Team:TU-Eindhoven/MRIProcessing

From 2013.igem.org

(Difference between revisions)
(Processing)
(MRI Data Processing)
Line 22: Line 22:
{{:Team:TU-Eindhoven/Template:FloatEnd | caption=Equations for analyzing the CEST MRI data. | id=MTRasymEquations }}
{{:Team:TU-Eindhoven/Template:FloatEnd | caption=Equations for analyzing the CEST MRI data. | id=MTRasymEquations }}
-
 
+
<br /><br />
-
 
+
-
 
+
Putting this principle into practice requires some processing steps. First of all, the asymmetric comparison should be conducted as shown in {{:Team:TU-Eindhoven/Template:Figure | id=MTRasymEquations }}. Where the MTR<sub>asym</sub> is the asymmetry in the z-spectrum. Furthermore, $S_{0}$ and $S_{w}^{\pm\Delta\omega_{sw}}$ are, respectively, the water signals without saturation and with saturation at $\Delta\omega_{sw}$ from bulk water. The PTR is the Proton Transfer Enhancement, which gives an indication of the sensitivity of an agent, independent of the concentration. In this research, the concentration was not measured accurately, but the mass of cell pellet was aimed to be kept constant, so the MTR<sub>asym</sub> plots can still be compared quite well.
Putting this principle into practice requires some processing steps. First of all, the asymmetric comparison should be conducted as shown in {{:Team:TU-Eindhoven/Template:Figure | id=MTRasymEquations }}. Where the MTR<sub>asym</sub> is the asymmetry in the z-spectrum. Furthermore, $S_{0}$ and $S_{w}^{\pm\Delta\omega_{sw}}$ are, respectively, the water signals without saturation and with saturation at $\Delta\omega_{sw}$ from bulk water. The PTR is the Proton Transfer Enhancement, which gives an indication of the sensitivity of an agent, independent of the concentration. In this research, the concentration was not measured accurately, but the mass of cell pellet was aimed to be kept constant, so the MTR<sub>asym</sub> plots can still be compared quite well.

Revision as of 19:33, 3 October 2013

Contents

MRI Data Processing

Until recently, the most common way of generating MRI contrast was by using heavy metal based contrast agents. Examples of these substances are the commercial Gadolinium(III) based Magnevist and the Iron Oxide based Resovist. A very obvious downside of using heavy metals is the toxicity of the agents in the human body. Fortunately, a new type of MRI has been developed, which allows for the use of organic compounds as contrast agent.

TU-Eindhoven Images CESTExplaination.jpg
CESTExplaination a) and b) Solute protons are saturated at their specific resonance frequency in the proton spectrum, this saturation is then transferred to water. c) Measurement of normalized water saturation, the Z-spectrum. d) result of the asymmetry analysis of the Z-spectrum. REFERENCE

The Principle

This new type of MRI goes by the name Chemical Exchange Saturation Transfer MRI or CEST MRI. The 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. 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. An other advantage of CEST MRI is that different kind of protons (e.g. amide and hydroxide protons) can be distinguished, which allows for 'multi-color' imaging using multiple contrast agents simultaneously.

Processing

To detect these protons in bulk water some processing steps are required. First of all, the imaging should be taken at different frequencies of the saturation pulse. This way the signal at different chemical shifts can be measured. When bulk water is set to 0 ppm, the signal plot will be roughly symmetric around zero, since saturation pulses will excite the bulk water in a similar way when the absolute shift is equal. This also implies that when the signals with a negative shift from the bulk water are compared with the signals with a positive shift, asymmetry can be detected. The CEST effect is exactly what causes asymmetry in the signal plot, because the chemical shift of the CEST compounds is different from the chemical shift of water. Therefore, when the absolute shift from bulk water of two saturation pulses is equal, this does not mean the absolute shift from the CEST compound is equal and the CEST protons will in one case get barely saturated (depending on its shift from bulk water of course).

$$\begin{aligned} MTR_{ asym} &= {{S_{w}^{-\Delta\omega_{sw}} - S_{w}^{-\Delta\omega_{sw}}}\over{S_0}} \\ PTE &= {{2 \cdot [H_{2}O]}\over{[polypeptide]}} \cdot MTR_{asym} \end{aligned} $$
MTRasymEquations Equations for analyzing the CEST MRI data.



Putting this principle into practice requires some processing steps. First of all, the asymmetric comparison should be conducted as shown in . Where the MTRasym is the asymmetry in the z-spectrum. Furthermore, $S_{0}$ and $S_{w}^{\pm\Delta\omega_{sw}}$ are, respectively, the water signals without saturation and with saturation at $\Delta\omega_{sw}$ from bulk water. The PTR is the Proton Transfer Enhancement, which gives an indication of the sensitivity of an agent, independent of the concentration. In this research, the concentration was not measured accurately, but the mass of cell pellet was aimed to be kept constant, so the MTRasym plots can still be compared quite well.

To eliminate the background signal of other lysine and arginine rich proteins, the asymmetric plots of the potential agents were compared to the asymmetric plots of the control sample, where no protein was overexpressed. In practice this can be compared to using an MRI image of human tissue without contrast agent as control for an image of tissue with contrast agent. This comparison was done in two different ways, one option results in the absolute difference compared to the control sample. The other method is relatively comparing the samples ().

$$\begin{aligned} C_{abs} &= MTR_{ asym}^{ agent} - MTR_{ asym}^{ control} \\ C_{rel} &= {{MTR_{ asym}^{ agent}}\over{MTR_{ asym}^{ control}}} - 1 \end{aligned} $$
ContrastComparison Comparison of agent samples and the control sample.

Results

When these processing steps are applied to the MRI results of this research, the following graphs can be acquired. shows the MTRasym, $C_{abs}$ (Absolute Difference) and $C_{rel}$ (Relative Difference) graphs for all potential contrast agents that were tested.

TU-Eindhoven Images allMRIGraphs.png
AllMRIGraphs Text needed.
Lysine protons are predicted to show contrast at a shift of $\pm 3.7 ppm$ whereas arginine should produce contrast at $\pm 2.0 ppm$. Using this information it can be readily seen that 1PJN and Poly(KS) both exhibit (lysine-)CEST contrast.

References