This mini-review summarizes studies my associates and I carried out that are relevant to the topic of the present volume [i.e. glutamate dehydrogenase (GDH)] using radioactive 13 N (t ½ 9.96 min) as a biological tracer. These studies revealed the previously unrecognized rapidity with which nitrogen is exchanged among certain metabolites in vivo. For example, our work demonstrated that a) the t ½ for conversion of portal vein ammonia to urea in the rat liver is ~10-11 sec, despite the need for five enzyme-catalyzed steps and two mitochondrial transport steps, b) the residence time for ammonia in the blood of anesthetized rats is ≤7-8 sec, c) the t ½ for incorporation of bloodborne ammonia into glutamine in the normal rat brain is <3 sec, and d) equilibration between glutamate and aspartate nitrogen in rat liver is extremely rapid (seconds), a reflection of the fact that the components of the hepatic aspartate aminotransferase reaction are in thermodynamic equilibrium. Our work emphasizes the importance of the GDH reaction in rat liver as a conduit for dissimilating or assimilating ammonia as needed. In contrast, our work shows that the GDH reaction in rat brain appears to operate mostly in the direction of ammonia production (dissimilation). The importance of the GDH reaction as an endogenous source of ammonia in the brain and the relation of GDH to the brain glutamine cycle is discussed. Finally, our work integrates with the increasing use of positron emission tomography (PET) and nuclear magnetic resonance (NMR) to study brain ammonia uptake and brain glutamine, respectively, in normal individuals and in patients with liver disease or other diseases associated with hyperammonemia.
Keywords[ 13 N]Ammonia; 13 N-labeled amino acids; alanine aminotransferase; aspartate aminotransferase; branched chain amino acid aminotransferase; glutamate dehydrogenase; glutamine cycle; nitrogen flux; transreamination; transdeamination; urea cycle
Historical13 N is a positron emitting isotope. In positron (or β + ) emission, the particle ejected from the nucleus of the decaying nuclide has the same mass, but opposite charge, to that of the electron. As with the more familiar β − (electron) emission, the ejected positrons are emitted with a spectrum of kinetic energies with characteristic E average and E max values. In the case of 13 N, the E max value is 1.2 MeV. By comparison, the E max values of the more familiar β − emissions of 14 C and 32 P are 0.16 and 1.7 MeV, respectively. After rapidly losing most of its kinetic energy, the ejected positron combines with a nearby electron to form a * Tel.: +1-914-597-3330; fax: +1-914-594-4058, Arthur_cooper@nymc.edu.Publisher's Disclaimer: This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final citable form. Please note that during the production...