IGEM:IMPERIAL/2007/Dry Lab/Modelling/ID: Difference between revisions

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==Formulation of the problem==
==Formulation of the problem==
*Questions to be answered with the approach
As described earlier, Infector Detector (ID) is a simple biological detector, which serves to expose bacterial biofilm. It functions by exploiting the inherent AHL production employed by the quorum-sensing bacteria, in the formation of such structures.<br>
*Verbal statement of background
 
*What does the problem entail?
<font color = red>~~Insert diagram illustrating this phenomenon </font><br>
*Hypotheses employed
 
Our project attempts to improve where previous methods of biofilm detection have proven ineffective: first and foremost, by focussing on the sensitivity of the system, to low levels of AHL production (bacterial chatter).
In doing so, a complete investigation of the level of sensitivity to [AHL] needs to be performed - in other words, what is the minimal [AHL] for appreciable expression of reporter protein. Furthermore, establish a functional range for AHL detection. How does increased [AHL] impact on maximal output of reporter protein?<br>
Also, how can the system performance be tailored, by exploiting the remaining state variables (e.g. varying initial [LuxR] and/or [pLux]). 
 
The system performance here revolves most importantly around AHL sensitivity; however, the effect on, maximal output of fluorescent reporter protein and/or response time is, likewise, of great importance.
 
Our approach, involves the proposal of two simple constructs, varying with respect to the manner in which LuxR is introduced into the system:
*Construct 1 - represented by [http://parts.mit.edu/registry/index.php/Part:BBa_T9002| T9002], incorporates constitutive expression of LuxR by pTET.
*Construct 2 - simpler in nature, lacks pTET; LuxR is introduced in purified form here.<br>
 
<font color = red>~~Here explain briefly why Construct 2 was selected, i.e. we were concerned with the time the system would take to reach steady-state (that is before energy-dependence was considered) - due to almost negligible <math> \delta_{LuxR}</math>, etc </font>.


==Selection of model structure==
==Selection of model structure==
*Present general type of model
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.
#is the level of description macro- or microscopic
 
#choice of a deterministic or stochastic (!) approach
It is for this reason that our approach to modelling the system follows a deterministic, continuous approximation. 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.
#use of discrete or continuous variables
 
#choice of steady-state, temporal, or spatio-temporal description
In adopting this approach, we perform the following assumptions:
*determinants for system behaviour? - external influences, internal structure...
 
*assign system variables
====Assumptions====
*Ignore spatial information of the system; we ignore molecular dynamics of the system - this is a kinetic model.
*Keep track of total number of molecules of each type - by tracking the concentrations of these state variables (as a continuous variable)
*System is homogeneous - well-stirred, so that the molecules of each type are spread uniformly throughout the spatial domain. In doing so, we assume thermal equilibrium
*Volume of the spatial domain remains constant
 
 
The system kinetics are determined by the following six coupled-ODEs.


==Our models==
==Establishing a representative model==


* '''Introduction'''
* '''Introduction'''
We can condition the system in various manners, but for the purposes of our project, Infector Detector, we will seek a formulation which is valid for both constructs considered. Our system can thus be modellied by the following Dynamical System:
We can condition the system in various manners, but for the purposes of our project, Infector Detector, we will seek a formulation which is valid for both constructs considered. <br><br>
 
Our initial approach assumed that energy would be in unlimited supply, and that our system would eventually reach steady-state (Model 1). Experimentation suggested otherwise; our system needed to be amended. This lead to the development of model 2, an energy-dependent network, where the dependence on energy assumed Hill-like dynamics:
<br><br>
<br><br>


<br><br>
===Model 1: Steady-state is attained; limitless energy supply <font color = red>''(link here to derivation)''</font>===
The system of equations for the two constructs varies strictly with respect to the value of the parameter k1. Construct 1 possesses a non-zero k1 rate constant, whereas for construct 2, a zero value is assumed.
 
<br>
<math>\frac{d[LuxR]}{dt} = k_1 + k_3[A] - k2[LuxR][AHL]- \delta_{LuxR}[LuxR]</math>
 
<br>
<math>\frac{d[AHL]}{dt} = k_3[A] - k2[LuxR][AHL]- \delta_{AHL}[AHL]</math>


<math>\frac{d[A]}{dt} = -k_3[A] + k2[LuxR][AHL]- k_4[A][P] + k_5[AP]</math>


===Model 1: Steady-state is attained; limitless energy supply ===
<math>\frac{d[P]}{dt} = -k_4[A][P] + k_5[AP]</math>


<math>\frac{d[AP]}{dt} = k_4[A][P] - k_5[AP]</math>


<math>\frac{d[GFP]}{dt} = k_6[AP] - \delta_{GFP}[GFP]</math>


===Model 2: Equations developed through steady-state analysis; however due to limited energy supply, we operate in the transient regime===
===Model 2: Equations developed through steady-state analysis; however due to limited energy supply, we operate in the transient regime===
<br>
<math>\frac{d[LuxR]}{dt} = k_1\bigg(\frac{[E]^n}{K_E^n + [E]^n}\bigg) + k_3[A] - k_2[LuxR][AHL]- \delta_{LuxR}[LuxR]</math>
<math>\frac{d[LuxR]}{dt} = k_1\bigg(\frac{[E]^n}{K_E^n + [E]^n}\bigg) + k_3[A] - k_2[LuxR][AHL]- \delta_{LuxR}[LuxR]</math>
<br>
<br>
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<math>\frac{d[A]}{dt} = -k_3[A] + k_2[LuxR][AHL]- k_4[A][P] + k_5[AP]</math>
<math>\frac{d[A]}{dt} = -k_3[A] + k_2[LuxR][AHL]- k_4[A][P] + k_5[AP]</math>


<math>\frac{d[P]}{dt} = -k_4[A][P] + k_5[P]</math>
<math>\frac{d[P]}{dt} = -k_4[A][P] + k_5[AP]</math>


<math>\frac{d[AP]}{dt} = k_4[A][P] - k_5[AP]</math>
<math>\frac{d[AP]}{dt} = k_4[A][P] - k_5[AP]</math>
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n is the positive co-operativity coefficient (Hill-coefficient)<br>
n is the positive co-operativity coefficient (Hill-coefficient)<br>
<math>K_E \ </math> the half-saturation coefficient
<math>K_E \ </math> the half-saturation coefficient
=== State Variables ===
<font color = red>Create similar table for state variables, as for parameter table below</font>
=== Model Parameters ===
<font color = red>Populate parameters table</font>
{| class="wikitable" border="1" cellspacing="0" cellpadding="2" style="text-align:left; margin: 1em 1em 1em 0; background: #f9f9f9; border: 1px #aaa solid; border-collapse: collapse;"
! Parameter
! Value                     
! Description
! Comment (literature, derived?)
|-
| k<sub>1</sub>
| x [units]
| max. transcription rate of constitutive promoter (pTET)
| Estimate
|-
| k<sub>2</sub>
|
|
|
|-
| k<sub>3</sub>
|
|
|
|-
| k<sub>4</sub>
|
|
|
|-
| k<sub>5</sub>
|
|
|
|-
| k<sub>6</sub>
| x [units]
|
|
|-
| <math> \delta_{GFP} </math>
| 0.029 hrs <sup>-1</sup>
| degradation rate of GFP
| Literature <font color = red> ~~ give reference </font>
|-
| <math> \delta_{LuxR} </math>
| x [units]
| degradation rate of LuxR
|
|-
| <math> \delta_{AHL} </math>
| x [units]
| degradation rate of AHL
|
|}
<br>
<br><br>
The system of equations for the two constructs varies strictly with respect to the value of the parameter k1. Construct 1 possesses a non-zero k1 rate constant, whereas for construct 2, a zero value is assumed.


==Generalities of the Model==
==Generalities of the Model==

Latest revision as of 18:00, 21 October 2007

Model Development for Infector Detector

Formulation of the problem

As described earlier, Infector Detector (ID) is a simple biological detector, which serves to expose bacterial biofilm. It functions by exploiting the inherent AHL production employed by the quorum-sensing bacteria, in the formation of such structures.

~~Insert diagram illustrating this phenomenon

Our project attempts to improve where previous methods of biofilm detection have proven ineffective: first and foremost, by focussing on the sensitivity of the system, to low levels of AHL production (bacterial chatter). In doing so, a complete investigation of the level of sensitivity to [AHL] needs to be performed - in other words, what is the minimal [AHL] for appreciable expression of reporter protein. Furthermore, establish a functional range for AHL detection. How does increased [AHL] impact on maximal output of reporter protein?
Also, how can the system performance be tailored, by exploiting the remaining state variables (e.g. varying initial [LuxR] and/or [pLux]).

The system performance here revolves most importantly around AHL sensitivity; however, the effect on, maximal output of fluorescent reporter protein and/or response time is, likewise, of great importance.

Our approach, involves the proposal of two simple constructs, varying with respect to the manner in which LuxR is introduced into the system:

  • Construct 1 - represented by T9002, incorporates constitutive expression of LuxR by pTET.
  • Construct 2 - simpler in nature, lacks pTET; LuxR is introduced in purified form here.

~~Here explain briefly why Construct 2 was selected, i.e. we were concerned with the time the system would take to reach steady-state (that is before energy-dependence was considered) - due to almost negligible [math]\displaystyle{ \delta_{LuxR} }[/math], etc .

Selection of model structure

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. 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.

In adopting this approach, we perform the following assumptions:

Assumptions

  • Ignore spatial information of the system; we ignore molecular dynamics of the system - this is a kinetic model.
  • Keep track of total number of molecules of each type - by tracking the concentrations of these state variables (as a continuous variable)
  • System is homogeneous - well-stirred, so that the molecules of each type are spread uniformly throughout the spatial domain. In doing so, we assume thermal equilibrium
  • Volume of the spatial domain remains constant


The system kinetics are determined by the following six coupled-ODEs.

Establishing a representative model

  • Introduction

We can condition the system in various manners, but for the purposes of our project, Infector Detector, we will seek a formulation which is valid for both constructs considered.

Our initial approach assumed that energy would be in unlimited supply, and that our system would eventually reach steady-state (Model 1). Experimentation suggested otherwise; our system needed to be amended. This lead to the development of model 2, an energy-dependent network, where the dependence on energy assumed Hill-like dynamics:

Model 1: Steady-state is attained; limitless energy supply (link here to derivation)


[math]\displaystyle{ \frac{d[LuxR]}{dt} = k_1 + k_3[A] - k2[LuxR][AHL]- \delta_{LuxR}[LuxR] }[/math]


[math]\displaystyle{ \frac{d[AHL]}{dt} = k_3[A] - k2[LuxR][AHL]- \delta_{AHL}[AHL] }[/math]

[math]\displaystyle{ \frac{d[A]}{dt} = -k_3[A] + k2[LuxR][AHL]- k_4[A][P] + k_5[AP] }[/math]

[math]\displaystyle{ \frac{d[P]}{dt} = -k_4[A][P] + k_5[AP] }[/math]

[math]\displaystyle{ \frac{d[AP]}{dt} = k_4[A][P] - k_5[AP] }[/math]

[math]\displaystyle{ \frac{d[GFP]}{dt} = k_6[AP] - \delta_{GFP}[GFP] }[/math]

Model 2: Equations developed through steady-state analysis; however due to limited energy supply, we operate in the transient regime


[math]\displaystyle{ \frac{d[LuxR]}{dt} = k_1\bigg(\frac{[E]^n}{K_E^n + [E]^n}\bigg) + k_3[A] - k_2[LuxR][AHL]- \delta_{LuxR}[LuxR] }[/math]
[math]\displaystyle{ \frac{d[AHL]}{dt} = k_3[A] - k_2[LuxR][AHL]- \delta_{AHL}[AHL] }[/math]

[math]\displaystyle{ \frac{d[A]}{dt} = -k_3[A] + k_2[LuxR][AHL]- k_4[A][P] + k_5[AP] }[/math]

[math]\displaystyle{ \frac{d[P]}{dt} = -k_4[A][P] + k_5[AP] }[/math]

[math]\displaystyle{ \frac{d[AP]}{dt} = k_4[A][P] - k_5[AP] }[/math]

[math]\displaystyle{ \frac{d[GFP]}{dt} = k_6[AP]\bigg(\frac{[E]^n}{K_E^n + [E]^n}\bigg) - \delta_{GFP}[GFP] }[/math]

[math]\displaystyle{ \frac{d[E]}{dt} = -\alpha_{1}k_1\bigg(\frac{[E]^n}{K_E^n + [E]^n}\bigg) - \alpha_{2}k_6[AP]\bigg(\frac{[E]^n}{K_E^n + [E]^n}\bigg) }[/math]


where:

[A] represents the concentration of AHL-LuxR complex
[P] represents the concentration of pLux promoters
[AP] represents the concentration of A-Promoter complex
k1, k2, k3, k4, k5, k6 are the rate constants associated with the relevant forward and backward reactions
[math]\displaystyle{ \alpha_i \ }[/math] represents the energy consumption due to gene transcription. It is a function of gene length.
n is the positive co-operativity coefficient (Hill-coefficient)
[math]\displaystyle{ K_E \ }[/math] the half-saturation coefficient

State Variables

Create similar table for state variables, as for parameter table below

Model Parameters

Populate parameters table

Parameter Value Description Comment (literature, derived?)
k1 x [units] max. transcription rate of constitutive promoter (pTET) Estimate
k2
k3
k4
k5
k6 x [units]
[math]\displaystyle{ \delta_{GFP} }[/math] 0.029 hrs -1 degradation rate of GFP Literature ~~ give reference
[math]\displaystyle{ \delta_{LuxR} }[/math] x [units] degradation rate of LuxR
[math]\displaystyle{ \delta_{AHL} }[/math] x [units] degradation rate of AHL




The system of equations for the two constructs varies strictly with respect to the value of the parameter k1. Construct 1 possesses a non-zero k1 rate constant, whereas for construct 2, a zero value is assumed.

Generalities of the Model

Simulations

Sensitivity Analysis