# The Azimuth Project Blog - Petri net programming (part 1) (Rev #13, changes)

Showing changes from revision #12 to #13: Added | Removed | Changed

# Contents

## Introduction

Petri nets are a simple model of computation with a range of modelling applications that include chemical reaction networks, manufacturing processes, and population biology dynamics. They are graphs through which entities flow and have their types transformed. They also have far-reaching mathematical properties which are the subject of an extensive literature. See the Network Theory series on the Azimuth Blog for a panoramic and well-diagrammed introduction to the theory and applications of Petri nets.

In this series of articles, we approach the concepts with the aim of writing programs that make them work. The readership would include coding enthusiasts, professional programmers, scientists interested in programming models, software engineers and computer scientists. The articles will present brief tutorials, give programs to exercise the concepts, and analyze the code. These illustrative programs should give the reader some clay to work with.

We Here now we introduce Petri nets and give a simulator program. It This will be applied to a “toy” model of a chemical reaction network for the synthesis and dissociation of H2O molecules.

## Definition of Petri nets

A Petri net is a diagram with two kinds of nodes: container nodes, called species (or “places”, “states”), which can hold zero or more tokens, and transition nodes, which are “wired” to some containers that called are itsinputs and some called itsoutputs. A transition can have multiple input or output connections to a single container.

When a transition fires, it removes one token from each input container, and adds one token to each output container. When there are multiple inputs or outputs to the same container, then that many tokens get removed or added.

The total state of the Petri net is described by a labelling function that which maps each container to the number of tokens it holds. A transition isenabled to fire in a labelling if there are enough tokens at its input containers. If no transitions are enabled, the it is halted. The sequencing is non-deterministic, because in a given labelling there may be several transitions that are enabled. Dataflow arises whenever one transition sends tokens to a container that is read by another transition.

## Using Petri nets to model Entity Conversion Networks

Petri nets can describe networks consisting of entities of different species, with conversion reactions from the input species to the output species. Each entity is symbolized by a token in the net, and all the tokens for a species are grouped into a container. The conversion of entities is symbolized by a transition that consumes input tokens and generates output tokens.

One application is to population dynamics. The tokens represent organisms, and the species are biological species. A simplified example, involving two species, Wolf and Rabbit, is given on the Network Theory page. There are three transitions: Birth, which takes one Rabbit in and outputs two Rabbits (like asexual reproduction), Predation, which converts Rabbit plus Wolf to Wolf plus Wolf, and Death, which inputs one Wolf and outputs nothing.

A major application is to chemical reaction networks. The entities are chemical units: molecules, isolated atoms, or ions. Each chemical unit is represented by a token in the net, and a container holds all of the tokens for a chemical species. Chemical reactions are then modeled as transitions that consume input tokens and generate output tokens.

We will be using the following simplified model for water formation and dissociation, which is presented in the Network Theory page.

• The species are H, O, and H2O.

• Transition combine inputs two H atoms and one O atom, and outputs an H2O molecule.

• Transition split is the reverse process, which inputs one H2 and outputs two H and one O.

Note that the model is intended to show the idea of chemical reaction Petri nets, so it is not physically realistic. The actual reactions involve H2, O2, and there are intermediate transitions involving OH for the stages of the reaction.

## A Petri net simulator

Here is our PROGRAM to simulate a Petri net. It uses parameters that describe the species, the transition, and an initial labelling, and then runs the net for a specified number of steps. At each stage of the process it chooses randomly among the enabled transitions, fires it, and prints the new labelling on the console.

Note: in the next article, on stochastic Petri nets, we will enhance the model with statistical parameters that control the relative firing rates of the transitions. Here we are establishing the groundwork.

### Running the script

The code is a self-contained Python script. See the APPENDIX for notes on obtaining the interpeter.

The model parameters are already coded into the script. So let’s give it whirl:

python petri1.py

This produced the output:

H, O, H2O, Transition
5, 3, 4, split
7, 4, 3, split
9, 5, 2, combine
7, 4, 3, combine
5, 3, 4, split
7, 4, 3, split
9, 5, 2, split
11, 6, 1, combine
9, 5, 2, split
11, 6, 1, split
13, 7, 0, ...

In words, we started out in a state with 5 H’s, 3 O’s, and 2 H2O’s, then a split took place, which increased H by 2, increased O by 1, and decreased H2O by one, then…

Running it again gives a different execution sequence.

### Top-level structure of the script

The script constructs a Petri net object, using parameters for the species and transitions, and then runs it.

Construct the net:

petriNet = PetriNet(
["H", "O", "H2O"],    # states
["combine", "split"], # transitions
[("combine",2,"H"), ("combine",1,"O"), ("split",1,"H2O")], # inputs
[("combine",1,"H2O"), ("split",2,"H"), ("split",1,"O")],   # outputs
#
# combine has 2 H inputs, 1 O input, and 1 H2O output
# split has 1 H20 input, 2 H outputs, and 1 O output
)

Sets up the initial condition of the net:

initialLabelling = {"H":5, "O":3, "H2O":4}

Then run it for twenty steps:

steps = 20
petriNet.RunSimulation(steps, initialLabelling)

Exercise: Improve the script to accept the model parameters from the command-line. Hints: Use “import sys,” and sys.argv[i]. Then you can pass strings like “[H, O, H20]” from the command line, and use the eval function on them.

### Anatomy of the program

We represent species by their strings names that (strings), name them, and use object classes for Transition and Petri PetriNet. net. A PetriNet instance will contain a collection of Transition instances, and it will contain the current labelling. The top-level method in PetriNet, called RunSimulation, makes repeated calls to a method FireOneRule. FireOneRule constructs the list of enabled transitions, chooses one randomly, and fires it. This work is supported by the Transition class, which provides methods IsEnabled, and Fire. The Fire method takes a labelling in, and updates the counts in it—decrementing the input token counts, and incrementing the output token counts.

The Transition class contains a map that describes the input connections. It maps each species name to the number of times that it is taken as input. The transition class contains a similar map to describe the output connections.

A Petri net object has a member that holds the current labelling, which is a map (dictionary) from stateName to the token count.

The chief data in the Petri net classes are the Transition objects, and the labeling, which describes the current configuration of the net.

The Transition object contains two maps… Transition exposes two key methods, both of which operate on labellings: isEnabled takes a labeling as parameter, and returns a boolean saying whether it is enabled to fire. This is determined by comparing the input map for the transition with the token counts in the labeling, to see if there is sufficient tokens for it to fire.

The constructor for the Petri net class takes the transition specifications, and “digests” them into the initial data structures used in the simulation. This involves constructing Transition objects for each of the transitions.

Each transition object contains a map (dictionary) from input species name to the number of times that the species is input to the transition, and an output map with the same structure.

The PetriNet class contains the list of species names, the list of transition names, the current labelling, which maps species names to integers, and a map from transition names to Transition objects.

The top-level method in PetriNet is RunSimulation, which makes repeated calls to a method called FireOneRule. FireOneRule constructs the list of enabled transitions, chooses one randomly, and fires it. This is facilitated by the methods IsEnabled and Fire on the Transition class.

The fire method takes a labeling in, and performs the action indicated by the transition: it removes tokens from the input, and adds tokens to the output. It modifies the labelling, decreasing the values for the inputs, and increasing the values for the outputs.

Here is the Transition class:

Now that our Petri net is equipped with a labelling and a list of Transitions, each with an isEnabled and fire method, it has everything that it needs to fire a rule: pick a transition, check if it is enabled in the current labelling, and if so, call the Fire method on the transition, to update the labelling to the new state. All that is left for running a simulation is to specify a rule for choosing which enabled transition to fire: For this, our first program, we will just choose a random transition.

The top-level entry point is the method runSimulation, which takes the initial labelling, and a number of states to iterate.

Here is the main Petri net class:

Note that the PetriNet inherits from a base class PetriNetDataStructures. This base class was separated for clarity, and contains the “housekeeping” methods needed to support PetriNet: printHeader, printLabelling, and, not to be forgotten, the constructor, which converts the specifications ‘[combine,2,H etc. into the actual transition objects. Here is the code for it:]

# Author line
#
#!/usr/bin/python
#
# for Windows without cygwin, use this form for the top line:
#!C:\Python27\python.exe

import string
from random import random,randrange

def selectRandom(list):
return list[randrange(len(list))]

# States are represented just by their names, no class is needed

class Transition:
# Fields used in this class:
#
# name -- transitionName
# inputs: stateName -> inputCount
# outputs: stateName -> outputCount

def __init__(this, transitionName):
this.transitionName = transitionName
this.inputs = {}
this.outputs = {}

def isEnabled(this, labelling):
for inputState in this.inputs.keys():
if labelling[inputState] < this.inputs[inputState]:
return False  # not enough tokens to fire

return True # good to go

def fire(this, labelling):

print this.transitionName

for inputName in this.inputs.keys():
labelling[inputName] = labelling[inputName] - this.inputs[inputName]

for outputName in this.outputs.keys():
labelling[outputName] = labelling[outputName] + this.outputs[outputName]

class PetriNetDataStructures:
# Fields:
#
# transitionNames
# stateNames
# transitionMap: transitionName -> TransitionObject
# labelling -- mapping (dict) from state name to count

def buildTransitions(this, inputSpecs, outputSpecs):
this.transitionMap = {}

for (transitionName, degree, stateName) in inputSpecs:
this.getTransition(transitionName).inputs[stateName] = degree

for (transitionName, degree, stateName) in outputSpecs:
this.getTransition(transitionName).outputs[stateName] = degree

def getTransition(this, transitionName):
if not(this.transitionMap.has_key(transitionName)):
this.transitionMap[transitionName] = Transition(transitionName)
return this.transitionMap[transitionName]

print string.join(this.stateNames, ", ") + ", Transition"

def printLabelling(this):
for stateName in this.stateNames:
print str(this.labelling[stateName]) + ",",

class PetriNet(PetriNetDataStructures):

def __init__(this, stateNames, transitionNames, inputMap, outputMap):
this.stateNames = stateNames
this.transitionNames = transitionNames
this.buildTransitions(inputMap, outputMap)

def runSimulation(this, iterations, initialLabelling):

this.labelling = initialLabelling
this.printLabelling()

i = 0
while not(this.isHalted()):

this.fireOneRule()
this.printLabelling();
i = i + 1
if i == iterations:
print "done"
return

print "halted"

def enabledTransitions(this):
return filter(
lambda transition: transition.isEnabled(this.labelling),
this.transitionMap.values())

def isHalted(this):
return len(this.enabledTransitions()) == 0

def fireOneRule(this):
selectRandom(this.enabledTransitions()).fire(this.labelling)

# now build a net for two opposite transitions:
# combine: formation of water molecule
# split: dissociation of water molecule

net = PetriNet(
["H", "O", "H2O"],    # states
["combine", "split"], # transitions
[("combine",2,"H"), ("combine",1,"O"), ("split",1,"H2O")], # inputs
[("combine",1,"H2O"), ("split",2,"H"), ("split",1,"O")],   # outputs
#
# combine has 2 H inputs, 1 O input, and 1 H2O output
# split has 1 H20 input, 2 H outputs, and 1 O output
)

initialLabelling = {"H": 5, "O": 3, "H2O": 4}
steps = 20

net.runSimulation(steps, initialLabelling)

## Conclusion

We’ve learned a cool new idea, and how to do something cool with it. This is only the beginning, in terms of the applications and the theory.

There is an important limitation to our current program: it just randomly picks a rule. In our example, the system just made a kind of random walk (back and forth) between the states of full dissociation – all H and O atoms, no H2O molecules – and all H2O molecules. But in a real system, the rates at which the transitions fires are probabilistically determined, and depend, among other things, on the temperature of the system. With a high probability for formation, and a low probability for dissociation, we would expect the system to reach an equilibrium state in which H2O is the predominant “token” in the system. [The relative concentration of H20 would depend on the relative probabilities of the transitions.]

This gives motivation for the topic of our next article, which is stochastic Petri nets.

## Appendix: Notes on the software environment

The sample programs here are in Python, which is a good language for simple proof-of-concept programs.

You have a few options to choose from, in terms of distributions:

• If you are on a Linux/unix type of system, it may already be installed, or use the package manager to install it.

• In Windows, you can use the version from the python.org web site. Alternatively, install cygwin, and choose Python on the setup menu, and then you can try to pretend that you are working in a nix system.

• Another interesting distribution is [from] Enthought, which comes pre-built with an open-source scientific and numeric computing environment, scipy, numpy, matplotlib, …

The program is distributed as a self-contained script, so from Linux and cygwin, you can just execute ./petri1.py. You just have to adjust the first line to point to the interpreter. Even from cygwin, you can refer to the native python executable, or the enthought distribution.

## References

• Network Theory

• Petri Nets – Wikipedia

• python

• cygwin

• enthought

## Stochastic Petri nets

A nice elaboration of the basic model is the stochastic Petri net, which consists of a Petri net, along with data that gives a rate coefficient for each transition. The firing rate for a transition will equal its rate coefficient times the product of the number of tokens at each input state (using multiple factors if a state occurs multiple times as an input).

This definition is motivated by the model of chemical reaction networks where the reaction rates are proportional to the product of the concentrations of the input constituents. We can think of the rate coefficient for a transition as a magnitude that takes into account both the “temperature” of the system of tokens and the “ease” with which the input tokens will combine to trigger the reaction, once they are brought into proximity.