Imperial/Infector Detector/Modelling

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Presented below are the most essential results of the simulations performed.
Presented below are the most essential results of the simulations performed.
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[[Image: IC07 Comparison AHL.png|thumb|left|600px|'''Figure 3''': Comparison of the sensitivity, response time and maximal output of <font color=red>Construct 1</font> and <font color=blue>Construct 2</font>, , for varying initial [AHL] <br>i.e. AHL<sub>0</sub> = 0, 0.1, 1, 5, 10, 100 & 1000 nM]]<br clear="all">
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[[Image: IC07 Comparison AHL.png|thumb|left|600px|'''Figure 3''': Comparison of the sensitivity, response time and maximal output of <font color=blue>Construct 1</font> and <font color=red>Construct 2</font>, for varying initial [AHL] i.e. AHL<sub>0</sub> = 0, , 1, 5, 10, 100 & 1000 nM]]<br clear="all">
====Discussion====
====Discussion====

Revision as of 04:45, 25 October 2007



Infector Detector: Modelling

Abstract

Infector Detector (ID) is a simple biological detector, which serves to expose bacterial biofilm. It functions by exploiting the inherent AHL (Acetyl Homoserine Lactone) production employed by certain types of quorum-sensing bacteria, in the formation of such structures.
This section presents a preliminary model for an AHL detector, which employs the backbone of the Lux quorum-sensing feedback mechanism. Figures 1 and 2 below illustrate the full system we are investigating.

In the design phase, two possible system constructs were proposed, as a solution to the problem of detecting AHL-producing biofilm.
According to our specifications, the most crucial feature of this system is the sensitivity to a minimum [AHL] of 5nm. In other words, we need to identify the minimal AHL concentration for appreciable expression of a chosen reporter protein.
Furthermore, we attempt to define a functional range for possible AHL detection. How does increased AHL concentration impact on the maximal output of reporter protein?
Finally, we investigate how the system performance can be tailored, by exploiting possible inputs to the system (e.g. varying initial LuxR concentration and/or concentration of pLux promoters). In performing such customizations, the question arises: what is the impact upon the maximal output of fluorescent reporter protein and/or response time?

We attempt to answer such questions by establishing a representative model, and consequently, conducting a simulation of the system in-silico.

Implementation & Reaction Network

In line with the concept of abstraction in Synthetic Biology, the correlation of the output of the proposed system constructs to their inputs, can be visualized by the following black-box illustrations of the two cases. It is evident that AHL is an input to both constructs; a function of the particular biofilm. Furthermore, energy and promoter concentration are included as auxillary inputs to both system constructs. LuxR, is an additional input, exclusive to construct 2, which lacks constitutive expression of LuxR by pTET.
(this of course occuring within our cell-free chassis)

Figure 1: Black-box for Construct 1
Figure 2: Black-box for Construct 2

The Reaction Network

AHL is assumed to diffuse freely "into" the system (we are dealing with cell-free system, which comes into direct contact with the biofilm). The target AHL molecules, produced by the biofilm, equilibrate between the two systems - the detector and the target. Once equilibrium of AHL is reached, AHL binds with the monomeric protein LuxR, which is either constitutively produced by construct 1, or directly introduced in purified form, as part of the solution which is construct 2. The binding of these two proteins yieds the product A, the intermediating LuxR-AHL complex, which is assumed to be immediately transcriptionally competent. The reactions here are considered as reversible (forward and backward reactions of this step governed by the kinetic constants k2 and k3 respectively). The formed transcription factor activates the transcription of the pLux operon, which codes for the relevant reporter protein, presented here as GFP. Activation occurs by way of the reversible binding of this transcription factor, A, to the response sequences in the operon (k4 and k5) . This leads to recruitment of RNA polymerase and increases the frequency of transcription initiation (Fuqua et al., 2001) of the construct gfp gene (strictly forward reaction, governed by k6).

Figure 3: Reaction network for Construct 1 (Energy-dependent)
Figure 4: Reaction network for Construct 2 (Energy-dependent)


Representative Model

In developing this model, we were interested in the behaviour at steady-state, that is when the system has equilibrated and the concentrations of the state variables remain constant.

At reasonably high molecular concentrations of the state variables, a continuous model can be adopted, which is represented by a system of ordinary differential equations.

It is for this reason that our approach to modelling the system follows a deterministic, continuous approximation.

We can condition the system in various manners, but for the purposes of our project, we will seek a formulation which is valid for both constructs considered, i.e. the governing equations are a represenation of both constructs.

The only difference is with regards to the parameter k1, the maximum transcription rate of the constitutive promoter (pTET). Therefore in construct 1, k1 is non-zero; k1 = 0 for construct 2 (which lacks pTET).

Our analysis took us through a number of models, but presented here is the most pertinent, most representative version. This model is based on energy-dependence (limited nutrient supply), which follows Hill-like dynamics.

The system kinetics are determined by the following coupled-ODEs. For a derivation of the governing equations, please access

Model 2, an energy-dependent network, where the dependence on energy assumes Hill-like dynamics



Model Parameters

Parameter Description
Kinetic
Constants
k1 Maximal constitutive transcription of LuxR by pTET
k2 Binding between LuxR and AHL
k3 Dissociation of protein complex LuxR-AHL (A)
k4 Binding between A and pLux promoter
k5 Dissociaton of A-pLux complex
k6 Transcription of FP
Degradation
Rates
δLuxR Degradation rate of LuxR
δAHL Degradation rate of AHL
δGFP Degradation rate of GFP
Hill Co-operativity
n Co-operativity coefficient describing the degree
of energy dependence, which follows Hill-like dynamics
Energy consumption
of transcription
α1 Energy consumption due to constitutive transcription of LuxR
α2 Energy consumption due to transcription of gfp gene


We now present the essential features of the system behaviour, simulated for a given set of parameters.

Simulations

Jaroslaw - Should we create a separate simulations page, perhaps? These plots are essential, and was also thinking of putting some 3-d plots of transfer function for C1 and C2. Also, this would allow more freedom with sizing of the images - better clarity if greater. I really don't think these simulations need to be cramped here.

Presented below are the most essential results of the simulations performed.

Figure 3: Comparison of the sensitivity, response time and maximal output of Construct 1 and Construct 2, for varying initial [AHL] i.e. AHL0 = 0, , 1, 5, 10, 100 & 1000 nM

Discussion

From figure 3, it is evident that the response time of construct 1 (C1) is far greater than that of construct 2 (C2). C1 crosses some arbitrary threshold, say 6000 a.u. at approximately t = 150min, whereas C2 below 10min. This is in line with our hypothesis, as we know steady-state has been forced upon the system in the case of construct 2 - by flooding the system with purified LuxR.

Secondly, the peak expression (max output) of GFP obtained for C1 is lower by approximately 50 percent. So, C2 produces a stronger output for corresponding [AHL]. However, although C2 is faster and generates a greater output, its energy consumption is far more pronounced. C1 thus has a greater lifespan.

Finally, in terms of sensitivity, construct 2 is also more sensitive to lower [AHL]; for the lowest [AHL] simulated, the peak output is 3 times greater than that of construct 1.


Figure 4: Comparison of constructs w.r.t their respective transfer functions, after t = 50min (x-axis is log-scaled)
Figure 5: Comparison of constructs w.r.t their respective transfer functions, after t = 200min (x-axis is log-scaled)

Discussion

Figures 4 and 5 illustrate the comparison of the transfer function of both constructs, at two time instances: t = 50min and t = 200min. Consider figure 5, which illustrates the greater sensitivity to AHL offered by construct 2. Appreciable expression of GFP occurs at concentration of AHL at least one order of magnitude lower than in the case of construct 1.

It can also be seen, that at saturation, the peak expression, is considerably greater - approximately 25 % greater than that offered by construct 1.

Figure 4, portrays clearly, the far superior response time of construct 2 (as expected).

Conclusions

From the simulations performed, construct 2 outperforms contruct 1 on the basis of sensitivity, response time and maximal output of reporter. Construct 1 is superior in terms of energy-efficiency. Its life-time is far greater than that of its counterpart.

It is evident that both constructs have their major strengths - strengths that require testing and validation in the context of the laboratory - this forms the pathway to their effective characterization.

Data Analysis follows the experimental data gathering stage, with the task of validation of the model, and ultimately extraction of biologically representative parameters.

Just testing image clarity, font size, colours

test
test

Software

All deterministic simulations were performed using Matlab 7 (The MathWorks Inc., Natick, MA).

  • m-files of all simulations are available on our Software page.

References

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