Team:LCG-UNAM-Mexico/Notebook/2008-October

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          <td class="subHeader" bgcolor="#99CC66" id="01">2008-10-01 </td>
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        <tr>
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<td class="bodyText"><div align="justify"><strong>WET LAB</strong>
 +
<p>We   used 18 tubes with 5ml of liquid   LBAm100 and  one control to grew  the 18 samples that we streaked yesterday from the pJET/rcnA clones.<br />
 +
  At the afternoon  we extracted the pJET/rcnA plasmids from the  18 clones using the  Alkaline Lysis  protocol.<br />
 +
  We load the plasmidic DNA from the  18 pJET/rcnA samples in a 1% agarose gel and ran them 1hr at 100volts.<br />
 +
<img src="https://static.igem.org/mediawiki/2008/d/d7/Nene21008.png" width="400" alt="Nene_II" /></p></div></td>
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           <td class="subHeader" bgcolor="#99CC66" id="02">2008-10-02</td>  
           <td class="subHeader" bgcolor="#99CC66" id="02">2008-10-02</td>  
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<td class="bodyText"><p><strong id="j4px2"><br />
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<td class="bodyText"><p>
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</strong>
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<p align="center"> <div align="justify"><strong><u>MODELING:</u></strong> </p>Hill Kinetics:<br>
-
<p align="center"> <strong>Hill Kinetics</strong> </p>
+
<p>REFERENCE: Irwin H. Segel's <i>Enzyme kinetics: Behaviour and Analysis of rapid equilibrium and Steady-state Enzyme systems</i>. </p>
-
<p> <strong>REFERENCE: <em>Segel; Enzyme kinetics: Behaviour and Analysis of rapid equilibrium and Steady-state Enzyme systems</em>.</strong> </p>
+
<p> <strong>Multiple Inhibition Analysis</strong> </p><br>
-
<p> <strong>Multiple Inhibition Analysis</strong> </p>
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<div id="mjrt"><img src="https://static.igem.org/mediawiki/2008/6/63/Kinetics-Pollo1.jpg" /></div>
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<p> </p>
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<p>&nbsp; </p>
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<div id="mjrt"><img src="http://docs.google.com/File?id=dntmktb_107gd4vzj6p_b" /></div>
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<br />
<br />
</p>
</p>
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   v/[Et]=([S]/Ks)kp/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks))                        <br />
   v/[Et]=([S]/Ks)kp/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks))                        <br />
   v=([S]/Ks)kp[Et]/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks))=([S]/Ks)Vmax/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks)) </p>
   v=([S]/Ks)kp[Et]/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks))=([S]/Ks)Vmax/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks)) </p>
-
<p> <strong>…with cooperativity     <br />
+
<p> <i>With cooperativity:     <br />
-
   </strong>v=([S]/Ks)Vmax/(1+2([I]/Ki)+([I]2/aKi2)+([S]/Ks))  <br />
+
   </i>v=([S]/Ks)Vmax/(1+2([I]/Ki)+([I]2/aKi2)+([S]/Ks))  <br />
-
   <em>* a factor</em> </p>
+
   <span class="font-size: small">*a factor<br></span> </p>
<p> It can be written in Hill's terms (if the cooperativity is strong).  </p>
<p> It can be written in Hill's terms (if the cooperativity is strong).  </p>
-
<p> <strong>System: </strong> cI repression</p>
+
<p> <i>System: </i> cI repression</p>
-
<p> <strong>Inhibitor:</strong>        cI:cI      (I)        <br />
+
<p> <i>Inhibitor:</i>        cI:cI      (I)        <br />
-
     <strong>“Enzyme”:       </strong>ρ          (ρ)        <br />
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     <i>“Enzyme”:       </i>ρ          (ρ)        <br />
-
     <strong>Substrate:          </strong>-           <br />
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     <i>Substrate:          </i>-           <br />
-
     <strong>Product:        </strong>RcnA     (P) </p>
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     <i>Product:        </i>RcnA     (P) </p>
-
<p> <strong>Union sites:         </strong>OR2 &amp; OR1          <br />
+
<p> <i>Binding sites:         </i>OR2 &amp; OR1          <br />
   I in OR1             -&gt;         ρI         <br />
   I in OR1             -&gt;         ρI         <br />
   I in OR2             -&gt;         Iρ </p>
   I in OR2             -&gt;         Iρ </p>
<p>  </p>
<p>  </p>
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<div id="ce:j"><img src="http://docs.google.com/File?id=dntmktb_108263t8wmw_b" /></div>
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<div id="ce:j"><img src="https://static.igem.org/mediawiki/2008/3/3e/Kinetics-Pollo2.jpg" /></div>
</p>
</p>
<p> </p>
<p> </p>
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   v/[ρt]= kp/(1+([I]/K5-1)+([I]/K5-2)+([I]2/K5))         <br />
   v/[ρt]= kp/(1+([I]/K5-1)+([I]/K5-2)+([I]2/K5))         <br />
   v= kp[ρt]/(1+([I]/K5-1)+([I]/K5-2)+([I]2/K5)) </p>
   v= kp[ρt]/(1+([I]/K5-1)+([I]/K5-2)+([I]2/K5)) </p>
-
<p> <strong>NOTE:</strong> We are ommiting the fact that cI:cI will be &quot;kidnapped&quot; by the promotor. This doesn't seem important since we only have 10 molecules of the promoter per cell, comparing with 150 basal molecules (without the AHL signal) of the dimer.</p>
+
<p> NOTE: We are not considering the fact that cI:cI will be sequestered by the promotor. This doesn't seem important since we only have 10 molecules of the promoter per cell, compared with 150 cI:cI molecules (without the AHL signal).</p>
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<p>&nbsp;</p>
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<p><strong>WET LAB</strong></p>
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         </td>
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<p>From the 18 samples we ran on the  gel only 8 were useful because they were between 3.5 and 4Kbp. (pJET/rcnA  should have 3874bp)..<br />
 +
  We used the samples : 2,4,6,9,10,  12,14,18 and double-digested them all night at 37°C using XbaI and HindIII  restriction enzymes; we also double-digested the pBBR1MCS-5  vector using the same restriction enzymes  mentioned before.</p>
 +
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<td class="bodyText"><p>&nbsp;</p>
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<td class="bodyText"><div align="justify">
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<p> <strong>Estimating the amount of AiiA per cell</strong> </p>
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<p> <strong><u>MODELING:</u></strong> </p>Estimating the amount of AiiA per cell:<br>
<p>  AiiA  is under the control of the lac promoter. The transcription and mRNA  degradation rates help us estimate the amount of mRNA present on the  cell. </p>
<p>  AiiA  is under the control of the lac promoter. The transcription and mRNA  degradation rates help us estimate the amount of mRNA present on the  cell. </p>
<p>    “The  half-life of protein A is assumed to be around 10 minutes which is  similar to what is used in Elowitz’s repressilator model [1].  Furthermore, we assume that a more aggressive degradation tail can  enable half-times on the order of two minutes for protein B.” </p>
<p>    “The  half-life of protein A is assumed to be around 10 minutes which is  similar to what is used in Elowitz’s repressilator model [1].  Furthermore, we assume that a more aggressive degradation tail can  enable half-times on the order of two minutes for protein B.” </p>
-
<p> Modeling the Lux/AiiA Relaxation Oscillator </p>
+
<p> Modeling the Lux/AiiA Relaxation Oscillator by Christopher Batten </p>
-
<p> Christopher Batten </p>
+
<p> In the paper AiiA is called protein B. Therefore the degradation rate for AiiA with an aggressive degradation tail is 0.0058/s. This would give us a lower limit. </p>
-
<p> In the paper AiiA is called protein B. Therefore the degradation rate for AiiA with an aggressive degradation tail is 0.0058 <em>s</em>-1. This would give us a lower limit. </p>
+
<p> Transcription initiation rate, km </p>
-
<p> “Transcription initiation rate, km </p>
+
<p> Malan et al. (1984) measured the transcription initiation rate at P1 and report the following value: km ≈ 0.18min-1 </p>
<p> Malan et al. (1984) measured the transcription initiation rate at P1 and report the following value: km ≈ 0.18min-1 </p>
<p>  mRNA degradation rate, jM </p>
<p>  mRNA degradation rate, jM </p>
-
<p> Kennell and Riezman (1977), measured a lacZ mRNA half-life of 1.5 min: ξM = 0.46min-1 </p>
+
<p> Kennell and Riezman (1977), measured a lacZ mRNA half-life of 1.5 min: ξM = 0.46/min </p>
<p>  lacZ mRNA translation initiation rate, кB </p>
<p>  lacZ mRNA translation initiation rate, кB </p>
-
<p> From  Kennell and Riezman (1977), translation starts every 3.2 s at the lacZ  mRNA. This leads to the following translation initiation rate: кB ≈ 18.8min-1” </p>
+
<p> From  Kennell and Riezman (1977), translation starts every 3.2 s at the lacZ  mRNA. This leads to the following translation initiation rate: кB ≈ 18.8/min </p>
<p> Santillán  M. and Mackey M. C. (2004). Influence of Catabolite Repression and  Inducer Exclusion on the Bistable Behavior of the lac Operon. Biophys J  86:1282–1292 </p>
<p> Santillán  M. and Mackey M. C. (2004). Influence of Catabolite Repression and  Inducer Exclusion on the Bistable Behavior of the lac Operon. Biophys J  86:1282–1292 </p>
-
<p> We  modified both transcription initiation and translation rates by  multiplying both rates by 4. This due to the fact that LuxR is a four  times smaller than LacZ: </p>
 
-
<p> LacZ has a length of 1024 aa </p>
 
-
<p> LuxR has a length of 250 aa </p>
 
<p> Simulating with simbiology, AiiA reaches stationary state at almost 3500 molecules per cell. </p>
<p> Simulating with simbiology, AiiA reaches stationary state at almost 3500 molecules per cell. </p>
-
<p>&nbsp;</p>
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<strong>WET LAB</strong>
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         </td>
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<p>We inactivated the enzymes by  putting them  at 65°C for 20min, Then we loaded  them into an 1% agarose gel and ran them for about 1hr  at 100volts.<br />
 +
  <img src="https://static.igem.org/mediawiki/2008/8/8c/Nene31008.png" alt="Nene_III" width="400" /><br />
 +
  We prepared a 1% low melting point  agarose Gel in order to cut from it the rcnA bands that we obtained by  double-digesting the pJET/rcnA plasmid.<br />
 +
  <img src="https://static.igem.org/mediawiki/2008/e/ea/31008purif.png" alt="Nene_iV" width="250" /><br />
 +
  pJET/rcnA(sample 6) 0.2418g<br />
 +
  pJET/rcnA(sample 12) 0.1872g<br />
 +
  We purified the gel band using the <strong>QIAquick  Gel Extraction Kit.</strong> <br />
 +
  After that we proceeded to ligate the pBBR1MCS-5  vector with the purified rcnA fragment using the <strong>Fermentas Rapid DNA  ligation kit.</strong> <br />
 +
  We left the ligation reaction at the  20°C room  the complete weekend.</p>
 +
         </div></td>
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<tr>
<tr>
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           <td class="subHeader" bgcolor="#99CC66" id="17">2008-10-17</td>  
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           <td class="subHeader" bgcolor="#99CC66" id="06">2008-10-06</td>  
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<td class="bodyText"><p>&nbsp;</p>
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<td class="bodyText"><div align="justify"><strong>WET LAB</strong>
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<p><strong>Stechiometric Matrix</strong></p>
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<p>We use the  ligated samples of pBBR1MCS-5/rcnA to  transform E.coli TOP10 by electroporation.<br />
 +
  We grew for 1hr the electroporated  cells in  1ml of LB at 37°C. We plated the growth  cells on a LB Gm20 agar plate .</p></div></td>
 +
        </tr> 
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<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="07">2008-10-07</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><strong>WET LAB</strong>
 +
<p>We streaked 4 LBGm20 agar plates  with different TOP10/pBBR1MCS-5-rcnA colonies, which were taken from the plates  that we made yesterday and let them grow all night.</p></div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="09">2008-10-09</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><strong>WET LAB</strong>
 +
<p>We took 3 samples from the  TOP10/pBBR1MCS-5-rcnA plates and put them into 3 tubes with 3ml of Liquid  LBGm20.<br />
 +
  We used the  <strong>Roche  Pasmid DNA extraction Kit </strong> in order  to obtain the pBBR1MCs-5 vector with rcnA.</p></div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="10">2008-10-10</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"> <strong>WET LAB</strong>
 +
<p>We ran a 1% agarose gel to verify  the extraction.<br />
 +
  <img src="https://static.igem.org/mediawiki/2008/7/7a/Extraccion_nene_1010108.jpg" alt="NENE_V" width="400" /><br />
 +
  The vector with rcnA was  double-digested in order to verify the correct ligation of the fragments.<br />
 +
  A 1% agarose gel was made to see the  digested vector.<br />
 +
  <img src="https://static.igem.org/mediawiki/2008/5/5b/101008_rcnArest_plasmido_bueno.PNG" alt="Gel enen" width="247" height="349" /><br />
 +
  The pBBR1MCs-5/rcnA was used to transform  W3110/YohM- competent cells by Heat shock. The transformed cells were plated on  LBGm20 agar plates and incubated at 37°C the whole night.</p></div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="11">2008-10-11</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><p><strong>WET LAB</strong></p>
 +
<p>The   W3110/YohM-/pBBR1MCs-5/rcnA colonies were streaked on LBGm20 agar plates  and incubated the whole night at 37°C.<br />
 +
  The planning for the measurements was completed and ready to start. &nbsp;<br />
 +
  The propose for  the determination of nickel internalization considerates to assume that when  the medium has certain nickel concentration, the presence of cells from  different strains will cause a variation in the resistivity(which, by the way  will affect conductivity). For the different strains that we are using, we  expect: </p>
 +
<table border="1" cellspacing="0" cellpadding="0">
 +
  <tr>
 +
    <td width="272" valign="top"><p>Strain </p></td>
 +
    <td width="440" valign="top"><p>Changes expected </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td width="272" valign="top"><p>W3110 / YohM- </p></td>
 +
    <td width="440" valign="top"><p>As this strain    doesn’t carry the efflux pump RcnA. We expect&nbsp; that the resistivity will    increase due to the nickel internalization. </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td width="272" valign="top"><p>W3110 / YohM- pBBIMRCS-5 </p></td>
 +
    <td width="440" valign="top"><p>We expect a    similar performance of these cells compared with W3110 / YohM-. However the    extrusion pump for gentamicine present in the plasmid could be adding    variation to the system. </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td width="272" valign="top"><p>W3110 / YohM- pBBIMRCS-5 RcnA </p></td>
 +
    <td width="440" valign="top"><p>This cells carry    the pBBIMRCS-5 plasmid with the efflux pump RcnA. Here, we expect    oscillations due to the presence of a pump which internalizes nickel and the    efflux pump. </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td width="272" valign="top"><p>W3110 / YohM+ </p></td>
 +
    <td width="440" valign="top"><p>We expect a    similar behavior to the one observed in W3110 / YohM- pBBIMRCS-5 RcnA. </p></td>
 +
  </tr>
 +
</table>
 +
<p>The two known  critical concentrations of NiSO4 are 2.2 mM, the minimum inhibitory, and 500uM the minimun  needed to repress RcnR activity. <br />
 +
  Planned  methodology: <br />
 +
  -Establishment of  a place to do the measurements. <br />
 +
  &nbsp; -We expect  to have a constant temperature during the measurement process. <br />
 +
  -Test the sensitivity of the measurement &nbsp;dispositive. To achieve this,  measurements will be done in agitation of: </p>
 +
<ul>
 +
  <ul>
 +
    <ul>
 +
      <ul>
 +
        <li>Just LB </li>
 +
        <li>LB with NiSO4 </li>
 +
        <li>LB with cells </li>
 +
      </ul>
 +
    </ul>
 +
  </ul>
 +
</ul>
 +
<p>&nbsp;</p>
 +
<div align="center">
 +
  <table border="1" cellspacing="0" cellpadding="0" width="273">
 +
    <tr>
 +
      <td width="50%"><p>Molarity</p></td>
 +
      <td width="49%"><p>NiSO4 μl&nbsp; from a solution 0.1M</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>0,0022 </p></td>
 +
      <td width="49%"><p>22</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>0,001 </p></td>
 +
      <td width="49%"><p>10</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>0,0001 </p></td>
 +
      <td width="49%"><p>1</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>0,00001 </p></td>
 +
      <td width="49%"><p>10</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>0,000001 </p></td>
 +
      <td width="49%"><p>1</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>0,0000001 </p></td>
 +
      <td width="49%"><p>10</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>0,00000001 </p></td>
 +
      <td width="49%"><p>1</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>0,000000001 </p></td>
 +
      <td width="49%"><p>10</p></td>
 +
    </tr>
 +
    <tr>
 +
      <td width="50%"><p>1E-10 </p></td>
 +
      <td width="49%"><p>1</p></td>
 +
    </tr>
 +
  </table>
 +
</div>
 +
<ul>
 +
  <ul>
 +
    <ul>
 +
      <ul>
 +
        <ul>
 +
          <li>(,001) Dilución de 10 microlitros de 0.1 M en 1 mililitro </li>
 +
          <li>(,00001) Dilución de 10 microlitros de 0.001M en 1  mililitro </li>
 +
          <li>(0,0000001) Dilución  de 10 microlitros de 0.00001  M en un mililitro </li>
 +
        </ul>
 +
      </ul>
 +
    </ul>
 +
  </ul>
 +
</ul>
 +
<p>Internalization </p>
 +
<p>-Grow the strain  YohM- in LB medium until reach an OD(optical density) of 0.4 to ensure that the  cells are in exponential phase. (Later this was changed to an OD of 0.5 at a  lambda of 600nm). </p>
 +
<p>-Plot  concentration vs&nbsp; time and calculate the slope <br />
 +
  slope= Internalization rate of Ni2+ </p>
 +
<p>Extrusion<br />
 +
  The following steps were  performed in order to prove the RcnA activity, and to get the enough data to  calculate conductivity&nbsp; from the resistivity measurements. These conductivity  data will be useful to get the extrusion rate of RcnA.</p>
 +
<p>-&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;  Grow the strains YohM-, YohM- + pBBMICS-5+RcnA, YohM- + pBBMICS-5 and YohM+ &nbsp;in LB medium until reach an OD(optical density) of  0.4 to ensure that the cells are in exponential phase. (Later this was changed  to an OD of 0.5 at a lambda of 600nm).<br />
 +
  -&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;  Take 1ml&nbsp; from each culture for each of the next nickel  concentrations: </p>
 +
<table border="1" cellspacing="0" cellpadding="0" align="left">
 +
  <tr>
 +
    <td valign="top"><p>Molarity</p></td>
 +
    <td valign="top"><p>Grams</p></td>
 +
    <td valign="top"><p>Conductivity</p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>0,0022&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>0,3404368&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>3,4375E-06 </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>0,001&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>0,154744&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,5625E-06 </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>0,0001&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>0,0154744&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,5625E-07 </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>0,00001&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>0,00154744&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,5625E-08 </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>0,000001&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>0,000154744&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,5625E-09 </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>0,0000001&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,54744E-05&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,5625E-10 </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>0,00000001&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,54744E-06&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,5625E-11 </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>0,000000001&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,54744E-07&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,5625E-12 </p></td>
 +
  </tr>
 +
  <tr>
 +
    <td valign="top"><p>1E-10&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,54744E-08&nbsp;&nbsp;&nbsp; </p></td>
 +
    <td valign="top"><p>1,5625E-13 </p></td>
 +
  </tr>
 +
</table>
 +
<p><br clear="all" />
 +
    <br />
 +
  - The measurements will be  performed during three minutes for each one strain</p></div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="12">2008-10-12</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"> <p> <strong>WET LAB</strong><br />
 +
  Some measurements were done in LB with and without nickel in order to  calibrate and prove the apparatus. Initially the measurement dispositive  included a gold electrode which seemed to be working properly.</p>
 +
</div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="13">2008-10-13</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><p><strong>WET LAB</strong></p>
 +
<p>Solutions nickel 500uM and without nickel at all were prepared from samples  of LB, and the strains YohM-, YohM- + pBBIMRCS-5 and YohM- + pBBIMRCS-5 + RcnA. </p>
 +
</div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="14">2008-10-14</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><p><strong>WET LAB</strong><br />
 +
The OD that the cells must reach was changed to 0.5 at a lambda of  600nm(This was due to the finding of the proper OD measurement in the strain  W3110). <br />
 +
Some adjusts were done to the measurement dispositive in order to increase  its sensibility.</p>
 +
</div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="15">2008-10-15</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><p><strong>WET LAB</strong><br />
 +
Preparation of the strains YohM-, YohM- + pBBIMRCS-5, and YohM- +  pBBIMRCS-5 + RcnA for the measurements. An overnight of each strain was grown  in LB. Samples of YohM- + pBBIMRCS-5, and YohM- + pBBIMRCS-5 + RcnA were  prepared with different concentrations of NiSO4 . That  concentrations includes a gradient from 1x10-3 M – 1X10-10M. And the two critical  concentrations 500uM and 2.2mM.</p>
 +
</div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="16">2008-10-16</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><p><strong>WET LAB</strong><br />
 +
Strains were prepared in pursuit to perform some new measurements. Samples  of LB, LB+ sulfate, and YohM-+RCNA+PBB were read. <br />
 +
Measurement intervals (100 milliseconds) semeed to be quite large, so its  correction was proposed. </p>
 +
</div></td>
 +
        </tr> 
 +
 
 +
 
 +
 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="17"><a name="oct17"></a>2008-10-17</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify">
 +
<p><strong><u>MODELING:</u></strong></p>Stoichiometric Matrix:<br>
<p> <em>Palsson, 2006</em></p>
<p> <em>Palsson, 2006</em></p>
<p>Flux vector                   -&gt;         <strong>v</strong>=(v1, v2, …, vn) <br />
<p>Flux vector                   -&gt;         <strong>v</strong>=(v1, v2, …, vn) <br />
Line 216: Line 480:
<p><strong>The  four fundamental subspaces</strong></p>
<p><strong>The  four fundamental subspaces</strong></p>
<p>&nbsp;</p>
<p>&nbsp;</p>
-
<strong>
+
<div id="q_q6"><img src="https://static.igem.org/mediawiki/2008/2/23/FromPalssonM1.jpg" width="500" /></div>
-
<div id="q_q6"><img src="http://docs.google.com/File?id=dntmktb_109dwhwh6dd_b" alt="" /></div>
+
<i>Image from Systems Biology: Properties of Reconstructed Networks by Bernhard O. Palsson</i>
<br />
<br />
-
</strong>
 
</p>
</p>
The vector produced by a linear transformation is in two orthogonal spaces  (the column and left null spaces), called the <em>domain</em>, and the vector being mapped is also in two orthogonal  spaces (the row and null spaces), called the <em>codomain</em> or the <em>range</em> of  the transformation.
The vector produced by a linear transformation is in two orthogonal spaces  (the column and left null spaces), called the <em>domain</em>, and the vector being mapped is also in two orthogonal  spaces (the row and null spaces), called the <em>codomain</em> or the <em>range</em> of  the transformation.
-
<p>The vectors in the left null space (<strong>l</strong><em>i</em>) represent a mass  conservation.</p>
+
<p>The vectors in the left null space (<i>l</i><em>i</em>) represent mass  conservation.</p>
<p>The flux vector can be decomposed into a  dynamic component and a steady-state component:      <br />
<p>The flux vector can be decomposed into a  dynamic component and a steady-state component:      <br />
   v = vdyn + vss</p>
   v = vdyn + vss</p>
-
<p>The steady state component satisfies Svss=0  and <strong>v</strong>ss is thus in the null space  of <strong>S.</strong></p>
+
<p>The steady state component satisfies Svss=0  and <i>v</si>ss is thus in the null space  of <i>S.</i></p>
-
<p>&nbsp;</p>
+
        </div></td>
-
        </td>
+
       </tr>   
       </tr>   
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="18">2008-10-18</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><p><strong>WET LAB</strong><br />
 +
Prosecution of correction of measurement intervals. </p></div></td>
 +
        </tr> 
 +
<tr>
 +
          <td class="subHeader" bgcolor="#99CC66" id="19">2008-10-19</td>
 +
        </tr>
 +
        <tr>
 +
<td class="bodyText"><div align="justify"><p>
 +
  <strong>WET LAB</strong><br />
 +
Due to the great variation observed in the data, some aspects of the  samples, measurements and electrodes were reconsidered. As the variations could  be caused by the ions present in the medium it was proposed to use a buffer  instead of LB medium. </p></div></td>
 +
        </tr> 
 +
 +
<tr>
<tr>
           <td class="subHeader" bgcolor="#99CC66" id="20">2008-10-20</td>  
           <td class="subHeader" bgcolor="#99CC66" id="20">2008-10-20</td>  
         </tr>
         </tr>
         <tr>
         <tr>
-
<td class="bodyText"><p>&nbsp;</p>
+
<td class="bodyText"><div align="justify">
-
<p>The higher the number of independent reaction  vectors, the smaller the orthogonal left null space. The higher the number of independent  reactions, the fewer conservation quantities exist.</p>
+
<b><u>MODELING:</u></b><br>
-
<p> <strong>FUNDAMENTAL SUBSPACES OF S</strong></p>
+
<p>The higher the number of independent reaction  vectors, the smaller the orthogonal left null space. The higher the number of independent  reactions, the fewer the conservation quantities exist.</p>
 +
<p> <b>FUNDAMENTAL SUBSPACES OF S</b></p>
<p>The dimensions  of both the column and row space is r (<em>rank</em>;  number of linearly independent rows and columns that the matrix contains).          <br />
<p>The dimensions  of both the column and row space is r (<em>rank</em>;  number of linearly independent rows and columns that the matrix contains).          <br />
   dim(Col(S))  = dim(Row(S)) = r    <br />
   dim(Col(S))  = dim(Row(S)) = r    <br />
Line 242: Line 522:
   Similarly, the flux vector is n-dimensional; thus,  <br />
   Similarly, the flux vector is n-dimensional; thus,  <br />
   dim(Null(S))  = n – r</p>
   dim(Null(S))  = n – r</p>
-
<p><img alt="*" width="11" height="11" />       <em>Null space</em>. The null space of <strong>S </strong>contains all the steady-state flux  distributions allowable in the network. The steady state is of much interest  since most homeostatic states are close to being steady states.</p>
+
<p><li>       <em>Null space</em>. The null space of <i>S </i>contains all the steady-state flux  distributions allowable in the network. The steady state is of much interest  since most homeostatic states are close to being steady states.</li></p>
-
<p><img alt="*" width="11" height="11" />       <em>Row space</em>. The row space of <strong>S </strong>contains all the dynamic flux distributions of  a network and thus the thermodynamic driving forces that change the rate of  reaction activity.</p>
+
<p><li>       <em>Row space</em>. The row space of <i>S </i>contains all the dynamic flux distributions of  a network and thus the thermodynamic driving forces that change the rate of  reaction activity. </li></p>
-
<p><img alt="*" width="11" height="11" />       <em>Left null space</em>. The left null space of <strong>S </strong>contains all the  conservation relationships, or <em>time invariants</em>, that a network contains. The sum of conserved  metabolites or conserved metabolic pools do not change with time and are combinations  of concentration variables.</p>
+
<p><li>       <em>Left null space</em>. The left null space of <i>S </i>contains all the  conservation relationships, or <em>time invariants</em>, that a network contains. The sum of conserved  metabolites or conserved metabolic pools do not change with time and are combinations  of concentration variables.</li></p>
-
<p><img alt="*" width="11" height="11" />       <em>Column space</em>. The column space of <strong>S </strong>contains all the possible  time derivatives of the concentration vector and thus shows how the  thermodynamic driving forces move the concentration state of the network.</p>
+
<p><li>       <em>Column space</em>. The column space of <i>S </i>contains all the possible  time derivatives of the concentration vector and thus shows how the  thermodynamic driving forces move the concentration state of the network.</li></p>
<p><strong>Singular Value Decomposition</strong></p>
<p><strong>Singular Value Decomposition</strong></p>
<p>SVD states that for a matrix S of  dimension m× n and of rank r, there are orthonormal matrices U (of dimension m  ×m) and V (of dimension n × n) and a matrix with diagonal elements ∑ = diag(σ1,  σ2, ... , σr ) with σ1 ≥ σ2 ≥ ··· ≥  σr &gt; 0 such that S = U∑VT</p>
<p>SVD states that for a matrix S of  dimension m× n and of rank r, there are orthonormal matrices U (of dimension m  ×m) and V (of dimension n × n) and a matrix with diagonal elements ∑ = diag(σ1,  σ2, ... , σr ) with σ1 ≥ σ2 ≥ ··· ≥  σr &gt; 0 such that S = U∑VT</p>
-
<p>A non-negative real number σ is a <strong>singular value</strong> for <em>M</em> if and only if there exist unit-length vectors <em>u</em> in <em>Km</em> and <em>v</em> in <em>Kn</em> such that            <br />
+
<p>A non-negative real number σ is a <i>singular value</i> for <em>M</em> if and only if there exist unit-length vectors <em>u</em> in <em>Km</em> and <em>v</em> in <em>Kn</em> such that            <br />
   Mv=σu and M*u=σv<br />
   Mv=σu and M*u=σv<br />
-
   The vectors <em>u</em> and <em>v</em> are called <strong>left-singular</strong> and <strong>right-singular  vectors</strong> for σ, respectively.        <br />
+
   The vectors <em>u</em> and <em>v</em> are called <i>left-singular</i> and <i>right-singular  vectors</i> for σ, respectively.        <br />
   In any singular value decomposition        <br />
   In any singular value decomposition        <br />
   M=UΣV*<br />
   M=UΣV*<br />
   the diagonal entries of Σ are necessarily equal to the singular values of <em>M</em>. The columns  of <em>U</em> and <em>V</em> are, respectively, left- and right-singular vectors  for the corresponding singular values.</p>
   the diagonal entries of Σ are necessarily equal to the singular values of <em>M</em>. The columns  of <em>U</em> and <em>V</em> are, respectively, left- and right-singular vectors  for the corresponding singular values.</p>
<p></p>
<p></p>
-
<div id="vnuf"><img src="http://docs.google.com/File?id=dntmktb_110hsrd79d6_b" /></div>
+
<div id="vnuf"><img src="https://static.igem.org/mediawiki/2008/b/bf/FromPalssonM2.jpg" width="500"/></div>
-
<div id="jlkw"><img src="http://docs.google.com/File?id=dntmktb_111frgwdrmp_b" /></div>
+
<i>Image from Systems Biology: Properties of Reconstructed Networks by Bernhard O. Palsson</i>
 +
<div id="jlkw"><img src="https://static.igem.org/mediawiki/2008/8/86/FromPalssonM3.jpg" width="500" height="280"/></div>
 +
<i>Image from Systems Biology: Properties of Reconstructed Networks by Bernhard O. Palsson</i>
</p>
</p>
-
<p> The columns of <strong>U </strong>are called the <em>left singular vectors </em>and the columns of <strong>V </strong>are the <em>right singular  vectors</em>. The columns of <strong>U </strong>and <strong>V </strong>give orthonormal bases for  all the four fundamental subspaces of <strong>S </strong>(see  Figure 8.3). The first <em>r </em>columns of <strong>U </strong>and <strong>V </strong>give orthonormal bases for  the column and row spaces, respectively. The last<em>m</em>− <em>r </em>columns of <strong>U </strong>give an  orthonormal basis for the left null space, and the last <em>n </em>− <em>r </em>columns or <strong>V </strong>give an  orthonormal basis for the null space.</p>
+
<p> The columns of <i>U </i>are called the <em>left singular vectors </em>and the columns of <i>V </i>are the <em>right singular  vectors</em>. The columns of <i>U </i>and <i>V </i>give orthonormal bases for  all the four fundamental subspaces of <i>S </i>(see  Figure 8.3). The first <em>r </em> columns of <i>U </i>and <i>V </i>give orthonormal bases for  the column and row spaces, respectively. The last<em>m</em>− <em>r </em>columns of <i>U </i>give an  orthonormal basis for the left null space, and the last <em>n </em>− <em>r </em>columns or <i>V </i>give an  orthonormal basis for the null space.</p>
-
<p>&nbsp;</p>
+
<p><strong>WET LAB</strong><br />
-
        </td>
+
Correction of the measurement intervals to 1 millisecond. <br />
 +
161008 <br /></p>        </div></td>
       </tr>   
       </tr>   
<tr>
<tr>
Line 266: Line 549:
         </tr>
         </tr>
         <tr>
         <tr>
-
<td class="bodyText"><p>&nbsp;</p>
+
<td class="bodyText"><div align="justify">
 +
<b><u>MODELING:</u></b><br>
<p><strong>THE (RIGTH) NULL SPACE OF S</strong></p>
<p><strong>THE (RIGTH) NULL SPACE OF S</strong></p>
-
<p>The right null space of <strong>S </strong>is defined by     <br />
+
<p>The right null space of <i>S </i>is defined by     <br />
-
   <strong>Sv</strong>ss = <strong>0 <br />
+
   <i>Sv</i>ss = <i>0 <br />
-
</strong>Thus, all the steady-state  flux distributions, <strong>v</strong>ss, are found in the null space. The null space has a dimension of <em>n </em>− <em>r</em>. Note that <strong>v</strong>ss must be orthogonal to all  the rows of <strong>S </strong>simultaneously and thus represents  a linear combination of flux values on the reaction map that sum to zero.</p>
+
</i>Thus, all the steady-state  flux distributions, <strong>v</strong>ss, are found in the null space. The null space has a dimension of <em>n </em>− <em>r</em>. Note that <strong>v</strong>ss must be orthogonal to all  the rows of <strong>S </strong>simultaneously and thus represents  a linear combination of flux values on the reaction map that sum to zero.</p>
<p><strong>Mathematics  versus biology</strong> </p>
<p><strong>Mathematics  versus biology</strong> </p>
-
<p><img alt="*" width="11" height="11" />        The null space represents all the possible functional, or phenotypic, states  of a network.</p>
+
<p><li>        The null space represents all the possible functional, or phenotypic, states  of a network.</li></p>
-
<p><img alt="*" width="11" height="11" />        A particular point in the polytope represents one network function or one  particular phenotypic state.</p>
+
<p><li>        A particular point in the polytope represents one network function or one  particular phenotypic state.</li></p>
-
<p><img alt="*" width="11" height="11" />        As we will see in Chapter 16, there are equivalent points in the cone  that lead to the same overall functional state of a network. Biologically, such  conditions are called <em>silent phenotypes</em>.</p>
+
<p><li>        As we will see in Chapter 16, there are equivalent points in the cone  that lead to the same overall functional state of a network. Biologically, such  conditions are called <em>silent phenotypes</em>.</li></p>
-
<p><img alt="*" width="11" height="11" />        The edges of the flux cone are the unique extreme pathways. Any flux  state in the cone can be decomposed into the extreme pathways. The unique set  of extreme pathways thus gives a mathematical description of the range of flux  levels that are allowed.</p>
+
<p><li>        The edges of the flux cone are the unique extreme pathways. Any flux  state in the cone can be decomposed into the extreme pathways. The unique set  of extreme pathways thus gives a mathematical description of the range of flux  levels that are allowed.</li></p>
<p>- The stoichiometric matrix has a  null space that corresponds to a linear combination of the reaction vectors  that add up to zero; so-called link-neutral combinations.</p>
<p>- The stoichiometric matrix has a  null space that corresponds to a linear combination of the reaction vectors  that add up to zero; so-called link-neutral combinations.</p>
<p>- The orthonormal basis given by  SVD does not yield a useful biochemical interpretation of the null space of the  stoichiometric matrix.</p>
<p>- The orthonormal basis given by  SVD does not yield a useful biochemical interpretation of the null space of the  stoichiometric matrix.</p>
<p><strong>THE LEFT NULL SPACE OF S</strong></p>
<p><strong>THE LEFT NULL SPACE OF S</strong></p>
-
<p><u>As with the (right) null space, the  choice of basis for the left null</u><u> space is important  in describing its contents in biochemically and biologically meaningful terms.</u></p>
+
<p>As with the (right) null space, the  choice of basis for the left null space is important  in describing its contents in biochemically and biologically meaningful terms.</p>
<p>…may represent mass conservation…</p>
<p>…may represent mass conservation…</p>
<p> <strong>THE ROW AND COLUMN SPACE OF S</strong></p>
<p> <strong>THE ROW AND COLUMN SPACE OF S</strong></p>
<p>The column and row spaces of the  stoichiometric matrix contain the concentration time derivatives and the  thermodynamic driving forces, respectively.</p>
<p>The column and row spaces of the  stoichiometric matrix contain the concentration time derivatives and the  thermodynamic driving forces, respectively.</p>
-
<p>&nbsp;</p>
+
        </div></td>
-
        </td>
+
       </tr>   
       </tr>   
-
<tr>
 
-
          <td class="subHeader" bgcolor="#99CC66" id="__">2008-10-__</td>
 
-
        </tr>
 
         <tr>
         <tr>
<td class="bodyText"><p>-</p>
<td class="bodyText"><p>-</p>

Latest revision as of 02:44, 30 October 2008

LCG-UNAM-Mexico:Notebook/October

Header image
iGEM 2008 TEAM
line decor
  
line decor

 
 
 
 
 
 
October

2008-10-01
WET LAB

We  used 18 tubes with 5ml of liquid  LBAm100 and  one control to grew the 18 samples that we streaked yesterday from the pJET/rcnA clones.
At the afternoon  we extracted the pJET/rcnA plasmids from the 18 clones using the  Alkaline Lysis protocol.
We load the plasmidic DNA from the 18 pJET/rcnA samples in a 1% agarose gel and ran them 1hr at 100volts.
Nene_II

2008-10-02

MODELING:

Hill Kinetics:

REFERENCE: Irwin H. Segel's Enzyme kinetics: Behaviour and Analysis of rapid equilibrium and Steady-state Enzyme systems.

Multiple Inhibition Analysis



v = kp[ES]          ->         v/[Et]=kp[ES]/([E]+[IE]+[EI]+[IEI]+[ES])

Ks=[E][S]/[ES]   ->         [ES]=[E][S]/Ks  
Ki=[I][E]/[IE]     ->         [IE]=[I][E]/Ki    
Ki=[EI][I]/[IEI]   ->         [IEI]=[EI][I]/Ki=[I]2[E]/Ki2

v/[Et]=([E][S]/Ks)kp/([E]+([I][E]/Ki)+([E][I]/Ki)+([I]2[E]/Ki2)+([E][S]/Ks)) 
v/[Et]=([S]/Ks)kp/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks))                       
v=([S]/Ks)kp[Et]/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks))=([S]/Ks)Vmax/(1+2([I]/Ki)+([I]2/Ki2)+([S]/Ks))

With cooperativity:    
v=([S]/Ks)Vmax/(1+2([I]/Ki)+([I]2/aKi2)+([S]/Ks)) 
*a factor

It can be written in Hill's terms (if the cooperativity is strong). 

System: cI repression

Inhibitor:        cI:cI      (I)       
“Enzyme”:       ρ          (ρ)       
Substrate:          -          
Product:        RcnA     (P)

Binding sites:         OR2 & OR1         
I in OR1             ->         ρI        
I in OR2             ->         Iρ

 

K5-1=[I][ρ]/[ρI] 
K5-2=[I][ρ]/[Iρ] 
a & b cooperativity factor

* K5=[ρ][I]2/[IρI]

K5=K5-1·K5-2·a

ΔGº=ΔGº1+ ΔGº2+ ΔGº12

1/K5=exp(-ΔGº/RT)=exp(ΔGº1/RT)+ exp(ΔGº2/RT)+ exp(ΔGº12/RT)

ρI         ->         ΔGº1=-11.7 kcal/mol    
Iρ         ->         ΔGº2=-10.1 kcal/mol    
Coop.   ->         ΔGº12=-2 kcal/mol        
ΔGº =-23.8 kcal/mol

v=k6·ρ  
v/[ρt]=kp[ρ]/([ρ]+[Iρ]+[ρI]+[IρI])          
v/[ρt]=[ρ]kp/([ρ]+([ρ][I]/K5-1)+([I][ρ]/K5-2)+([I]2[ρ]/K52))
v/[ρt]= kp/(1+([I]/K5-1)+([I]/K5-2)+([I]2/K5))        
v= kp[ρt]/(1+([I]/K5-1)+([I]/K5-2)+([I]2/K5))

NOTE: We are not considering the fact that cI:cI will be sequestered by the promotor. This doesn't seem important since we only have 10 molecules of the promoter per cell, compared with 150 cI:cI molecules (without the AHL signal).

WET LAB

From the 18 samples we ran on the gel only 8 were useful because they were between 3.5 and 4Kbp. (pJET/rcnA should have 3874bp)..
We used the samples : 2,4,6,9,10, 12,14,18 and double-digested them all night at 37°C using XbaI and HindIII restriction enzymes; we also double-digested the pBBR1MCS-5  vector using the same restriction enzymes mentioned before.

2008-10-03

MODELING:

Estimating the amount of AiiA per cell:

AiiA is under the control of the lac promoter. The transcription and mRNA degradation rates help us estimate the amount of mRNA present on the cell.

“The half-life of protein A is assumed to be around 10 minutes which is similar to what is used in Elowitz’s repressilator model [1]. Furthermore, we assume that a more aggressive degradation tail can enable half-times on the order of two minutes for protein B.”

Modeling the Lux/AiiA Relaxation Oscillator by Christopher Batten

In the paper AiiA is called protein B. Therefore the degradation rate for AiiA with an aggressive degradation tail is 0.0058/s. This would give us a lower limit.

Transcription initiation rate, km

Malan et al. (1984) measured the transcription initiation rate at P1 and report the following value: km ≈ 0.18min-1

mRNA degradation rate, jM

Kennell and Riezman (1977), measured a lacZ mRNA half-life of 1.5 min: ξM = 0.46/min

lacZ mRNA translation initiation rate, кB

From Kennell and Riezman (1977), translation starts every 3.2 s at the lacZ mRNA. This leads to the following translation initiation rate: кB ≈ 18.8/min

Santillán M. and Mackey M. C. (2004). Influence of Catabolite Repression and Inducer Exclusion on the Bistable Behavior of the lac Operon. Biophys J 86:1282–1292

Simulating with simbiology, AiiA reaches stationary state at almost 3500 molecules per cell.

WET LAB

We inactivated the enzymes by putting them  at 65°C for 20min, Then we loaded them into an 1% agarose gel and ran them for about 1hr  at 100volts.
Nene_III
We prepared a 1% low melting point agarose Gel in order to cut from it the rcnA bands that we obtained by double-digesting the pJET/rcnA plasmid.
Nene_iV
pJET/rcnA(sample 6) 0.2418g
pJET/rcnA(sample 12) 0.1872g
We purified the gel band using the QIAquick Gel Extraction Kit.
After that we proceeded to ligate the pBBR1MCS-5 vector with the purified rcnA fragment using the Fermentas Rapid DNA ligation kit.
We left the ligation reaction at the 20°C room the complete weekend.

2008-10-06
WET LAB

We use the  ligated samples of pBBR1MCS-5/rcnA to transform E.coli TOP10 by electroporation.
We grew for 1hr the electroporated cells in  1ml of LB at 37°C. We plated the growth cells on a LB Gm20 agar plate .

2008-10-07
WET LAB

We streaked 4 LBGm20 agar plates with different TOP10/pBBR1MCS-5-rcnA colonies, which were taken from the plates that we made yesterday and let them grow all night.

2008-10-09
WET LAB

We took 3 samples from the TOP10/pBBR1MCS-5-rcnA plates and put them into 3 tubes with 3ml of Liquid LBGm20.
We used the  Roche Pasmid DNA extraction Kit  in order to obtain the pBBR1MCs-5 vector with rcnA.

2008-10-10
WET LAB

We ran a 1% agarose gel to verify the extraction.
NENE_V
The vector with rcnA was double-digested in order to verify the correct ligation of the fragments.
A 1% agarose gel was made to see the digested vector.
Gel enen
The pBBR1MCs-5/rcnA was used to transform W3110/YohM- competent cells by Heat shock. The transformed cells were plated on LBGm20 agar plates and incubated at 37°C the whole night.

2008-10-11

WET LAB

The  W3110/YohM-/pBBR1MCs-5/rcnA colonies were streaked on LBGm20 agar plates and incubated the whole night at 37°C.
The planning for the measurements was completed and ready to start.  
The propose for the determination of nickel internalization considerates to assume that when the medium has certain nickel concentration, the presence of cells from different strains will cause a variation in the resistivity(which, by the way will affect conductivity). For the different strains that we are using, we expect:

Strain

Changes expected

W3110 / YohM-

As this strain doesn’t carry the efflux pump RcnA. We expect  that the resistivity will increase due to the nickel internalization.

W3110 / YohM- pBBIMRCS-5

We expect a similar performance of these cells compared with W3110 / YohM-. However the extrusion pump for gentamicine present in the plasmid could be adding variation to the system.

W3110 / YohM- pBBIMRCS-5 RcnA

This cells carry the pBBIMRCS-5 plasmid with the efflux pump RcnA. Here, we expect oscillations due to the presence of a pump which internalizes nickel and the efflux pump.

W3110 / YohM+

We expect a similar behavior to the one observed in W3110 / YohM- pBBIMRCS-5 RcnA.

The two known critical concentrations of NiSO4 are 2.2 mM, the minimum inhibitory, and 500uM the minimun needed to repress RcnR activity.
Planned methodology:
-Establishment of a place to do the measurements.
  -We expect to have a constant temperature during the measurement process.
-Test the sensitivity of the measurement  dispositive. To achieve this, measurements will be done in agitation of:

        • Just LB
        • LB with NiSO4
        • LB with cells

 

Molarity

NiSO4 μl  from a solution 0.1M

0,0022

22

0,001

10

0,0001

1

0,00001

10

0,000001

1

0,0000001

10

0,00000001

1

0,000000001

10

1E-10

1

          • (,001) Dilución de 10 microlitros de 0.1 M en 1 mililitro
          • (,00001) Dilución de 10 microlitros de 0.001M en 1 mililitro
          • (0,0000001) Dilución de 10 microlitros de 0.00001 M en un mililitro

Internalization

-Grow the strain YohM- in LB medium until reach an OD(optical density) of 0.4 to ensure that the cells are in exponential phase. (Later this was changed to an OD of 0.5 at a lambda of 600nm).

-Plot concentration vs  time and calculate the slope
slope= Internalization rate of Ni2+

Extrusion
The following steps were performed in order to prove the RcnA activity, and to get the enough data to calculate conductivity  from the resistivity measurements. These conductivity data will be useful to get the extrusion rate of RcnA.

-          Grow the strains YohM-, YohM- + pBBMICS-5+RcnA, YohM- + pBBMICS-5 and YohM+  in LB medium until reach an OD(optical density) of 0.4 to ensure that the cells are in exponential phase. (Later this was changed to an OD of 0.5 at a lambda of 600nm).
-          Take 1ml  from each culture for each of the next nickel concentrations:

Molarity

Grams

Conductivity

0,0022   

0,3404368   

3,4375E-06

0,001   

0,154744   

1,5625E-06

0,0001   

0,0154744   

1,5625E-07

0,00001   

0,00154744   

1,5625E-08

0,000001   

0,000154744   

1,5625E-09

0,0000001   

1,54744E-05   

1,5625E-10

0,00000001   

1,54744E-06   

1,5625E-11

0,000000001   

1,54744E-07   

1,5625E-12

1E-10   

1,54744E-08   

1,5625E-13



- The measurements will be performed during three minutes for each one strain

2008-10-12

WET LAB
Some measurements were done in LB with and without nickel in order to calibrate and prove the apparatus. Initially the measurement dispositive included a gold electrode which seemed to be working properly.

2008-10-13

WET LAB

Solutions nickel 500uM and without nickel at all were prepared from samples of LB, and the strains YohM-, YohM- + pBBIMRCS-5 and YohM- + pBBIMRCS-5 + RcnA.

2008-10-14

WET LAB
The OD that the cells must reach was changed to 0.5 at a lambda of 600nm(This was due to the finding of the proper OD measurement in the strain W3110).
Some adjusts were done to the measurement dispositive in order to increase its sensibility.

2008-10-15

WET LAB
Preparation of the strains YohM-, YohM- + pBBIMRCS-5, and YohM- + pBBIMRCS-5 + RcnA for the measurements. An overnight of each strain was grown in LB. Samples of YohM- + pBBIMRCS-5, and YohM- + pBBIMRCS-5 + RcnA were prepared with different concentrations of NiSO4 . That concentrations includes a gradient from 1x10-3 M – 1X10-10M. And the two critical concentrations 500uM and 2.2mM.

2008-10-16

WET LAB
Strains were prepared in pursuit to perform some new measurements. Samples of LB, LB+ sulfate, and YohM-+RCNA+PBB were read.
Measurement intervals (100 milliseconds) semeed to be quite large, so its correction was proposed.

2008-10-17

MODELING:

Stoichiometric Matrix:

 Palsson, 2006

Flux vector                   ->         v=(v1, v2, …, vn)
Concentration vector      ->         x=(x1, x2, …, xm)          
->         δx/δt = S·v

δxi/δt=∑Sikvk

The four fundamental subspaces

 

Image from Systems Biology: Properties of Reconstructed Networks by Bernhard O. Palsson

The vector produced by a linear transformation is in two orthogonal spaces (the column and left null spaces), called the domain, and the vector being mapped is also in two orthogonal spaces (the row and null spaces), called the codomain or the range of the transformation.

The vectors in the left null space (li) represent mass conservation.

The flux vector can be decomposed into a dynamic component and a steady-state component:     
v = vdyn + vss

The steady state component satisfies Svss=0 and vss is thus in the null space of S.

2008-10-18

WET LAB
Prosecution of correction of measurement intervals.

2008-10-19

WET LAB
Due to the great variation observed in the data, some aspects of the samples, measurements and electrodes were reconsidered. As the variations could be caused by the ions present in the medium it was proposed to use a buffer instead of LB medium.

2008-10-20
MODELING:

The higher the number of independent reaction vectors, the smaller the orthogonal left null space. The higher the number of independent reactions, the fewer the conservation quantities exist.

 FUNDAMENTAL SUBSPACES OF S

The dimensions of both the column and row space is r (rank; number of linearly independent rows and columns that the matrix contains).         
dim(Col(S)) = dim(Row(S)) = r   
Since the dimension of the concentration vector is m, we have     
dim(Left Null(S)) = m− r
Similarly, the flux vector is n-dimensional; thus, 
dim(Null(S)) = n – r

  •        Null space. The null space of S contains all the steady-state flux distributions allowable in the network. The steady state is of much interest since most homeostatic states are close to being steady states.
  •        Row space. The row space of S contains all the dynamic flux distributions of a network and thus the thermodynamic driving forces that change the rate of reaction activity.
  •        Left null space. The left null space of S contains all the conservation relationships, or time invariants, that a network contains. The sum of conserved metabolites or conserved metabolic pools do not change with time and are combinations of concentration variables.
  •        Column space. The column space of S contains all the possible time derivatives of the concentration vector and thus shows how the thermodynamic driving forces move the concentration state of the network.
  • Singular Value Decomposition

    SVD states that for a matrix S of dimension m× n and of rank r, there are orthonormal matrices U (of dimension m ×m) and V (of dimension n × n) and a matrix with diagonal elements ∑ = diag(σ1, σ2, ... , σr ) with σ1 ≥ σ2 ≥ ··· ≥ σr > 0 such that S = U∑VT

    A non-negative real number σ is a singular value for M if and only if there exist unit-length vectors u in Km and v in Kn such that           
    Mv=σu and M*u=σv
    The vectors u and v are called left-singular and right-singular vectors for σ, respectively.       
    In any singular value decomposition       
    M=UΣV*
    the diagonal entries of Σ are necessarily equal to the singular values of M. The columns of U and V are, respectively, left- and right-singular vectors for the corresponding singular values.

    Image from Systems Biology: Properties of Reconstructed Networks by Bernhard O. Palsson
    Image from Systems Biology: Properties of Reconstructed Networks by Bernhard O. Palsson

     The columns of U are called the left singular vectors and the columns of V are the right singular vectors. The columns of U and V give orthonormal bases for all the four fundamental subspaces of S (see Figure 8.3). The first r columns of U and V give orthonormal bases for the column and row spaces, respectively. The lastmr columns of U give an orthonormal basis for the left null space, and the last n r columns or V give an orthonormal basis for the null space.

    WET LAB
    Correction of the measurement intervals to 1 millisecond.
    161008

    2008-10-21
    MODELING:

    THE (RIGTH) NULL SPACE OF S

    The right null space of S is defined by    
    Svss = 0
    Thus, all the steady-state flux distributions, vss, are found in the null space. The null space has a dimension of n r. Note that vss must be orthogonal to all the rows of S simultaneously and thus represents a linear combination of flux values on the reaction map that sum to zero.

    Mathematics versus biology

  •        The null space represents all the possible functional, or phenotypic, states of a network.
  •        A particular point in the polytope represents one network function or one particular phenotypic state.
  •        As we will see in Chapter 16, there are equivalent points in the cone that lead to the same overall functional state of a network. Biologically, such conditions are called silent phenotypes.
  •        The edges of the flux cone are the unique extreme pathways. Any flux state in the cone can be decomposed into the extreme pathways. The unique set of extreme pathways thus gives a mathematical description of the range of flux levels that are allowed.
  • - The stoichiometric matrix has a null space that corresponds to a linear combination of the reaction vectors that add up to zero; so-called link-neutral combinations.

    - The orthonormal basis given by SVD does not yield a useful biochemical interpretation of the null space of the stoichiometric matrix.

    THE LEFT NULL SPACE OF S

    As with the (right) null space, the choice of basis for the left null space is important in describing its contents in biochemically and biologically meaningful terms.

    …may represent mass conservation…

     THE ROW AND COLUMN SPACE OF S

    The column and row spaces of the stoichiometric matrix contain the concentration time derivatives and the thermodynamic driving forces, respectively.

    -