2/Hz and A2/Hz for spectral density, V2 and A2 for integrated noise).

#### 4.3.5 .OP: Operating Point Analysis

General form:

     .OP


The inclusion of this line in an input file directs SPICE to determine the DC operating point of the circuit with inductors shorted and capacitors opened. Note: a DC analysis is automatically performed prior to a transient analysis to determine the transient initial conditions, and prior to an AC small-signal, Noise, and Pole-Zero analysis to determine the linearized, small-signal models for non- linear devices (see the keepopinfo variable above).

#### 4.3.6 .PZ: Pole-Zero Analysis

General form:

     .PZ NODE1 NODE2 NODE3 NODE4 { CUR | VOL } { POL | ZER | PZ } [ VECTOR | SCALAR ]


Examples:

     .PZ 1 0 3 0 CUR POL
.PZ 2 3 5 0 VOL ZER
.PZ 4 1 4 1 CUR PZ
.PZ IN 0 OUT 0 CUR PZ VECTOR


The inclusion of this line in an input file directs SPICE to perform a pole-zero analysis. CUR stands for a transfer function of the type (output voltage)/(input current) while VOL stands for a transfer function of the type (output voltage)/(input voltage). POL stands for pole analysis only, ZER for zero analysis only and PZ for both. This feature is provided mainly because if there is a nonconvergence in finding poles or zeros, then, at least the other can be found. Finally, NODE1 and NODE2 are the two input nodes and NODE3 and NODE4 are the two output nodes. Thus, there is complete freedom regarding the output and input ports and the type of transfer function.

macspice provides an optional argument to select the output format. the default and scalar option is the traditional spice 3 one-root-per-vector format. the vector format collects all the roots into single vectors, 'poles' and 'zeros' as applicable.

the stopping-criteria for the search can be modified by setting the following variables:

 pziter The iteration limit for pole-zero analysis. This must be at least 50 and has a default value of 200. pzmaxfreq The upper limit for the range searched during pole-zero analysis. The default value is 1e22 (Hz).

In interactive mode, the command syntax is the same except that the first field is PZ instead of .PZ. To print the results, one should use the command 'print all'.

#### 4.3.7 .SENS: DC or Small-Signal AC Sensitivity Analysis

General form:

     .SENS OUTVAR
.SENS OUTVAR AC DEC ND FSTART FSTOP
.SENS OUTVAR AC OCT NO FSTART FSTOP
.SENS OUTVAR AC LIN NP FSTART FSTOP


Examples:

     .SENS V(1,OUT)
.SENS V(OUT) AC DEC 10 100 100k
.SENS I(VTEST)


The sensitivity of OUTVAR to all non-zero device parameters is calculated when the SENS analysis is specified. OUTVAR is a circuit variable (node voltage or voltage-source branch current). The first form calculates sensitivity of the DC operating-point value of OUTVAR. The second form calculates sensitivity of the AC values of OUTVAR. The parameters listed for AC sensitivity are the same as in an AC analysis (see ".AC" above). The output values are in dimensions of change in output per unit change of input (as opposed to percent change in output or per percent change of input).

#### 4.3.8 .TF: Transfer Function Analysis

General form:

     .TF OUTVAR INSRC


Examples:

     .TF V(5, 3) VIN


The TF line defines the small-signal output and input for the DC small-signal analysis. OUTVAR is the small-signal output variable and INSRC is the small-signal input source. If this line is included, SPICE computes the DC small-signal value of the transfer function (output/input), input resistance, and output resistance. For the first example, SPICE would compute the ratio of V(5, 3) to VIN, the small-signal input resistance at VIN, and the small-signal output resistance measured across nodes 5 and 3.

#### 4.3.9 .TRAN: Transient Analysis

General form:

     .TRAN TSTEP TSTOP [ [ TSTART ] TMAX ] [ UIC ]


Examples:

     .TRAN 1NS 100NS
.TRAN 1NS 1000NS 500NS
.TRAN 10NS 1US


The inclusion of this line in an input file directs SPICE to perfom a transient analysis of the circuit. TSTEP is the printing or plotting increment for line-printer output. For use with the post-processor, TSTEP is the suggested computing increment. TSTOP is the final time, and TSTART is the initial time. If TSTART is omitted, it is assumed to be zero. The transient analysis always begins at time zero. In the interval <zero, TSTART>, the circuit is analyzed (to reach a steady state), but no outputs are stored. In the interval <TSTART, TSTOP>, the circuit is analyzed and outputs are stored. TMAX is the maximum step-size that SPICE uses; for default, the program chooses either TSTEP or (TSTOP-TSTART)/50.0, whichever is larger. TMAX is useful when one wishes to guarantee a computing interval which is smaller than the printer increment, TSTEP. (See also §4.4.4 .FOUR)

[Note: I recommend that you set TMAX explicitly. Certain circuits, particularly those involving sinusoidal oscillation, fool the integrator into increasing the timestep too much. For circuits which use short pulses, TMAX should be no more than about 50 times the shortest feature of interest. There is also an internal lower limit 1e-9*TMAX imposed on TSTEP and non-convergent circuits may give 'Timestep too short' messages indicating this limit has been hit. CDHW.]

UIC (use initial conditions) is an optional keyword which indicates that the user does not want SPICE to solve for the quiescent operating point before beginning the transient analysis. If this keyword is specified, SPICE uses the values specified using IC=... on the various elements as the initial transient condition and proceeds with the analysis. If the .IC control line has been specified, then the node voltages on the .IC line are used to compute the initial conditions for the devices. Look at the description on the .IC幸运飞艇超稳计划群 control line for its interpretation when UIC is not specified.

### 4.4 BATCH OUTPUT

#### 4.4.1 .SAVE Lines

General form:

     .SAVE [ vector ... ]


Examples:

     .SAVE i(vin) input output
.SAVE @m1[id]


The vectors listed on the .SAVE line are recorded in the rawfile for use later with Spice 3 or nutmeg (nutmeg is just the data-analysis half of Spice 3, without the ability to simulate). The standard vector names are accepted. If no .SAVE line is given, then the default set of vectors are saved (node voltages and voltage source branch currents). If .SAVE lines are given, only those vectors specified are saved. For more discussion on internal device data, see Appendix B. See also the section on the interactive command interpreter for information on how to use the rawfile.

#### 4.4.2 .PRINT Lines

General form:

     .PRINT PRTYPE OV1 [ OV2 ... OV8 ]


Examples:

     .PRINT TRAN V(4) I(VIN)
.PRINT DC V(2) I(VSRC) V(23, 17)
.PRINT AC VM(4, 2) VR(7) VP(8, 3)


The PRINT line defines the contents of a tabular listing of one to eight output variables. PRTYPE is the type of the analysis (DC, AC, TRAN, NOISE, or DISTO幸运飞艇超稳计划群) for which the specified outputs are desired. The form for voltage or current output variables is the same as given in the previous section for the print command; Spice2 restricts the output variable to the following forms (though this restriction is not enforced by Spice 3):

V(N1<,N2>)
specifies the voltage difference between nodes N1 and N2. If N2 (and the preceding comma) is omitted, ground (0) is assumed. For compatibility with spice2, the following five additional values can be accessed for the ac analysis by replacing the "V" in V(N1,N2) with: VR - real part; VI - imaginary part; VM - magnitude; VP - phase; VDB - 20*log10(magnitude).
I(VXXXXXXX)
specifies the current flowing in the independent voltage source named VXXXXXXX. Positive current flows from the positive node, through the source, to the negative node. For the ac analysis, the corresponding replacements for the letter I may be made in the same way as described for voltage outputs.

#### 4.4.3 .PLOT Lines

General form:
     .PLOT PLTYPE OV1 [ (PLO1, PHI1) ] [ OV2  [ (PLO2, PHI2) ] ... OV8 ]

Examples:
     .PLOT DC V(4) V(5) V(1)
.PLOT TRAN V(17, 5) (2, 5) I(VIN) V(17) (1, 9)
.PLOT AC VM(5) VM(31, 24) VDB(5) VP(5)
.PLOT DISTO HD2 HD3(R) SIM2
.PLOT TRAN V(5, 3) V(4) (0, 5) V(7) (0, 10)


The PLOT line defines the contents of one plot of from one to eight output variables. PLTYPE is the type of analysis (DC, AC, TRAN, NOISE, or DISTO) for which the specified outputs are desired. The syntax for the OVI is identical to that for the .PRINT line and for the plot command in the interactive mode.

The overlap of two or more traces on any plot is indicated by the letter X.

When more than one output variable appears on the same plot, the first variable specified is printed as well as plotted. If a printout of all variables is desired, then a companion .PRINT line should be included.

There is no limit on the number of .PLOT lines specified for each type of analysis.

#### 4.4.4 .FOUR: Fourier Analysis of Transient Analysis Output

General form:

     .FOUR FREQ OV1 [ OV2 OV3 ... ]


Examples:

     .FOUR 100K  V(5)


The Four (or Fourier) line controls whether SPICE performs a Fourier analysis as a part of the transient analysis. FREQ is the fundamental frequency, and OV1 is the output vector for which results are desired. The Fourier analysis is performed over the interval <TSTOPperiod, TSTOP>, where TSTOP is the final time specified for the transient analysis, and period is one period of the fundamental frequency. The DC component and the first nine harmonics are determined. For maximum accuracy, TMAX (see the .TRAN line) should be set to no more than period/100.0 (or less for very high-Q circuits).

The variable nfreqs幸运飞艇超稳计划群 sets the number of frequencies computed by this analysis (default 10).