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xschem/xschem_library/examples/poweramp.sch

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do not duplicate empty strings as NULLs in hash tables
2023-10-09 12:49:11 +02:00
v {xschem version=3.4.4 file_version=1.2
*
* This file is part of XSCHEM,
* a schematic capture and Spice/Vhdl/Verilog netlisting tool for circuit
* simulation.
* Copyright (C) 1998-2023 Stefan Frederik Schippers
*
* This program is free software; you can redistribute it and/or modify
* it under the terms of the GNU General Public License as published by
* the Free Software Foundation; either version 2 of the License, or
* (at your option) any later version.
*
* This program is distributed in the hope that it will be useful,
* but WITHOUT ANY WARRANTY; without even the implied warranty of
* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
* GNU General Public License for more details.
*
* You should have received a copy of the GNU General Public License
* along with this program; if not, write to the Free Software
* Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
}
populating xschem git repo
2020-08-08 15:47:34 +02:00
G {}
small sample xschemrc fix
2020-10-06 21:59:23 +02:00
K {}
populating xschem git repo
2020-08-08 15:47:34 +02:00
V {}
S {}
E {}
L 18 845 -530 880 -530 {}
L 18 845 -530 845 -450 {}
L 18 845 -450 880 -450 {}
L 18 880 -450 900 -400 {}
L 18 900 -400 910 -400 {}
L 18 910 -580 910 -400 {}
L 18 900 -580 910 -580 {}
L 18 880 -530 900 -580 {}
L 18 880 -530 880 -450 {}
L 18 900 -580 900 -400 {}
optimize custom data plots and expression evaluation, added avg()
2022-02-12 13:20:24 +01:00
B 2 1200 -500 1880 -310 {flags=graph
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
y1 = -0.0059
y2 = 11
[experimental] add waveform display of ngspice simulation data directly in xschem drawing area
2021-12-22 04:39:23 +01:00
divy = 6
update poweramp.sch floater attributes(floater->name)
2023-05-19 09:28:17 +02:00
x1=0.00562909
x2=0.0165959
[experimental] add waveform display of ngspice simulation data directly in xschem drawing area
2021-12-22 04:39:23 +01:00
divx=10
Graph UI improvements. Persistent bold waves. Graph UI bug fixes
2022-01-28 04:44:07 +01:00
node="i(v.x1.vu)
i(v.x0.vu)
i(v.x1.vd)
i(v.x0.vd)"
Graph UI: example circuit updates
2022-01-28 05:32:12 +01:00
color="11 13 12 7"
set line buffering when stderr redirected to file
2023-01-20 18:25:43 +01:00
unitx=m
jpeg_quality=30}
optimize custom data plots and expression evaluation, added avg()
2022-02-12 13:20:24 +01:00
B 2 1200 -830 1880 -520 {flags=graph
better backannotation info placement in net labels, fixes in translate() for @spice_get_voltage and @spice_get_current, fixes in ngspice_backannotate routines.
2022-09-21 17:24:16 +02:00
y1 = -49
y2 = 58
fix wave panning if a non graph added, better error reporting in png writer function, better flags option names for special objejcts (image and graphs)
2022-01-21 02:16:51 +01:00
divy = 12
update poweramp.sch floater attributes(floater->name)
2023-05-19 09:28:17 +02:00
x1=0.00562909
x2=0.0165959
Better axis label placement, smooth waves move/zoom with mouse, compile option to store sim data as floats instead of doubles, option for axis scaling (p,n,u,m,k,M,G), load waveforms command is a toggle (load / free)
2021-12-24 12:17:00 +01:00
divx=10
Graph UI improvements. Persistent bold waves. Graph UI bug fixes
2022-01-28 04:44:07 +01:00
node="outp
outm
vpp
vnn
x1.vboost
x0.vboost"
Graph UI: example circuit updates
2022-01-28 05:32:12 +01:00
color="4 15 6 12 7 4"
set line buffering when stderr redirected to file
2023-01-20 18:25:43 +01:00
unitx=m
jpeg_quality=30}
optimize custom data plots and expression evaluation, added avg()
2022-02-12 13:20:24 +01:00
B 2 1200 -1020 1880 -830 {flags=graph
better backannotation info placement in net labels, fixes in translate() for @spice_get_voltage and @spice_get_current, fixes in ngspice_backannotate routines.
2022-09-21 17:24:16 +02:00
y1 = 0
y2 = 830
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
divy = 6
update poweramp.sch floater attributes(floater->name)
2023-05-19 09:28:17 +02:00
x1=0.00562909
x2=0.0165959
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
divx=10
unitx=m
color="4 7"
allow wave alias naming, fix off-by-one errors in plot_raw_custom_data() calls
2022-02-14 17:51:18 +01:00
node="\\"supply power;i(vcurrvnn) vnn * i(vcurrvpp) vpp * +\\"
set line buffering when stderr redirected to file
2023-01-20 18:25:43 +01:00
\\"running average supply power;i(vcurrvnn) vnn * i(vcurrvpp) vpp * + 200u ravg()\\""
jpeg_quality=30}
allow wave alias naming, fix off-by-one errors in plot_raw_custom_data() calls
2022-02-14 17:51:18 +01:00
B 2 1200 -310 1880 -120 {flags=graph
better backannotation info placement in net labels, fixes in translate() for @spice_get_voltage and @spice_get_current, fixes in ngspice_backannotate routines.
2022-09-21 17:24:16 +02:00
y1 = 0
y2 = 840
optimize custom data plots and expression evaluation, added avg()
2022-02-12 13:20:24 +01:00
divy = 6
update poweramp.sch floater attributes(floater->name)
2023-05-19 09:28:17 +02:00
x1=0.00562909
x2=0.0165959
optimize custom data plots and expression evaluation, added avg()
2022-02-12 13:20:24 +01:00
divx=10
unitx=m
color="4 7"
allow wave alias naming, fix off-by-one errors in plot_raw_custom_data() calls
2022-02-14 17:51:18 +01:00
node="\\"Load power;outm outp - i(v.x1.v8) *\\"
set line buffering when stderr redirected to file
2023-01-20 18:25:43 +01:00
\\"Running Average Load power;outm outp - i(v.x1.v8) * 200u ravg()\\""
jpeg_quality=30}
example schematics formatting
2022-02-16 01:08:16 +01:00
B 2 1740 -1110 1877 -1050 {flags=image
alpha=0.6
set line buffering when stderr redirected to file
2023-01-20 18:25:43 +01:00
image_data=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
ps_invert=true
jpeg_quality=30}
fix find_closest_dataset() if log scale axes are used
2022-09-13 13:39:25 +02:00
B 2 1570 -1107.5 1708 -1045 {flags=image
alpha=0.6
image=/home/schippes/x/xyce.png
set line buffering when stderr redirected to file
2023-01-20 18:25:43 +01:00
image_data=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
ps_invert=true
jpeg_quality=30}
populating xschem git repo
2020-08-08 15:47:34 +02:00
T {actual value
small sample xschemrc fix
2020-10-06 21:59:23 +02:00
50u} 400 -820 0 0 0.4 0.4 {}
populating xschem git repo
2020-08-08 15:47:34 +02:00
T {actual value
small sample xschemrc fix
2020-10-06 21:59:23 +02:00
50u} 400 -360 0 0 0.4 0.4 {}
populating xschem git repo
2020-08-08 15:47:34 +02:00
T {actual value
50u} 50 -750 0 0 0.4 0.4 {}
T {actual value
50u} 80 -290 0 0 0.4 0.4 {}
T {actual value
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
200} 860 -1280 0 0 0.4 0.4 {}
[experimental] add waveform display of ngspice simulation data directly in xschem drawing area
2021-12-22 04:39:23 +01:00
T {Select one or more graphs (and no other objects)
optimize custom data plots and expression evaluation, added avg()
2022-02-12 13:20:24 +01:00
and use arrow keys to zoom / pan waveforms} 1110 -1120 0 0 0.3 0.3 {}
clear text member `floater_ptr` when text is changed to force cache update
2023-05-14 02:45:56 +02:00
T {@spice_get_voltage} 761.875 -786.09375 0 0 0.8 0.8 {layer=15
(2) update poweramp.sch floater attributes(floater->name)
2023-05-19 09:36:02 +02:00
name=p9}
clear text member `floater_ptr` when text is changed to force cache update
2023-05-14 02:45:56 +02:00
T {@spice_get_voltage} 761.875 -206.09375 0 0 0.8 0.8 {layer=15
update poweramp.sch floater attributes(floater->name)
2023-05-19 09:28:17 +02:00
name=p14}
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
N 70 -1220 70 -1200 {lab=#net1}
N 70 -1080 70 -1060 {lab=#net2}
populating xschem git repo
2020-08-08 15:47:34 +02:00
N 710 -700 860 -700 {lab=OUTM}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
N 500 -1150 570 -1150 {lab=VSS}
N 570 -1150 570 -1140 {lab=VSS}
N 570 -1140 610 -1140 {lab=VSS}
N 540 -1190 570 -1190 {lab=IN}
N 610 -1200 700 -1200 {lab=REFP}
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
N 260 -1070 260 -1060 {lab=VNN}
N 260 -1140 260 -1130 {lab=VSS}
N 70 -1060 100 -1060 {lab=#net2}
N 70 -1220 100 -1220 {lab=#net1}
N 260 -1140 270 -1140 {lab=VSS}
N 240 -1220 270 -1220 {lab=VPP}
N 240 -1060 260 -1060 {lab=VNN}
N 240 -1140 260 -1140 {lab=VSS}
populating xschem git repo
2020-08-08 15:47:34 +02:00
N 550 -950 710 -950 {lab=OUTM}
N 400 -890 550 -890 {lab=FBN}
N 550 -770 550 -750 {lab=IN}
N 350 -890 350 -700 {lab=FBN}
N 710 -950 710 -700 {lab=OUTM}
N 710 -240 860 -240 {lab=OUTP}
N 260 -220 350 -220 {lab=INX}
N 550 -490 710 -490 {lab=OUTP}
N 400 -430 550 -430 {lab=FB}
N 350 -430 350 -240 {lab=FB}
N 710 -490 710 -240 {lab=OUTP}
exampels/poweramp.sch and examples/cmos_example.sch show how to use dynamuc ngspice simulation data backannotation, optimized fix of previous bbox bug
2020-10-20 19:48:59 +02:00
N 240 -400 240 -380 {lab=VPP}
populating xschem git repo
2020-08-08 15:47:34 +02:00
N 260 -220 260 -190 {lab=INX}
N 260 -130 260 -110 {lab=VSS}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
N 500 -1070 570 -1070 {lab=VSS}
N 540 -1110 570 -1110 {lab=IN}
N 610 -1120 700 -1120 {lab=REFM}
populating xschem git repo
2020-08-08 15:47:34 +02:00
N 200 -220 240 -220 {lab=INX}
N 550 -310 550 -290 {lab=VSS}
N 650 -700 710 -700 {lab=OUTM}
N 650 -240 710 -240 {lab=OUTP}
N 240 -220 260 -220 {lab=INX}
N 260 -680 350 -680 {lab=VSSX}
exampels/poweramp.sch and examples/cmos_example.sch show how to use dynamuc ngspice simulation data backannotation, optimized fix of previous bbox bug
2020-10-20 19:48:59 +02:00
N 240 -860 240 -840 {lab=VPP}
populating xschem git repo
2020-08-08 15:47:34 +02:00
N 260 -680 260 -650 {lab=VSSX}
N 260 -590 260 -570 {lab=VSS}
N 240 -680 260 -680 {lab=VSSX}
N 180 -680 240 -680 {lab=VSSX}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
N 870 -1200 890 -1200 {lab=IN_INT}
N 870 -1200 870 -1170 {lab=IN_INT}
populating xschem git repo
2020-08-08 15:47:34 +02:00
N 400 -1000 400 -980 {lab=VPP}
N 400 -540 400 -520 {lab=VPP}
N 860 -700 860 -520 {lab=OUTM}
N 860 -460 860 -240 {lab=OUTP}
N 350 -890 400 -890 {lab=FBN}
N 350 -430 400 -430 {lab=FB}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
N 570 -1060 610 -1060 {lab=VSS}
N 570 -1070 570 -1060 {lab=VSS}
added attributes spice_ignore=short, verilog_ignore=short, .... that will transform the instance into a short in the current netlisting mode, shorting all pins to the same net. Works similarly as lvs_ignore=short, but does not need lvs_ignore global setting
2023-06-07 03:41:49 +02:00
N 270 -1220 310 -1220 {lab=VPP}
N 260 -1060 310 -1060 {lab=VNN}
N 270 -1140 310 -1140 {lab=VSS}
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
N 270 -1150 270 -1140 { lab=VSS}
N 270 -1220 270 -1210 { lab=VPP}
added attributes spice_ignore=short, verilog_ignore=short, .... that will transform the instance into a short in the current netlisting mode, shorting all pins to the same net. Works similarly as lvs_ignore=short, but does not need lvs_ignore global setting
2023-06-07 03:41:49 +02:00
N 400 -920 400 -890 { lab=FBN}
N 400 -460 400 -430 { lab=FB}
N 240 -780 240 -680 { lab=VSSX}
N 240 -320 240 -220 { lab=INX}
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
N 160 -1220 180 -1220 {lab=#net3}
N 160 -1060 180 -1060 {lab=#net4}
N 70 -1140 180 -1140 {lab=#net5}
C {vsource.sym} 70 -1170 0 0 {name=V1 value="dc 50 pwl 0 0 1m 50"}
C {vsource.sym} 70 -1110 0 0 {name=V0 value="dc 50 pwl 0 0 1m 50"}
C {lab_pin.sym} 310 -1220 0 1 {name=p5 lab=VPP}
C {lab_pin.sym} 310 -1060 0 1 {name=p6 lab=VNN}
C {lab_pin.sym} 310 -1140 0 1 {name=p3 lab=VSS}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {lab_pin.sym} 860 -240 0 1 {name=p14 lab=OUTP}
C {res.sym} 860 -490 0 1 {name=R1 m=1 value=8}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {lab_pin.sym} 500 -1150 0 0 {name=p26 lab=VSS}
C {lab_pin.sym} 540 -1190 0 0 {name=p31 lab=IN}
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
C {vcvs.sym} 610 -1170 0 0 {name=E3 value=\{gain*0.99\}}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {lab_pin.sym} 700 -1200 0 1 {name=p32 lab=REFP}
C {capa.sym} 260 -1100 0 0 {name=C3 m=1 value="100u"}
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
C {res.sym} 130 -1220 1 1 {name=R11 m=1 value=0.3}
C {res.sym} 130 -1060 1 1 {name=R9 m=1 value=0.3}
revert pro floaters. black hole, wrong approach
2022-02-22 12:09:04 +01:00
C {res.sym} 550 -920 0 1 {name=R19 m=1 value='100k'
}
hide_texts=true attribute added on instance will avoid the display of all symbol texts (will be probably used when using floater symbol texts)
2023-05-12 12:09:20 +02:00
C {res.sym} 550 -860 0 1 {name=R0 m=1 value="'100k/gain'"}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {lab_pin.sym} 550 -750 0 0 {name=p108 lab=IN}
C {mos_power_ampli.sym} 500 -660 0 0 {name=x1}
C {lab_pin.sym} 350 -640 0 0 {name=p2 lab=VPP}
C {lab_pin.sym} 350 -620 0 0 {name=p4 lab=VNN}
C {lab_pin.sym} 860 -700 0 1 {name=p9 lab=OUTM}
C {mos_power_ampli.sym} 500 -200 0 0 {name=x0}
C {lab_pin.sym} 350 -180 0 0 {name=p12 lab=VPP}
C {lab_pin.sym} 350 -160 0 0 {name=p13 lab=VNN}
exampels/poweramp.sch and examples/cmos_example.sch show how to use dynamuc ngspice simulation data backannotation, optimized fix of previous bbox bug
2020-10-20 19:48:59 +02:00
C {res.sym} 240 -350 0 1 {name=R6 m=1 value=100k}
C {lab_pin.sym} 240 -400 0 0 {name=p7 lab=VPP}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {res.sym} 260 -160 0 1 {name=R7 m=1 value=100k}
C {lab_pin.sym} 260 -110 0 0 {name=p15 lab=VSS}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {lab_pin.sym} 500 -1070 0 0 {name=p20 lab=VSS}
C {lab_pin.sym} 540 -1110 0 0 {name=p21 lab=IN}
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
C {vcvs.sym} 610 -1090 0 0 {name=E0 value=\{-gain*0.99\}}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {lab_pin.sym} 700 -1120 0 1 {name=p23 lab=REFM}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {lab_pin.sym} 240 -250 0 0 {name=p8 lab=INX}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {lab_pin.sym} 870 -1050 0 0 {name=p126 lab=VSS}
C {lab_pin.sym} 950 -1200 0 1 {name=p127 lab=IN}
ngspice_backannotate.tcl: handle Xyce operating point data, removed hspice_netlist (no more existent)
2022-09-13 12:01:58 +02:00
C {capa.sym} 550 -800 0 0 {name=C5 m=1 value="100n ; ic=0"}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {lab_pin.sym} 550 -290 0 0 {name=p11 lab=VSS}
ngspice_backannotate.tcl: handle Xyce operating point data, removed hspice_netlist (no more existent)
2022-09-13 12:01:58 +02:00
C {capa.sym} 550 -340 0 0 {name=C6 m=1 value="100n ; ic=0"}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {lab_pin.sym} 350 -200 0 0 {name=p28 lab=VSS}
C {lab_pin.sym} 350 -660 0 0 {name=p1 lab=VSS}
C {res.sym} 550 -460 0 1 {name=R2 m=1 value='100k'}
C {res.sym} 550 -400 0 1 {name=R3 m=1 value="'100k/(gain-2)'"}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {vsource.sym} 870 -1140 0 0 {name=V3
exampels/poweramp.sch and examples/cmos_example.sch show how to use dynamuc ngspice simulation data backannotation, optimized fix of previous bbox bug
2020-10-20 19:48:59 +02:00
xvalue="dc 0 pulse -.1 .1 1m .1u .1u 10.1u 20u"
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
value="dc 0 sin 0 1 \{frequ\} 1m"
populating xschem git repo
2020-08-08 15:47:34 +02:00
}
exampels/poweramp.sch and examples/cmos_example.sch show how to use dynamuc ngspice simulation data backannotation, optimized fix of previous bbox bug
2020-10-20 19:48:59 +02:00
C {res.sym} 240 -810 0 1 {name=R4 m=1 value=100k}
C {lab_pin.sym} 240 -860 0 0 {name=p18 lab=VPP}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {res.sym} 260 -620 0 1 {name=R5 m=1 value=100k}
C {lab_pin.sym} 260 -570 0 0 {name=p10 lab=VSS}
C {res.sym} 400 -950 0 1 {name=R8 m=1 value=100k}
ngspice_backannotate.tcl: handle Xyce operating point data, removed hspice_netlist (no more existent)
2022-09-13 12:01:58 +02:00
C {capa.sym} 170 -220 1 0 {name=C4 m=1 value="100n ; ic=0"}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {lab_pin.sym} 140 -220 0 0 {name=p0 lab=IN}
ngspice_backannotate.tcl: handle Xyce operating point data, removed hspice_netlist (no more existent)
2022-09-13 12:01:58 +02:00
C {capa.sym} 150 -680 1 0 {name=C1 m=1 value="100n ; ic=0"}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {lab_pin.sym} 120 -680 0 0 {name=p17 lab=VSS}
C {lab_pin.sym} 240 -710 0 0 {name=p22 lab=VSSX}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {res.sym} 920 -1200 1 1 {name=R10 m=1 value=2}
populating xschem git repo
2020-08-08 15:47:34 +02:00
C {lab_pin.sym} 400 -1000 0 0 {name=p24 lab=VPP}
C {res.sym} 400 -490 0 1 {name=R13 m=1 value=100k}
C {lab_pin.sym} 400 -540 0 0 {name=p16 lab=VPP}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {vsource.sym} 870 -1080 0 0 {name=Vin value=0 xvalue="pwl 0 .1 1m .1 1.01m 0"
populating xschem git repo
2020-08-08 15:47:34 +02:00
}
C {lab_pin.sym} 350 -270 0 0 {name=p19 lab=FB}
C {lab_pin.sym} 350 -730 0 0 {name=p25 lab=FBN}
C {title.sym} 160 -30 0 0 {name=l2 author="Stefan Schippers"}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {lab_pin.sym} 870 -1200 0 0 {name=p27 lab=IN_INT}
add backannotation info (as hidden text) in lab_pin.sym, lab_wire.sym, transitioning example schematics from old (push) backannotation model to new pull model.
2022-09-19 11:22:04 +02:00
C {ammeter.sym} 210 -1220 3 0 {name=vcurrvpp net_name=true }
C {ammeter.sym} 210 -1060 3 0 {name=vcurrvnn net_name=true }
C {ammeter.sym} 210 -1140 3 0 {name=vcurrvss net_name=true }
if floaters are used to display simulation data (@spice_get_voltage) force update on floater text caches on `b` cursor move
2023-05-14 02:22:18 +02:00
C {launcher.sym} 710 -70 0 0 {name=h2
spice_probe_dynamic.sym added to devices, retrieves node voltages with a pull method, so always updated, "@@pin" syntax in translate(), same as in format string for netlisting,print hilight nodes (ctrl-alt-j) will print .save instructions if netlist mode set to spice
2020-10-20 01:05:40 +02:00
descr="Ctrl-Click
Clear all probes"
tclcommand="
xschem push_undo
xschem set no_undo 1
xschem set no_draw 1
set lastinst [xschem get instances]
for \{ set i 0 \} \{ $i < $lastinst \} \{incr i \} \{
set type [xschem getprop instance $i cell::type]
if \{ [regexp \{(^|/)probe$\} $type ] \} \{
xschem setprop $i voltage fast
\}
if \{ [regexp \{current_probe$\} $type ] \} \{
xschem setprop $i current fast
\}
if \{ [regexp \{differential_probe$\} $type ] \} \{
xschem setprop $i voltage fast
\}
\}
xschem set no_undo 0
xschem set no_draw 0
xschem redraw
"
}
fixes and comments in annotation schematic examples
2020-12-29 23:17:00 +01:00
C {capa.sym} 270 -1180 0 0 {name=C2 m=1 value="100u"}
correct size calculation when inserting new unscaled image
2022-01-25 00:52:49 +01:00
C {ngspice_get_expr.sym} 535 -475 0 1 {name=r18
exampels/poweramp.sch and examples/cmos_example.sch show how to use dynamuc ngspice simulation data backannotation, optimized fix of previous bbox bug
2020-10-20 19:48:59 +02:00
node="[ngspice::get_current \{r2[i]\}]"
descr = current
}
add backannotation info (as hidden text) in lab_pin.sym, lab_wire.sym, transitioning example schematics from old (push) backannotation model to new pull model.
2022-09-19 11:22:04 +02:00
C {ngspice_get_expr.sym} 585 -895 0 0 {name=r1
exampels/poweramp.sch and examples/cmos_example.sch show how to use dynamuc ngspice simulation data backannotation, optimized fix of previous bbox bug
2020-10-20 19:48:59 +02:00
node="[ngspice::get_current \{r19[i]\}]"
descr = current
}
update poweramp.sch, remove obsolete comments
2023-04-18 00:35:23 +02:00
C {ngspice_get_expr.sym} 830 -480 2 0 {name=r29
better backannotation info placement in net labels, fixes in translate() for @spice_get_voltage and @spice_get_current, fixes in ngspice_backannotate routines.
2022-09-21 17:24:16 +02:00
node="[format %.4g [expr \{([ngspice::get_voltage outm] - [ngspice::get_voltage outp]) * [ngspice::get_current \{r1[i]\}]\}]] "
exampels/poweramp.sch and examples/cmos_example.sch show how to use dynamuc ngspice simulation data backannotation, optimized fix of previous bbox bug
2020-10-20 19:48:59 +02:00
descr = power
}
if floaters are used to display simulation data (@spice_get_voltage) force update on floater text caches on `b` cursor move
2023-05-14 02:22:18 +02:00
C {launcher.sym} 710 -120 0 0 {name=h3
synchronize command sending to gaw with gaw replies so at the end the tcp channel is closed gracefully (avoid port in use error messages). Timeout whatchdog is set to prevent forever waits/deadlocks.
2020-11-07 21:07:16 +01:00
descr="Load file into gaw"
comment="
This launcher gets raw filename from current schematic using 'xschem get schname'
and stripping off path and suffix. It then loads raw file into gaw.
This allow to use it in any schematic without changes.
"
tclcommand="
set rawfile [file tail [file rootname [xschem get schname]]].raw
gaw_cmd \\"tabledel $rawfile
load $netlist_dir/$rawfile
table_set $rawfile\\"
unset rawfile"
}
add backannotation info (as hidden text) in lab_pin.sym, lab_wire.sym, transitioning example schematics from old (push) backannotation model to new pull model.
2022-09-19 11:22:04 +02:00
C {spice_probe.sym} 710 -860 0 0 {name=p40 analysis=tran }
C {spice_probe.sym} 710 -400 0 0 {name=p41 analysis=tran }
C {spice_probe.sym} 660 -1200 0 0 {name=p42 analysis=tran }
C {spice_probe.sym} 670 -1120 0 0 {name=p43 analysis=tran }
C {spice_probe.sym} 950 -1200 0 0 {name=p44 analysis=tran }
update examples and ngspice_get_value.sym (@descr attribute)
2020-12-28 23:18:13 +01:00
C {launcher.sym} 1000 -270 0 0 {name=h1
ngspice_backannotate.tcl: handle Xyce operating point data, removed hspice_netlist (no more existent)
2022-09-13 12:01:58 +02:00
descr="Backannotate"
update poweramp.sch, remove obsolete comments
2023-04-18 00:35:23 +02:00
tclcommand="xschem annotate_op $netlist_dir/poweramp_op.raw"}
rpn expressions in graphs
2022-02-12 04:55:02 +01:00
C {ngspice_get_expr.sym} 130 -1010 0 0 {name=r19
fix make_sym.awk duplicating name= attribute in generated symbol
2020-12-29 15:41:15 +01:00
node="[ngspice::get_current \{r9[i]\}]"
descr = current
}
add backannotation info (as hidden text) in lab_pin.sym, lab_wire.sym, transitioning example schematics from old (push) backannotation model to new pull model.
2022-09-19 11:22:04 +02:00
C {spice_probe.sym} 300 -1220 0 0 {name=p45 analysis=tran }
C {spice_probe.sym} 300 -1060 0 0 {name=p46 analysis=tran }
optimize custom data plots and expression evaluation, added avg()
2022-02-12 13:20:24 +01:00
C {launcher.sym} 1145 -1165 0 0 {name=h5
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
descr="load ngspice waves"
handle spice simulation files with multiple datasets
2021-12-25 05:15:52 +01:00
tclcommand="
xschem raw_read accepts an optional type argument after file name (tran, ac, dc, op, ...) to select type of simulation to load from raw file. New command xschem annotate_op will replace ngspice::annotate tcl procedure.
2022-09-20 16:49:42 +02:00
xschem raw_read $netlist_dir/poweramp.raw tran
handle spice simulation files with multiple datasets
2021-12-25 05:15:52 +01:00
"
}
optimize custom data plots and expression evaluation, added avg()
2022-02-12 13:20:24 +01:00
C {launcher.sym} 1450 -30 0 0 {name=h6
xyce quircks/integration for ac analysis, refuse to stretch unscalable images, more example schematics
2022-02-03 00:40:59 +01:00
descr="Graph Manual page"
url="https://xschem.sourceforge.io/stefan/xschem_man/graphs.html"}
update poweramp.sch floater attributes(floater->name)
2023-05-19 09:28:17 +02:00
C {simulator_commands.sym} 1020 -450 0 0 {name=COMMANDS
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
simulator=ngspice
only_toplevel=false
value="
.option ITL4=20000 ITL5=0
vvss vss 0 dc 0
.temp 30
.param frequ=5k
.param gain=45
.option savecurrents
** models are generally not free: you must download
** SPICE models for active devices and put them into the below
** referenced file in simulation directory.
.include \\"models_poweramp.txt\\"
.control
save all
op
tclpropeval2(): hierarchy separator replacement for Xyce no more necessary
2022-09-13 00:53:47 +02:00
write poweramp_op.raw
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
tran 8e-7 0.07 uic
* .FOUR 20k v(outm,outp)
* .probe i(*)
plot outp outm
save p(r*) p(v*)
write poweramp.raw
.endc
"}
update poweramp.sch floater attributes(floater->name)
2023-05-19 09:28:17 +02:00
C {simulator_commands.sym} 1020 -650 0 0 {name=COMMANDS1
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
simulator=xyce
only_toplevel=false
value="
.option ITL4=20000 ITL5=0
vvss vss 0 dc 0
.temp 30
.param frequ=5k
.param gain=45
** models are generally not free: you must download
** SPICE models for active devices and put them into the below
** referenced file in simulation directory.
.include \\"models_poweramp.txt\\"
.tran 8e-7 0.07 uic
ngspice_backannotate.tcl: handle Xyce operating point data, removed hspice_netlist (no more existent)
2022-09-13 12:01:58 +02:00
* .op
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
.print tran format=raw file=poweramp_xyce.raw v(*) i(*)
+ v(x1:*) v(x0:*) i(x1:*) i(x0:*)
ngspice_backannotate.tcl: handle Xyce operating point data, removed hspice_netlist (no more existent)
2022-09-13 12:01:58 +02:00
* .print dc format=raw file=poweramp_op.raw v(*) i(*) v(x1:*) v(x0:*) i(x1:*) i(x0:*)
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
"}
C {launcher.sym} 1495 -1165 0 0 {name=h7
descr="load Xyce waves"
tclcommand="
xschem raw_read accepts an optional type argument after file name (tran, ac, dc, op, ...) to select type of simulation to load from raw file. New command xschem annotate_op will replace ngspice::annotate tcl procedure.
2022-09-20 16:49:42 +02:00
xschem raw_read $netlist_dir/poweramp_xyce.raw tran
ask confirmation if pressing "s" for simulate; node lists in graph dialog box are returned as they are with no tcleval() resolution; poweramp.sch now can be simulated unchanged with Xyce
2022-09-13 00:31:20 +02:00
"
}