Part:BBa_K1123018
Poly(Arginine-Glycine) Protein
This part contains the DNA sequence of a protein of our own design. We first repeated the Arginine-Glycine amino acid pair 6 times to obtain a sequence of 12 amino acids. This sequence was then repeated a total of 36 times. Between these repeats no extra amino acids were added. The idea behind this protein was to provide ourselves with a high concentration of amino acids with amide groups which we could then use to provide CEST contrast in an MRI.
Sequence and Features
- 10COMPATIBLE WITH RFC[10]
- 12INCOMPATIBLE WITH RFC[12]Illegal NotI site found at 74
Illegal NotI site found at 338 - 21COMPATIBLE WITH RFC[21]
- 23COMPATIBLE WITH RFC[23]
- 25COMPATIBLE WITH RFC[25]
- 1000COMPATIBLE WITH RFC[1000]
Characterization
Characterization by the TU Eindhoven 2013 iGEM Team
This part was designed to generate CEST MRI contrast. The basic principle behind this technique is based on compounds that contain pools of exchangeable protons that can be selectively saturated using radiofrequency irradiation. Upon proton exchange with bulk water, these compounds can be indirectly visualized by measuring the bulk water using an MRI machine. The amino acids Lysine, Arginine, Threonine and Serine contain those exchangeable protons and polypeptides containing those amino acids in abundance are therefore potential contrast agents (see also [http://2013.igem.org/Team:TU-Eindhoven/Background CEST 101]).
The protein of this part has a Arginine percentage of 50 %, which is high compared to other (native) proteins. Therefore, it was expected that this protein would be detectable using CEST MRI.
Methods
The proteins were (aerobically) overexpressed in BL21 using a pET28a vector with a T7 promotor. The bacteria were spun down and fixed in PFA. The entire pellet (bacteria containing our proteins) was then measured in a 7 T Bruker MRI machine. First, the correct water frequency was determined, the machine was shimmed, i.e. a homogeneous magnetic field was created. The first measurement was a T2 weighed image for general orientation. Subsequently local shimming was performed on each of the separate pellets. For the final measurements, the saturation pulse was set to vary from ca. -4ppm to ca. +4ppm (relative to water), the measurements were averaged over 8 separate scans. Also a S0 (without saturation pulse) image was taken.
Results
This data was processed resulting in a asymmetry plot (MTR_assymetric) and a contrast plot visualizing the difference of the sample with the control sample. This was done by both subtracting (absolute difference) and dividing (relative difference). For a complete overview of the processing steps see the TU-Eindhoven 2013 [http://2013.igem.org/Team:TU-Eindhoven/MRIProcessing MRI Data Processing page]. The results are shown below:
Conclusion
Around 2.0 ppm there seems to be an arginine peak in the MTR_assymetric plot, but it is hard to distinguish from background noise. Also when compared to the control sample it remains unclear whether the peak is caused by Arginine or a difference in concentration between the sample and the control sample. Therefore the agent can not be clearly distinguished from the background and there is no clear CEST contrast.
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