Team:ETHZ Basel/Modeling/Light Switch

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(Facing the Combinatorial Explosion)
 
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= Modeling of the light switch =
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= The light switch =
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[[Image:ETHZ_Basel_molecular_comb.png|thumb|400px|'''Schematical overview of the devices and change upon light pulse induction.''' LSP refers to light switch protein, AP to anchor protein, anchor to the plasmid anchor and Che to the attacked protein of the chemotaxis pathway.]]
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We created two models representing the different biological approaches on how to control the tumbling frequency of the E. lemming,
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# a model representing the [[Team:ETHZ_Basel/Modeling/Light_Switch#Modeling of the PhyB/PIF3 light switch|PhyB/PIF3 based localization]] of proteins of the chemotaxis pathway,
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# a model representing the [[Team:ETHZ_Basel/Modeling/Light_Switch#Archeal light receptor|Archeal light receptor]].
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== Background ==
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== Modeling of the PhyB/PIF3 light switch ==
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In our biological setup, the relocation of one of the chemotaxis pathway proteins (either CheR, CheB, CheY or CheZ) is achieved by fusing them to a light-sensitive protein LSP1 (either to PhyB or to PIF3), which dimerizes by red light induction with the corresponding LSP2 (PIF3 or PhyB), fused to a spatially dislocated anchor. Since we decided to implement two different models of the chemotaxis pathway (see Sektion [[https://2010.igem.org/Team:ETHZ_Basel/Modeling/Chemotaxis|Chemotaxis Pathway]]), modeling all setups implemented in the wet-lab would have resulted in 16 different models:  
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[[Image:ETHZ_Basel_molecular_comb.png|thumb|400px|'''Figure 1: Schematic overview of the devices and change upon light pulse induction.''' LSP refers to light switch protein, AP to anchor protein and Che to the attacked protein of the chemotaxis pathway.]]
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=== Background ===
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In our biological setup, the relocation of one of the chemotaxis pathway proteins (either CheR, CheB, CheY or CheZ) is achieved by fusing them to a light-sensitive protein LSP1 (either to PhyB or to PIF3), which dimerizes by red light induction with the corresponding LSP2 (PIF3 or PhyB), fused to a spatially dislocated anchor. Since we decided to implement two different models of the chemotaxis pathway (see section [[Team:ETHZ_Basel/Modeling/Chemotaxis|Chemotaxis Pathway]]), modeling all setups implemented in the wet-lab would have resulted in 16 different models:  
|{CheR, CheB, CheY, CheZ} × {PhyB, PIF3} × {Model 1, Model 2}|=16.
|{CheR, CheB, CheY, CheZ} × {PhyB, PIF3} × {Model 1, Model 2}|=16.
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Inspired by the modular approach used as the [[Team:ETHZ_Basel/Biology/Cloning|Cloning Strategy]] in the wet-lab, we decided to decrease the combinatorial explosion by also applying a novel modular approach. Not only did this approach reduce the amount of models by a factor of four, it also allowed to widely separate the differential equations of the chemotaxis pathway from those of the light-induced localization system by simultaneously decreasing redundancies and thus decreasing the danger of slip of the pens. The underlying mathematical model for the light-induced relocation was completely developed by us (for a short discussion of the recently by Sorokina et al. published light-induced relocation system and why we did not use it, see here) as well as - to our knowledge - the approach to couple this model to models of the chemotaxis pathway.
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Inspired by the modular approach used for the [[Team:ETHZ_Basel/Biology/Cloning|Cloning Strategy]] in the wet-lab, we decided to decrease the combinatorial explosion by also applying a novel modular approach. Not only did this approach reduce the amount of models by a factor of four, but it also allowed to widely separate the differential equations of the chemotaxis pathway from those of the light-induced localization system by simultaneously decreasing redundancies and thus decreasing the danger of slip of the pens. The underlying mathematical model for the light-induced relocation was completely developed by us (for a short discussion of the recently by Sorokina et al. published light-induced relocation system and why we did not use it, see [[Team:ETHZ_Basel/Modeling/Sorokina|here]]) as well as - to our knowledge - the approach to couple this model to models of the chemotaxis pathway.
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== General remarks ==
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=== Assumptions ===
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In [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]]] Sorokina et al developed (''in vivo'') and modeled (''in silico'') the reversible activation of different phytochromes by red light and their deactivation by far-red light in yeast. Their main model is based on the proteins PhyA and FHL, which have similar properties as PhyB and PIF3 used in E. lemming , as described by the underlying [[Team:ETHZ_Basel/Biology/Molecular_Mechanism|molecular mechanism]].
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The following assumptions have been made according to the [[Team:ETHZ_Basel/Biology/Molecular_Mechanism| molecular mechanism]] to link the light switch and chemotaxis models:
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In this system, PhyA is fused to the Gal4 bindig domain (GBD) and FHL to the Gal4 transcriptional activator domain. Upon activation with red light, both chimeric proteins bind to each other and the complex can activate the transcription of a lacZ reporter which is under the control of a GAL4-responsive artificial promoter. Upon deactivation with far-red light, the complex dissociates and transcription of the lacZ gene is significantly reduced.
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In this model, Sorokina et al assume that PhyA protein sequesteres and only free PhyA can interact with FHL. They state that this interaction is necessary to explain the experimental data presented in the paper, consisting of the strength of fluorescence induced by lacZ over time for different experimental settings. It should be noticed that this signal constantly changes with time in the range of hours.
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* Upon red light pulse induction, the two light-sensitive protein (LSP1 and LSP2) domains can hetero-dimerize.
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* The TetR-LSP2 can bind to the operator (tetO) on the DNA.
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* Only after both reactions took place, we assume the Che protein to be spatially dislocated. This means
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** CheR-LSP1 is not able to methylate the MCPs anymore,
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** CheY-LSP1 can't be phosphorylated and interact with the motor anymore; nevertheless, it still can be dephosphorylated.
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** CheB-LSP1 is not able to demethylate the MCPs and can't be phosphorylated anymore, but still can be dephosphorylated,
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** CheZ-LSP1 can't dephosphorylate CheY anymore (This assumption is very unsteady, since CheY is not strictly located).
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* If only one of the reactions took place, we assume that the localization and activity of the fusion proteins are the same as for wild-type cells.
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== Implementation ==
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All of these assumptions will lead to a decrease of tumbling / directed movement ratio upon red light induction and an increase of corresponding far-red light induction.
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One of the models of system described by Sorokina et al [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]]] is available in the SBML format [[Team:ETHZ Basel/Modeling/Light_Switch#References|[2]]]. The model was exported to Matlab using SBToolbox2 [[Team:ETHZ Basel/Modeling/Light_Switch#References|[3]]]. However, only the system without input light signals was possible to be reproduced as presented in the paper [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]]], since the parameters necessary to define these signals were missing.
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It was tried to reverse engineer these parameters from the information given in the paper. However, the model available in SBML was slightly different from the model as described in the article: It was not possible to set the strength of the red and far-red light signals directly, but only the derivatives could be adjusted. This modeling decision might have been made to circumvent the problem that some integrators fail to solve a system of differential equations correctly when facing a step change too high in one of the derivatives. To test the model, this work-around was removed and the light inputs were not changed by steps, but by ramps with a length of 1s, which is significant smaller than the other time constants which were relevant for this part of the model.  When reproduction of the published data was tried, it was recognized that the strengths of the light signals had to be decreased by approximately 40 fold. Since the exactly inputs of the original simulations were unknown, it was not possible to deduce the reason for this necessary change in the parameters of the model.
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=== Facing the Combinatorial Explosion ===
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The main problem in separating <i>in silico</i> the chemotaxis pathway from the light-induced relocation system is the non-existence of a hierarchical relationship between the two sub-models: The properties of the chemotaxis pathway are clearly influenced if the ''active'' concentration of one of its key species drops, such that a natural strategy that stands out is giving the amount of localized proteins, obtained by the localization model, as an input to the chemotaxis model. However, also the concentration of the localized species of the localization model change depending on the reactions in the chemotaxis model, since several of the Che proteins are modeled as two or more molecular species. For example, the CheY protein is modeled as two species, one representing the phosphorylated and one the non-phosphorylated molecular concentration. Thus, the two models cannot be represented as e.g. a hierarchical block structure. This fact makes a modular approach significant more complicated.
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Furthermore, several other parameters were not available. These parameters were mainly needed to calculate the fluorescence signal strength from the lacZ concentration. In the paper [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]]], it was stated that these parameters were obtained for every experiments separatly by fits. To evaluate if the model can reproduce the data in the paper, one of the more important parameters (RLU in [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]]]) was estimated and the other parameters were set to the standard values from the SBML model, since changes of these parameters had similar effects.
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Our approach to modularize the model is based on an observation of the reaction directions which can take place in the overall model. For example, Figure 2 shows all eight species which have to be implemented to adequately describe the localization and phosphorylation states of CheY when fused to PhyB (the reactions taking place without CheY-PhyB, as for example the binding and unbinding of the PIF3-TetR monomer to tetO, are not depicted for simplicity). As can be seen, the reactions of the chemotaxis pathway and the reactions of the light model have different directions. The reactions of the light model are horizontal and independent of the phosphorylation level of CheY. On the other hand, the reactions of the chemotaxis model are vertically. However, one of the reactions of the chemotaxis model is not independent of the states mainly influenced by the light model: When CheY is localized at the DNA, the receptor complex cannot transfer a phosphor to it anymore. The respective species diagrams for the other three species (CheZ, CheB, CheR) as well as for the other light model (the Che protein is fused to PIF3 instead of PhyB) look similar, although the number of rows and columns can change.
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[[Image:ETHZ_Basel_chemotaxis_CheYSpecies.jpg|thumb|center|550px|'''Figure 2: Different species representing different localization and phosphorylation states of CheY.]]
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== Evaluation of the model ==
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We used this regularity to modularize the overall model: A variable table of states representing the concentration of all Che proteins in their different phosphorylation and localization modes is shared between the light model and the chemotaxis model. The number of rows of this table is dynamically determined by the chemotaxis model and the number of columns is determined by the light model, depending on the choice of which Che protein is fused to which light sensitive protein. The light model may only change the distribution of the species in each row, but may not change their sum (conservation relation). The chemotaxis model on the other hand may only change the distribution of the species concentration in each column. Although the tables may have different sizes, always the last column is representing the localized proteins. The chemotaxis model thus only applies a subset of reactions to this row, as mentioned in the assumptions.  
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{| border="0" align="center"
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|- valign="top"
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|[[Image:Sorokina1.jpg|thumb|440px|'''Figure 1.''' Reaction of the model to no light input (dashed black curve), red light for 10 min at t=18h (black curve), red light for 10 min at t=18h followed by a 10min far-red pulse after 0h (blue), 0.5h (cyan), 1h (red), 3h (green), 9h (blue). The values for RLU were set so that the data reproduced the measured data as described by Sorokina et al. This figure corresponds to figure 6A in [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]]].]]
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|[[Image:Sorokina2.jpg|thumb|440px|'''Figure 2.''' Same as Figure 1, only with the same value for RLU for every experiment (set to a value to reproduce Figure 8A in [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]).]]]]
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|}
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With the changes made to the model, it was possible to reproduce the data as presented in the paper. Two of the most significant figures (see Figure 1 and 2) were reproduced, which show the response of the system to different light input signals: Whether to no light input at all (dark), a single red light pulse at t=18h lasting for 10 min, or a 10 min red light pulse at t=18h followed by a 10 min far-red light pulse after 0.5h, 1h, 3h, or 9h. All experiments qualitatively and quantitaively reproduced the simulation results obtained by Sorokina et al (see Figure 6B and Figure 8A in [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]]]).
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All other species of both models are not shared between the two models, which also in any other way as mentioned above act independently. Using this approach we succeeded in uncoupling the model of the PhyB/PIF3 system from the model of the chemotaxis pathway, reducing the amount of redundancy and possible error sources significantly.
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== References ==
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== Archeal light receptor ==
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[1] [http://www.jbioleng.org/content/3/1/15  Sorokina et al: A switchable light-input, light-output system modelled and constructed in yeast. J Biol Eng. 2009 Sep 17;3:15.]
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Another modeling technique we employed in implementing the E. lemming was to fuse an archaeal photoreceptor to the'' E. coli'' chemotactic transducer, i.e. we replaced the usual receptor of E. coli that binds & is activated by chemo-attractant, with a receptor that is activated by blue-green light as demonstrated by Jung et al. (2001) [[Team:ETHZ Basel/Modeling/Light_Switch#References|[1]]].
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[2] [http://www.biomedcentral.com/content/supplementary/1754-1611-3-15-S3.XML 1754-1611-3-15-S3.XML]
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For the description of the molecular processes we could use our already [[Team:ETHZ_Basel/Modeling/Chemotaxis|implemented chemotaxis models]] from which we picked the chemotaxis model suggested by [[Team:ETHZ_Basel/Modeling/Chemotaxis|Mello & Tu (2003)]]. We had to replace the interaction between the chemo-attractant and the receptor with a interaction between light and the receptor which gives rise to the same set of events down stream of the chemotaxis pathway.
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[3] [http://www.sbtoolbox2.org/ SBToolbox2]
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The strategy to model this interaction was to define the dynamic receptor occupancy as a dynamic function of the light input. The receptor occupancy reflects the fraction of receptors activated by the stimulus (chemo-attractant or light).
 +
 
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With the help of this implementation, we were able to display the internal CheYp concentration, to estimate the photoreceptor occupancy and to calculate the bias as shown in the [[Team:ETHZ_Basel/Achievements/E_lemming|E. lemming section]].
 +
 
 +
== Download ==
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Both light switch models are included within the [[Team:ETHZ_Basel/Achievements/Matlab_Toolbox|Matlab Toolbox]] and can be downloaded there.
 +
 
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== References ==
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[1] [http://jb.asm.org/cgi/reprint/183/21/6365?maxtoshow=&hits=10&RESULTFORMAT=1&andorexacttitle=and&andorexacttitleabs=and&fulltext=An+archaeal+photosignal-transducing+module+mediates+phototaxis+in+%27%27Escherichia+&andorexactfulltext=and&searchid=1&FIRSTINDEX=0&sortspec=relevance&resourcetype=HWCIT: Jung et al: An Archaeal Photosignal-Transducing Module Mediates Phototaxis in Escherichia coli]

Latest revision as of 03:55, 28 October 2010

The light switch

We created two models representing the different biological approaches on how to control the tumbling frequency of the E. lemming,

  1. a model representing the PhyB/PIF3 based localization of proteins of the chemotaxis pathway,
  2. a model representing the Archeal light receptor.

Modeling of the PhyB/PIF3 light switch

Figure 1: Schematic overview of the devices and change upon light pulse induction. LSP refers to light switch protein, AP to anchor protein and Che to the attacked protein of the chemotaxis pathway.

Background

In our biological setup, the relocation of one of the chemotaxis pathway proteins (either CheR, CheB, CheY or CheZ) is achieved by fusing them to a light-sensitive protein LSP1 (either to PhyB or to PIF3), which dimerizes by red light induction with the corresponding LSP2 (PIF3 or PhyB), fused to a spatially dislocated anchor. Since we decided to implement two different models of the chemotaxis pathway (see section Chemotaxis Pathway), modeling all setups implemented in the wet-lab would have resulted in 16 different models:

|{CheR, CheB, CheY, CheZ} × {PhyB, PIF3} × {Model 1, Model 2}|=16.

Inspired by the modular approach used for the Cloning Strategy in the wet-lab, we decided to decrease the combinatorial explosion by also applying a novel modular approach. Not only did this approach reduce the amount of models by a factor of four, but it also allowed to widely separate the differential equations of the chemotaxis pathway from those of the light-induced localization system by simultaneously decreasing redundancies and thus decreasing the danger of slip of the pens. The underlying mathematical model for the light-induced relocation was completely developed by us (for a short discussion of the recently by Sorokina et al. published light-induced relocation system and why we did not use it, see here) as well as - to our knowledge - the approach to couple this model to models of the chemotaxis pathway.

Assumptions

The following assumptions have been made according to the molecular mechanism to link the light switch and chemotaxis models:

  • Upon red light pulse induction, the two light-sensitive protein (LSP1 and LSP2) domains can hetero-dimerize.
  • The TetR-LSP2 can bind to the operator (tetO) on the DNA.
  • Only after both reactions took place, we assume the Che protein to be spatially dislocated. This means
    • CheR-LSP1 is not able to methylate the MCPs anymore,
    • CheY-LSP1 can't be phosphorylated and interact with the motor anymore; nevertheless, it still can be dephosphorylated.
    • CheB-LSP1 is not able to demethylate the MCPs and can't be phosphorylated anymore, but still can be dephosphorylated,
    • CheZ-LSP1 can't dephosphorylate CheY anymore (This assumption is very unsteady, since CheY is not strictly located).
  • If only one of the reactions took place, we assume that the localization and activity of the fusion proteins are the same as for wild-type cells.

All of these assumptions will lead to a decrease of tumbling / directed movement ratio upon red light induction and an increase of corresponding far-red light induction.

Facing the Combinatorial Explosion

The main problem in separating in silico the chemotaxis pathway from the light-induced relocation system is the non-existence of a hierarchical relationship between the two sub-models: The properties of the chemotaxis pathway are clearly influenced if the active concentration of one of its key species drops, such that a natural strategy that stands out is giving the amount of localized proteins, obtained by the localization model, as an input to the chemotaxis model. However, also the concentration of the localized species of the localization model change depending on the reactions in the chemotaxis model, since several of the Che proteins are modeled as two or more molecular species. For example, the CheY protein is modeled as two species, one representing the phosphorylated and one the non-phosphorylated molecular concentration. Thus, the two models cannot be represented as e.g. a hierarchical block structure. This fact makes a modular approach significant more complicated.

Our approach to modularize the model is based on an observation of the reaction directions which can take place in the overall model. For example, Figure 2 shows all eight species which have to be implemented to adequately describe the localization and phosphorylation states of CheY when fused to PhyB (the reactions taking place without CheY-PhyB, as for example the binding and unbinding of the PIF3-TetR monomer to tetO, are not depicted for simplicity). As can be seen, the reactions of the chemotaxis pathway and the reactions of the light model have different directions. The reactions of the light model are horizontal and independent of the phosphorylation level of CheY. On the other hand, the reactions of the chemotaxis model are vertically. However, one of the reactions of the chemotaxis model is not independent of the states mainly influenced by the light model: When CheY is localized at the DNA, the receptor complex cannot transfer a phosphor to it anymore. The respective species diagrams for the other three species (CheZ, CheB, CheR) as well as for the other light model (the Che protein is fused to PIF3 instead of PhyB) look similar, although the number of rows and columns can change.

Figure 2: Different species representing different localization and phosphorylation states of CheY.

We used this regularity to modularize the overall model: A variable table of states representing the concentration of all Che proteins in their different phosphorylation and localization modes is shared between the light model and the chemotaxis model. The number of rows of this table is dynamically determined by the chemotaxis model and the number of columns is determined by the light model, depending on the choice of which Che protein is fused to which light sensitive protein. The light model may only change the distribution of the species in each row, but may not change their sum (conservation relation). The chemotaxis model on the other hand may only change the distribution of the species concentration in each column. Although the tables may have different sizes, always the last column is representing the localized proteins. The chemotaxis model thus only applies a subset of reactions to this row, as mentioned in the assumptions.

All other species of both models are not shared between the two models, which also in any other way as mentioned above act independently. Using this approach we succeeded in uncoupling the model of the PhyB/PIF3 system from the model of the chemotaxis pathway, reducing the amount of redundancy and possible error sources significantly.

Archeal light receptor

Another modeling technique we employed in implementing the E. lemming was to fuse an archaeal photoreceptor to the E. coli chemotactic transducer, i.e. we replaced the usual receptor of E. coli that binds & is activated by chemo-attractant, with a receptor that is activated by blue-green light as demonstrated by Jung et al. (2001) [1].

For the description of the molecular processes we could use our already implemented chemotaxis models from which we picked the chemotaxis model suggested by Mello & Tu (2003). We had to replace the interaction between the chemo-attractant and the receptor with a interaction between light and the receptor which gives rise to the same set of events down stream of the chemotaxis pathway.

The strategy to model this interaction was to define the dynamic receptor occupancy as a dynamic function of the light input. The receptor occupancy reflects the fraction of receptors activated by the stimulus (chemo-attractant or light).

With the help of this implementation, we were able to display the internal CheYp concentration, to estimate the photoreceptor occupancy and to calculate the bias as shown in the E. lemming section.

Download

Both light switch models are included within the Matlab Toolbox and can be downloaded there.

References

[1] [http://jb.asm.org/cgi/reprint/183/21/6365?maxtoshow=&hits=10&RESULTFORMAT=1&andorexacttitle=and&andorexacttitleabs=and&fulltext=An+archaeal+photosignal-transducing+module+mediates+phototaxis+in+%27%27Escherichia+&andorexactfulltext=and&searchid=1&FIRSTINDEX=0&sortspec=relevance&resourcetype=HWCIT: Jung et al: An Archaeal Photosignal-Transducing Module Mediates Phototaxis in Escherichia coli]