File format translation

We need a universal translator system that can translate in all directions between Free EDA tools, possible future free EDA tools, and outside tools that are likely to be used with free EDA tools.

Of course, everything to everything is not reasonable. So, set a limit of circuit oriented free EDA tools, possible future tools, and outside tools that are likely to be used them. Of course, tool formats where translation doesn't make sense don't need to be supported.

Most tools use a format much like a netlist, often with some special information. So, use a netlist based intermediate format. First translate to the intermediate format, then translate out. The intermediate format should be sufficiently expressive that there can be a lossless round trip from the tool format to the intermediate format and back.

Lossless means that the resultant file is equivalent in how it works. It is not necessary to preserve formatting and other things that don't matter.

All of the formats needing translation presently consist of lists of objects, with some kind of encapsulation. Each object has connections and attributes.

This suggests the possible of a standard netlist format as the intermediate format.

Further discussion related only to formats that fit this model.

If possible, the format chosen should have a history of use for at least part of this, and have a published specification that is externally controlled and freely available.

There needs to be a way to merge changes from any target/source without messing up other parts.

• schematic
• layout
• simulation

Lossless round trip is required, so archival storage can use the intermediate format.

• gschem
• pcb
• gnucap
• Icarus Verilog
• NGspice
• Qucs
• Kicad
• Magic
• Electric
• Xcircuit
• Fritzing

Support for these will allow gEDA tools to play nice with the commercial world. Basic functionality is needed, but it doesn't need to be lossless. Lossless should be possible, but it is not a high priority to actually implement it.

• Eagle
• Orcad
• LTspice
• Pads

Hopefully having a translator system will provide a seed so these can be done.

• Back annotation from layout or simulation to schematic
• Static timing analysis
• Post-layout signal integrity simulation.
• Layout - schematic comparison
• Use of the same schematic for the whole project.

• Plotting
• Commands
• Behavioral modeling
• Translating the symbols or footprints themselves.

All of these consist of lists of objects, with connections and attributes.

It is tradition that a netlist is used for interchange, but the traditional approach only goes one way, because information is lost in the translation.

The format must convey the meaning, not necessarily in the same way as the tool's native format or internal storage.

It is not necessary to translate parts that are usually in libraries, and are tool specific, such as models, symbols, or footprints.

All contenders for possible formats must support a lossless round-trip to any other.

A popular netlist format. It has a history of use for interchange, but not yet for physical placement. Problems: irregular syntax, not sufficiently expressive. These problems have been a major hassle for years for developers. It is well accepted, but not by people who know it well.

The structural subset is a good netlist format. It is regular, sufficiently expressive, and has a published standard. It has a history of use for interchange, but not yet for physical placement.

The structural subset is a good netlist format. It is regular, sufficiently expressive, and has a published standard. It has a history of use for interchange, but not yet for physical placement.

The structural subset is a good netlist format. It is regular, sufficiently expressive, but belongs to one company (Cadence), so rule it out. It has a history of use for simulation only.

XML is not really a format but a syntax. A good format can easily be made based on XML, but has no history of use in a similar context. The syntax is well documented but there is no outside documentation of application in any related use.

This part is the only part where there is not a strong history of use for VHDL and Verilog.

Ideas:

• Parameters are not the same as attributes. Parameters are electrical parameters. Attributes are part of the markup.
• Parameters can have attributes.
• Nets are also objects with connections, parameters, and attributes. Nets have meaning in all contexts.
• A place on a schematic can be considered to be an object, with connections and attributes.
• Pads, connectors, thermals, vias .. are also objects, with connections and attributes.
• Use `define (assuming Verilog format) to set aside sections that have meaning in one context but not another.
• This is a high level description. Take a high level view across all. It's not lines, boxes, and circles.
• If you must, lines, boxes, and circles can be objects too, but not translatable because they have no meaning in other contexts.
• Attributes that have no meaning are silently ignored. Attributes that have meaning in one context but not in another context are ignored where they have no meaning.

Choosing the Verilog format as one possibility.

The unit of encapsulation is the “module”:

module my-module(connections);
// contents
endmodule

Each object in the list has a consistent syntax:

type #(parameters) name (connections);

Example:

Here is a simple circuit, plain Verilog, no placement yet.

module amp (a, c);
  resistor #(.r(1k)) r1 (.p(a), .n(b));
  resistor #(.r(1k)) r2 (.p(b), .n(c));
  opamp741 #(.gain(100k)) u1 (.p(c), .n(0), .ps(0), .pn(b));
endmodule

Looking at it one line at a time:

module amp (a, c);

A “module” is the unit of encapsulation. This one is called “amp”, and it has two connections to outside, “a” and “c”.

resistor #(.r(1k)) r1 (.p(a), .n(b));

This line instantiates a “resistor”. It could be a symbol, a device, a footprint, depending on the application.

The ”#” introduces a parameter list. “r” is the name of a parameter. “1k” is the value (a string).

“r1” is the instance name,

It has two pins, named “p” and “n'. Node “b” connects to pin “p” and node “c” connects to pin “n”.

The type (“resistor”) refers to a model in simulation. In layout or schematic, it would refer to a footprint, indirectly.

In simulation, the models often come from some place external, or might come with the simulator. You might substitute different models for the same device, depending what you want to do.

In layout or schematic, the footprints and symbols are not conveyed by this file, and might be changed in a transfer, like you would change a font in a text document. This provides a mechanism for making changes like from through-hole to surface mount parts.

In the above example, both connect to node b directly. In a schematic or layout representation the connection would not be direct, but through a “net”.

module amp (.a(a0), .c(c0));
  resistor #(.r(1k)) r1 (.p(a1), .n(b1));
  resistor #(.r(1k)) r2 (.p(b2), .n(c2));
  opamp741 #(.gain(100k)) u1 (.p(c3), .n(0), .ps(0), .pn(b3));

  net a (a0, a1);
  net b (b1, b2, b3);
  net c (c0, c2, c3);
endmodule

We have replaced the nodes with nets, which are now first class objects. This will give us a way to represent the interconnect in a schematic drawing or a layout. It also provides essential data to support analysis and simulation of the interconnect.

Looking at net “b” as an example, it has 3 connections : r1 pin n, p2 pin p, and u1 pin pn.

The Verilog standard defines some “system” parameters for all devices to show position.

• $xposition (x coordinate, in meters)
• $yposition (y coordinate, in meters)
• $angle (rotation, in degrees)
• $hflip (flag: flip horizontally, +1=no flip, -1=flip)
• $vflip (flag: flip vertically, +1=no flip, -1=flip)

These “system” parameters are real parameters, so we won't use them here. We will use them as inspiration for “attributes” instead.

The Verilog standard gives a way to add “attributes” to just about anything.

(* attribute = value *) resistor r1 (.p(2), .n(3));

We will use a special prefix for the attribute names, so the various uses can coexist. The prefix will be one or two upper case letters, a single digit [0..9], and an underscore. The digit is a selector, allowing several different markups in the same file. This prefix list can be extended for other uses.

We add a third dimension “z”, and a third flip “zflip”. We shorten xposition to x, yposition to y, and add a number to have multiple positions. The “z” may indicate a layer name instead of a dimension, depending on the application.

Now we use the attributes to specify the location. We need to locate the various objects. In most cases, we need to specify some point of every object that will identify its location. Some programs use some notion of a “center”, which is ambiguous. We will use the electrical connection points, often called “pins”, as the location points for things that have an electrical connection. For objects that do not have electrical connections, reference points can be used.

We will number the pins, by position, 0, 1, 2, … Then we use x0,y0, and so on to locate them. Usually one of them is adequate to locate an object. The others can “float”, allowing the actual location to be determined by the surroundings. It is permissible to overspecify locations, provided they are self-consistent, and consistent with connections.

In addition to the positions, hflip, vflip, and angle are supported. If there is both a flip and an angle, flip will be done first, then angle.

Another attribute named for the specific tool (example: S0_geda) can be used to stash tool specific data that doesn't fit otherwise. This is intended to assist with a translation from this format back to the tool format. Normally, this would be a string containing a composite of the info (S0_geda=“5 10 0 0 0 0 1”) If more than one string in a scope is needed, suffixes can be used. (S0_geda_color=“blue” S0_geda_symbol=“resistor-1.sym”) These are stored and passed on without any interpretation.

module amp (.a(a0), .c(c0));
  (* S0_x0=-5m, S0_y0=0m *)  input a0;
  (* S0_x0=30m, S0_y0=-3m *) output c0;
                             ground g0;
                             ground g1;

  (* S0_x0=0m,  S0_y0=0m *)  resistor #(.r(1k))      r1 (.p(a1), .n(b1));
  (* S0_x0=24m, S0_y0=7m *)  resistor #(.r(1k))      r2 (.p(b2), .n(c2));
  (* S0_x0=25m, S0_y0=-3m *) opamp741 #(.gain(100k)) u1 (.p(c3), .n(g1), .ps(g0), .ns(b3));

  net a (a0, a1);
  net b (b1, b2, b3);
  net c (c0, c2, c3);
endmodule

• This is a schematic, using a 1 mm grid.
• The lines “input” and “output” are pins, explicitly located.
• The lines “resistor” and “opamp741” are components, explicitly located by pin 0 of each, all called “p” here, by coincidence.
• The lines “ground” are the ground symbol. The first is node “g0”, which is the “ps” pin (”+” input, pin 2) of “u1”, so it is implicitly located there. The other is node “g1”, which is the “n” pin (pin 1) of “u1”, so this one is also implicitly located. An explicit location could have been specified, but is not necessary because it can be determined by the symbol for “u1”.
• The location of other nodes will follow based on the symbol or footprint geometry.
• It is ok to leave some, or even most, unspecified, so they will be located by context.
• It is ok to locate a node more than once, provided the locations are the same.
• If locations of the same node are not the same, the tool shall issue a warning, and make a correction to assure connectivity is correct.
• Locating one pin of a footprint or symbol determines the location of the symbol or footprint.
• In the above example, the I/O pins and components have been explicitly located.
• The nets have been implicitly located.
• The nodes b1 and c2 are implicitly located by the resistor symbol for r1 and r2.

The choice of which nodes to locate could have been different. The following example produces exactly the same result.

module amp (.a(a0), .c(c0));
  input a0;
  output c0;
  ground g0;
  ground g1;

  resistor #(.r(1k))      r1 (.p(a1), .n(b1));
  resistor #(.r(1k))      r2 (.p(b2), .n(c2));
  opamp741 #(.gain(100k)) u1 (.p(c3), .n(g1), .ps(g0), .ns(b3));

  (* S0_x0=-5m, S0_y0=0m,  S0_x1=0m,  S0_y1=0m *)  net a (a0, a1);
  (* S0_x1=24m, S0_y1=7m *)                        net b (b1, b2, b3);
  (* S0_x0=30m, S0_y0=-3m, S0_x2=25m, S0_y2=-3m *) net c (c0, c2, c3);
endmodule

The following example is overdetermined, but legal, and produces the same result.

module amp (.a(a0), .c(c0));
  (* S0_x0=-5m, S0_y0=0m *)  input a0;
  (* S0_x0=30m, S0_y0=-3m *) output c0;
                             ground g0;
                             ground g1;

  (* S0_x0=0m,  S0_y0=0m *)  resistor #(.r(1k))      r1 (.p(a1), .n(b1));
  (* S0_x0=24m, S0_y0=7m *)  resistor #(.r(1k))      r2 (.p(b2), .n(c2));
  (* S0_x0=25m, S0_y0=-3m *) opamp741 #(.gain(100k)) u1 (.p(c3), .n(g1), .ps(g0), .ns(b3));

  (* S0_x0=-5m, S0_y0=0m,  S0_x1=0m,  S0_y1=0m *)  net a (a0, a1);
  (* S0_x1=24m, S0_y1=7m *)                        net b (b1, b2, b3);
  (* S0_x0=30m, S0_y0=-3m, S0_x2=25m, S0_y2=-3m *) net c (c0, c2, c3);
endmodule

Files can be combined.

module amp (.a(a0), .c(c0));
  input a0;
  output c0;

  resistor #(.r(1k))      r1 (.p(a1), .n(b1));
  resistor #(.r(1k))      r2 (.p(b2), .n(c2));
  opamp741 #(.gain(100k)) u1 (.p(c3), .n(0), .ps(0), .ns(b3));

  (* S0_x0=-5m, S0_y0=0m,  S0_x1=0m,  S0_y1=0m,  PC0_x0=-5m, PC0_y0=0m,  PC0_x1=0m,  PC0_y1=0m *)  net a (a0, a1);
  (* S0_x1=24m, S0_y1=7m *)                   (* PC0_x1=24m, PC0_y1=7m *)                          net b (b1, b2, b3);
  (* S0_x0=30m, S0_y0=-3m, S0_x2=25m, S0_y2=-3m, PC0_x0=30m, PC0_y0=-3m, PC0_x2=25m, PC0_y2=-3m *) net c (c0, c2, c3);
endmodule

Portions that apply in only certain contexts can be selectively included with 'ifdef:

module amp (.a(a0), .c(c0));
  input a0;
  output c0;

  resistor #(.r(1k))      r1 (.p(a1), .n(b1));
  resistor #(.r(1k))      r2 (.p(b2), .n(c2));
  opamp741 #(.gain(100k)) u1 (.p(c3), .n(0), .ps(0), .ns(b3));

`ifdef SCHEMATIC
  (* S0_x0=-5m, S0_y0=0m,  S0_x1=0m,  S0_y1=0m *)  net a (a0, a1);
  (* S0_x1=24m, S0_y1=7m *)                        net b (b1, b2, b3);
  (* S0_x0=30m, S0_y0=-3m, S0_x2=25m, S0_y2=-3m *) net c (c0, c2, c3);
`endif
`ifdef LAYOUT    
  (* PC0_x0=-5m, PC0_y0=0m,  PC0_x1=0m,  PC0_y1=0m *)  net a (a0, a1);
  (* PC0_x1=24m, PC0_y1=7m *)                          net b (b1, b2, b3);
  (* PC0_x0=30m, PC0_y0=-3m, PC0_x2=25m, PC0_y2=-3m *) net c (c0, c2, c3);
`endif
endmodule

Paramset and module can be used, with ifdef, to add info that may be needed for particular applications.

`ifdef GSCHEM
  paramset opamp741 symbol
    .file(opamp4.sym);
  paramset resistor symbol
    .file(resistor2.sym);
`endif
`ifdef SIMULATION
  module opamp741 ( .....
    .....
  endmodule
`endif

module net23842 (1,2,3,4);
  net n23482 (1,2,4);
  net n84333 (2,3);
endmodule