Download presentation
Presentation is loading. Please wait.
Published byWendy Meachum Modified over 10 years ago
1
Bryan Addeman April 6, 2010
2
Background Theory Motivation Measurements Moving Forward
3
Label specific metabolites with 13 C 12 C isotope is not magnetically active
5
Natural abundance of 13 C is ≈ 1.11% Amount of signal is related to gyromagnetic ratio (γ) & abundance ◦ γ H = 42.58 (Mhz/T) ◦ γ 13C = 10.71 (Mhz/T) Hyperpolarization can give a factor of 10,000x more initial signal
6
Inject sample mixed with free radical Cool to 1.4 K in a High magnetic field Bombard sample with microwaves Mix with heated solution Duration: 1.5 hours Amount of Hyperpolarization decays with time (T1) Robarts DNP Hyperpolarizer
7
Spin-Spin RelaxationSpin-Lattice Relaxation T1T2
9
Effects of low magnetic fields on T1values for hyperpolarized 13 C Pyruvic Acid
10
Hyperpolarized sample transport: ◦ B o : High (DNP) -> Low -> High (MRI) What happens to the sample in transit? T1 relaxation is a characteristic of the molecule that can be measured
11
SpinmasterOxford Instruments MQC Variable magnetic field ◦ B o = 0.0-0.9 T Desktop NMR system ◦ B o = 0.55 T Both devices can measure Signal amplitude at time intervals
12
B o =0.55, 13 C enriched Pyruvic Acid Fit Equation Non-Linear Least Squares Fit
13
SpinmasterMQC (0.55 Static Field) Field Strength (T) T1 (s)Fit Error (s)T1 (s)Fit Error (s) 0.5552.60.4458.30.31 0.023568.70.2587.00.82 0.023574.20.7883.70.56
14
Need to take more measurements to understand the effects low field strengths on T1 values
15
Supervisors Dr. Charles McKenzie Dr. Lanette Friesen- Walder Dr. Tim Scholl Dr. Jake Onwuachi Lab Curtis Wiens Samantha Flood Steven Yange Elmer Soto Trevor Wade
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.