Team:Leeds/Results

Bacterial growth curves

We are monitoring the growth of our bacteria containing our devices to see if the genes we inserted have any effect on bacterial growth.

Control Bacterial Growth Curve

In this experiment we used our chosen expression cells and monitored their growth on SB media both in the presence of chloramphenicol and without chloramphenicol. As the bacteria do not contain our plasmid that codes for chloramphenicol resistance, we didn't expect them to grow when it was present. The graph produced from the absorbance measurements taken over time, shows the growth of the bacteria. It has a clear lag and log phase when the bacteria are grown in SB media only. But as expected, the graph shows that the bacteria do not grow in the presence of chloramphenicol. This graph will be used as a control and other growth curves of bacteria containing our device will be compared to it in order to determine whether the genes we inserted cause an effect on cell growth.

Characterisation of Device 1

Growth Curve

Bacteria were grown which contained Device 1; their absorbance was monitored over time and then the rate of growth compared to bacteria that do not contain Device 1. The graph clearly shows that inserting Device 1 into cells considerably slows their growth in log phase compared with the growth of cells without Device 1 but the lag phase is shorter than in the bacteria without the inserted device. The key difference however is that bacteria containing Device 1 don't grow to as high optical density in log phase as the bacteria without Device 1.

Membrane Stress

Investigation of literature regarding the action and regulation of the Cpx pathway lead to the discovery that the system as a whole responds to a large variety of membrane stresses, something that could be true of the specific promoter we chose to use (pCpxR). As a result of this we deemed it necessary to investigate the response of our promoter to each individual membrane stress.

Individually many of the experiments produced erratic and seemingly random data which is listed independently below. However plotting all average readings together shows that there is a dramatic increase in response to the stress induced by the silica beads comparative to all the chemically induced membrane stresses we used.

This indicates that it would be possible to detect the presence of silica beads in solution, in principle, using our binding and detection system, certainly when silica beads are present at relatively high concentrations. However further work needs to be done to assess whether this high response remains across a range of silica bead concentrations in solution.

In light of these results, some of these experiments were repeated for more accurate results. How the Cpx pathway reacts to temperature is already well characterised in the literature and by the Calgary 2010 iGem team.

The Ethanol gradient, Triton X-100 gradient and pH gradient were all repeated. In the second experiment, a robotic pipette was used to directly fill the 96 well plate to reduce human error. Excluding wells with imposed pH gradient, all wells were kept at pH 7 using Tris.HCl buffer, the pH gradient was also achieved with a Tris.HCl buffer.

The 96 well plates were then incubated while shaking while shaking for 2 hours at 37 degrees to allow time for GFP to mature. A longer incubation time was introduced to give more conclusive results.

Triton X-100

Between the concentration values of 0.1-9% triton X-100 the data shows roughly the relationship that was expected, a rise in GFP production as the triton concentration increases. This is likely due to triton acting as a detergent resulting in damage to the plasma membrane of cells, activating the Cpx pathway in general, including the cpxR promoter. Past 10% Triton X-100 concentration it is assumed that cells are dying in large quantities, being unable to produce GFP at all or in very limited amounts before they are killed. This explains the corrected fluorescence readings reducing to below zero. The reason for the large spike in fluorescence at Triton concentrations >20% is unclear, a possibly explanation for this is the total lysis of the cell, expelling all cellular components resulting in background GFP levels having a larger fluorescence reading due to reduced scattering from within the cell.

pH Effects

The slight fluctuations across the pH scale are in line with the background fluorescence readings from our cell cultures, representing the standard levels of cpx activation as the cells collide, disperse in solution and divide during replication.

The higher levels of expression at both low and high pH are likely to be due to the pH extremes denaturing proteins and disrupting interactions within the plasma membrane. It could be assumed that pH’s further into the extremes of acid and base would completely lyse and kill the cells resulting in a possibly lower fluorescence.

Ethanol

In this test a large, seemingly anomalous spike in an initial experiment was re-tested with smaller increasing increments of ethanol. The results are somewhat erratic but the peak just before 3% ethanol can be seen, before the fluorescence reading goes on to trough again.

Membrane Stress - Atomic Force Microscopy

Atomic Force Microscopy utilises Van-Der-Waals forces to attract the tip towards a surface, causing the bending of a cantilever, onto which a laser is pointed. The tip deflection causes the laser light to also be deflected and this is tracked using a bank of photodiodes. AFM is typically used to image surfaces at the atomic scale, as well as for Force Spectroscopy. When used in Force Spectroscopy, the tip is brought into direct contact with the sample, allowing the sample protein to bind to the silicon tip. Then, the AFM is slowly retracted at varying forces or to varying distances, applying a force to the protein. This causes portions of the protein to unravel, and the distinct patterns associated with α-helices and β-pleated sheets can be seen in this data. This allows the exact secondary and tertiary structure of a protein to be determined, but also the energy profile of various conformations, which in turn tells us how the protetin folds.

For Bio-Device 1 however, the team wanted to measure how much force was required to trigger the stress activated Cpx Pathway. This was to be done by observing the culture under the fluoroscope portion of the F-AFM, and then "prod" a bacterium at a low force, slowly increasing the stress until a fluorescence response was seen. This would then give a direct measure of the stress threshold for Cpx, a value currently unknown in the literature. However, as with all new experiments, there were some teething issues. Firstly, it can be seen from the image that the culture were already fluorescing a little, likely due to smaller stresses in solution, although some can clearly be seen in the middle of binomial fission, which is known to also activate the pathway. The other issue was with trying to keep the bacterial cells stable enough to continually poke them with AFM tip. Normally, this sort of experiment is performed on Giant Unilamellar Vesicles and microbubbles about 5 micron wide. These microstructures are naturally forming precursors to cells, and thus of great interest to bio-physicists. However, as trying to poke a structure 5 microns wide with a tip only 40nm at its widest is akin to throwing a needle from space onto a ship in the Atlantic ocean, experimenters usually adhere the bubbles to the surface with a binding peptide. This could not be done for bio-device 1 without potentially triggering the pathway, so instead, it was hoped a more viscous solution and some micro-troughs scratched into the glass slide surface would be enough to keep them steady. Again though, bacteria are very different to inert bubbles of lipids, and tend to forcibly move themsleves regardless, hence results remained inconclusive. The approach showed some promise however, and it is hoped further work will be undertaken on this at a later date. In the meantime however, it is clear that on the microscale, there is always some fluorescence, so a background reading will always be necessary to make use of Micro-Beagle. Additionally, it may be worth using evolutionary development techniques to mutate a strain with a higher threshold tolerance.

Characterisation of Si4

Growth Curve

Here the growth of cells containing Si4 was monitored via absorbance and compared to the growth of cells that do not contain Si4. As was seen when device 1 was inserted into the cells, the growth is slowed down considerably. Although the graph shows a log and a lag phase for the cells containing Si4, the absorbance reached in log phase is very low compared to cells without Si4; it is even lower than the absorbance reached for cells containing Device 1.

Characterisation of Device 3

Growth Curve

This graph shows the results of monitoring the growth of cells with contain Device 3. As with cells containing Device 1 and Device 2, the growth of the cells is considerably slowed down when compared with cells that do not contain any device at all. A slight change in the gradient of the graph can be seen showing the transition of the cell growth from lag to log phase, so the cells are still growing normally, but the insertion of Device 3 is restricting the growth of the cells.

Confocal Microscopy

Device 2 containing INP+Si4 along with Cpx and a Green Fluorescent Protein (GFP) coding region were incubated with silica beads of 5 micron diameter. The following images were taken with a confocal microscope.
In the images containing the cells, it can be clearly witnessed that GFP is produced. This could be either due to direct binding of the Si4 peptide to the silica beads, or through other elements of stress, such as cell division and cellular movement. Certain cells produced significantly higher amounts GFP, owing to the increased brightness of fluorescence in the images. This is apparent at instances when a cell appears to have bound to the silica bead. Most of the cells, however, failed to successfully associate with the silica beads present in solution. To this effect, it can be suggested that the Si4 polypeptide is perhaps not as efficient at interacting with the surface of the silica beads or that expression under the chosen promoter was lower than expected.
In certain cases, the fluorescence yield from the GFP molecules was reflected through the silica beads. Those samples had a uniform streak of light amplified through most of the silica beads in solution. These images were taken out and the ones used in discussion are the ones containing Device 2 bound to silica beads.
In the samples containing only the cells with Device 2 construct in them without silica beads being present, not a significant amount of fluorescence was detected. A few cells appeared to have produced GFP, however that is only due to external cellular stress cause by various factors

Scannning Electron Microscopy

The gallery above contains images that were produced by the Scanning Electron Microscope (SEM) at the University of Leeds. Device 2 was incubated in solution of varying concentrations of a silicate compound, which was solubilized using the sol-gel method from Tetraethyl orthosilicate (TEOS). Samples were incubated at room temperature, as well as some were done at 45ºC. For the control samples, cells without the Device 2 construct gene were used, and did not react with the silicate compound.

Silicate compound forming distinct spheres can be witnessed in one of the images. EDX chemical composition data is also included with each image, which allows assessment of the elements that are present in each sample. The high carbon output is partially due to the carbon adhesive used to isolate the samples for SEM. The silicate compound would envelop the cells either fully or partially and this can be gathered from the images shown. The images of control samples exemplify the silicate compound not extensively bound to the cells.

FACS

Device 2 contains our INP+Si4 construct, along with the Cpx and GFP genes. It was characterized using a flow cytometry method called Fluorescence-activated cell sorting (FACS) in solution with and without beads. The FASC images contain Side scattering and Forward scattering information, relating to relative size and density of the cells.

In the assay containing Device 2 with beads, there was an increase in the percentage of Population 3 (coloured in blue), from 0.1 to 2.2. This is suggestive of representing our Device 2 cells bound to silica beads. In contrast, the assay, which contained only Device 2 cells, had a very insignificant percentage of Population 3 (0.1%).

This suggests that our Device may successfully be binding to the silica beads utilizing the INP+Si4 construct, however not in all cases. This could either be due to not having enough time for the Device to binding to the silica, or that our Si4 binding domain is not as effective as it should be.