Nuclear magnetic resonance study of muscle water protons in muscular dystrophy of chickens

Using the pulsed nuclear magnetic resonance (NMR) spectroscopy, the spin-lattice (T1) and the spin-spin (T2) relaxations times of water protons from samples of pectoralis major muscles of normal (line 412) and homozygous dystrophic (line 413) chickens were measured. Both the T1 and T2 were significantly increased (P less than 0.05) in the dystrophic muscles. The mean values of the relaxation times are given +/- S.D. The T1 values were 654 +/- 22 msec in normal and 692 +/- 41 msec in dystrophic muscles. The T2 values for normal and dystrophic muscles were 39 +/- 4 msec and 52 +/- 7 msec, respectively. Although the water content of dystrophic muscles (78.9 +/- 0.6%) determined by gravimetric methods was significantly higher than normal muscles (74.9 +/- 1.1%), this difference in tissue hydration could not explain quantitatively the increase of T1 and T2 values in the dystrophic muscles. The results of the measurements of the relaxation times seem to suggest that there are changes in the composition and/or conformational state of the proteins.     

The effects of cholera enterotoxin on intestinal tissue water as measured by nuclear magnetic resonance (NMR) spectroscopy.

Cholera enterotoxin has been postulated to change the configuration of the intracellular protein-water system, altering the permeability of the cell to water. Using nuclear magnetic resonance (NMR) spectroscopy, this protein-water relationship can be examined. Small intestinal loops in the rat were injected with 0.5 ml of either Schwarz/Mann cholera enterotoxin (40 mug/cc saline solution) or normal saline. Full thickness segments of intestine from each loop were taken and percentage water (using a gravimetric procedure which includes a correction for fat) and NMR relaxation times were determined. The mean value +/- S.D. for tissue water was 79.49 +/- 2.65% in the controls and 84.52 +/- 2.01% in the cholera specimens (p less than .001). T1 (spin-lattice) relaxation times were 521.22 +/- 69.5 msec in the controls and 667.96 +/- 119.25 msec in cholera tissue (p less than .001). T2 (spin-spin) relaxation times were 62.34 +/- 9.59 msec in controls and 80.35 +/- 21.46 msec in cholera tissue (p less than .02). These findings are consistent with the theory that cholera enterotoxin acts to alter intracellular protein-water relationship.     

NMR relaxation times of water protons in human colon cancer cell lines and clones

Established lines of human colon cancer cells from several sources (LS180, LS174T, HT29, SW480, SW1345) had water proton nuclear magnetic resonance (NMR) spin-lattice relaxation times (T1) of 460 +/- 45 msec to 982 +/- 9 msec and spin-spin relaxation times (T2) of 83 +/- 6 msec to 176 +/- 6 msec. Two clones derived from single cells of line LS174T were similar in T1 and T2 to the parent line. Differences among the cell lines were not totally a function of cellular hydration. Normal adult and fetal human primary colon cells were wetter and had higher T1 and T2 values than established cell lines. Relaxation times in this study substantiate variations seen for human colon tumors in earlier studies. Established cell lines maintained water relaxation times similar to tumor tissue values. Along with other morphological and biochemical criteria, the relaxation times suggest that these established human colon cancer cell lines may serve as a good experimental model for the study of human colon cancer.     

Magnetic resonance of water protons in fresh human blood plasma

Spin-lattice (T1-) relaxation times of fresh human blood plasma at 13.2 MHz and 29 degrees C ranged from 1263 milliseconds (msec) to 1709 msec. Spin-spin (T2-) relaxation times of those samples were between 446 msec and 753 msec. Proton magnetic resonance (p.m.r.) phantoms of such blood plasma were made with ferric chloride and corn starch in dilute hydrochloric acid, and also in dilute sulfuric acid. Their Fe3+ ion concentrations approximated 138 micrograms (micrograms) per deciliter (dl). Both T1 and T2 of any of these p.m.r. phantoms were within limits of those described above for fresh human blood plasma. Lowering of the concentration of the Fe3+ ion--in an experimental corn starch solution--was manifested in longer T1.     

Classes of hydration sites at protein-water interfaces: the source of contrast in magnetic resonance imaging.

Immobilized protein solute, approximately 20 wt %, alters the longitudinal and transverse nuclear magnetic relaxation rates 1/T1 and 1/T2 of solvent water protons in a manner that makes their values indistinguishable from those of a typical human tissue. There is now a quantitative theory at the molecular level (S.H. Koenig and R. D. Brown III (1993) Magn. Reson. Med. 30:685-695) that accounts for this, as a function of magnetic field strength, in terms of several distinguishable classes of water-binding sites at the protein-water interface at which significant relaxation and solute-solvent transfer of proton Zeeman energy occur. We review the arguments that these several classes of sites, characterized by widely disparate values of the resident lifetimes tau M of the bound waters, are associated with different numbers of hydrogen bonds that stabilize the particular protein-water complex. The sites that dominate relaxation-and produce contrast in magnetic resonance imaging (MRI), which derives from 1/T1 and 1/T2 of tissue water protons-have tau M approximately 10(-6)s. These, which involve four hydrogen bonds, occupy < or = 1% of the protein-water interface. Sites that involve three bonds, although more numerous, have < or = 20% smaller intrinsic effect on relaxation. The greater part of the "traditional" hydration monolayer, with even shorter-lived hydrogen-bonded waters, has little influence on solvent relaxation and is relatively unimportant in MRI. Finally, we argue, from the data, that most of the protein of tissue (a typical tissue is mostly protein) must be rotationally immobile (with Brownian rotational relaxation times slower than that of a 5 x 10(7) Da (very heavy) globular protein). We propose a functional basis for this immobilization ("cytoplasmic order"), and then indicate a way in which this order can break down ("cytoplasmic chaos") as a result of neoplastic transformation (cancer) and alter water-proton rates of pathological tissue and, hence, image contrast in MRI.     

Pulsed nuclear magnetic resonance study of 17-O, 2-D, and 1-H of water in frog striated muscle.

Whole gastrocnemius muscles were incubated in Ringer's solution enriched with H2-17O; the paired contralateral gastrocnemius muscles were incubated in a similar solution enriched with deuterons, as well. Subsequently, the longitudinal relaxation times (T1) were measured 17-O, 2-D, and 1-H, both at 8.1 MHz and at 4.3 MHz. The results indicate that: (a) the absolute values of T1 characterizing the three nuclides are different in muscle and pure water. (b) the longitudinal relaxation rates of all three have an identical frequency dependence over the range studied, (c) the ratio (T1)2D/(T1)17ois the same in muscle water and pure water, while the ratio (T1)1H/(T1)17o is 2.1 times greater in pure water than it is in muscle water, and (d) 30-49 percent substitution of 2-D for 1-H has very little effect on the spin-lattice relaxation of tissue water protons. These data suggest that muscle water is in rapid exchange between a small fraction of immobilized molecules and a large fraction of free water. The results render unlikely the possibility that hypothetical ordering of muscle water significantly contributes to its longitudinal relaxation.     

Improved discrimination of normal and malignant tissue using 1H NMR relaxation time measurements at 2.18 MHz

The 1H NMR spin-lattice relaxation time (T1), spin-spin relaxation time (T2), and spin-lattice relaxation time in the rotating frame (T1rho) were determined for Novikoff hepatoma, Walker-256 Carcinosarcoma, Sarcoma-180 and Ehrlich Ascites tumor as well as for 7 normal tissues in the rat at 2.18 MHz. T1 values yielded improved discrimination of normal and malignant tissue compared to previous results at higher frequencies.     

Proton magnetic relaxation dispersion in solutions of the cuproprotein diamine oxidase.

Proton nuclear magnetic resonance relaxation measurements were made over the range 4.7--220 MHz for aqueous solutions of hog kidney diamine oxidase. The values of 1/T1 give rise in two distinct dispersions, at 16 and 75 MHz, whereas 1/T2 displays a minimum at 20 MHz. The temperature dependence of relaxation rates in all cases yield apparent activation energies less than 0.6 kcal/mol. These data indicate to us that the two Cu(II) ions of diamine oxidase are intrinsically different in terms of their electronic relaxation characteristics and hence, chemical environments. Low field limits of the two electronic relaxation times are 2 and 10 ns, with one of these correlation times being frequency dependent. The value of the frequency-dependent electronic relaxation time is governed by interactions that are modulated by a process having a correlation time of 5 ps.     

The potency of fluorinated ether anesthetics correlates with their 19F spin-spin relaxation times in brain tissue

In this study, four fluorinated ether anesthetics and one non-anesthetic fluorinated alkane were observed in rat brain and adipose tissue using 19F-NMR spectroscopy. Measurements of 19F spin-spin relaxation times (T2) of the anesthetics in brain revealed T2 values (0.5-4.5 msec) that correlated linearly with the anesthetic potency (ED50) of the drugs. The non-anesthetic was present at very low concentrations in brain and had a T2 value (18.5 msec) far longer than that of any of the anesthetics. All of the drugs were present at high concentration in peripheral adipose tissue. 19F T2 values for these drugs in adipose tissue (200-400 msec) were far larger than the values observed in brain and did not correlate with anesthetic potency. These results indicate that volatile anesthetic molecules have a specific affinity for neural tissue and that immobilization of anesthetic molecules in brain correlates with anesthetic potency. The results with adipose tissue suggest that the interaction of anesthetic with brain tissue cannot be explained by a simple partition of these drugs into lipid.     

Role of 'cell type' in proton relaxation in normal and neoplastic lymph nodes characterized by pulsed NMR spectroscopy

Pulsed NMR studies have been undertaken on malignant lymphomas. It has been observed that water proton spin-lattice relaxation times of lymph node tissues show increase in lymphnodes of Hodgkin's and Non-Hodgkin's lymphoma as compared to those in normal subjects. The T1 values of normal lymphnodes showed a range of 200-300 msec, while the metastatic lymphnodes showed a range of 400-600 msec at 20 MHz. These studies have brought out the importance of histopathological significance and the role of 'cell type' and biomolecules as a factor influencing water proton relaxation times. Further the relevance of the present in vitro studies to Magnetic Resonance Imaging of ex vivo images of normal and metastatic lymphnodes has become evident from some recent studies reported in normal and afflicted lymphnodes.     

Magnetic resonance studies of the interaction of Co2+ and phosphoenolpyruvate with pyruvate kinase.

Co2+, which activates rabbit muscle pyruvate kinase, competes with Mn2+ for the active site of the enzyme with a KD of 46 muM. Co2+ binds to phosphoenolpyruvate with a KD of 4.1 mM. The structures of the binary Co2+/P-enolpyruvate, and quaternary pyruvate kinase/Co2+/K+/P-enolpyruvate complexes were studied using EPR and the effects of Co2+ on the longitudinal (T1) and transverse (T2) relaxation times of the protons of water and P-enolpyruvate and the phosphorus of P-enolpyruvate. The EPR spectra of all complexes at 6 K, disappear above 40 K and reveal principal g values between 2 and 7 indicating high spin Co2+. For free Co2+ and for the binary Co2+/P-enolpyruvate complex, the T1 of water protons was independent of frequency in the range 8, 15, 24.3, 100, and 220 MHz. Assuming coordination numbers (q) of 6 and 5 for free Co2+ and Co2+/P-enolpyruvate, respectively, correlation times (tauc) of 1.3 times 10(-13) and 1.7 times 10(-13) s, were calculated. The distances from Co2+ and phosphorus and to the cis and trans protons in the binary Co2+/P-enolpyruvate complex calculated from their T1 values were 2.7 A, 4.1 A, AND 5.3 A, respectively, indicating an inner sphere phosphoryl complex. Consistent with direct phosphoryl coordination, a large Co2+ to phosphorus hyperfine contact coupling constant (A/h) of 5 times 10(5) Hz was determined by the frequency dependence of the T2 of phosphorus at 25.1, 40.5, and 101.5 MHz. For both enzyme complexes, the dipolar correlation time tauc was 2 times 10(-12) s and the number of rapidly exchanging water ligands (q) was 0.6 as determined from the frequency dependence of the T1 of water protons. In the quaternary enzyme/Co2+/K+/P-enolyruvate complex this tauc value was consistent with the frequency dependence of the T1 of the phosphorus of enzyme-bound P-enolpyruvate at 25.1 and 40.5 MHz. Distances from enzyme-bound C02+ to the phosphorus and protons of P-enolpyruvate, from their T1 values, were 5.0 A and 8 to 10 A, respectively, indicating a predominantly (greater than or equal to 98%) second spere complex and less than 2% inner sphere complex. Consistent with a second sphere complex on the enzyme, an A/h value of less than 10(3) Hz was determined from the frequency dependence of the T2 of phosphorus. In all complexes the exchange reates were found to be faster than the paramagnetic relaxation rates and the hyperfine contact interaction was found to be small compared to the dipolar interaction. The results thus indicate that the interaction of C02+ with P-enolpyruvate is greatly decreased upon binding to the active site of pyruvate kinase.     

NMR relaxation of protein and water protons in diamagnetic hemoglobin solutions

We have measured T1 and T2 of protein and water protons in hemoglobin solutions using broad-line pulse techniques; selective excitation and detection methods enabled the intrinsic protein and water relaxation rates, as well as the spin-transfer rate between them, to be obtained at 5, 10, and 20 MHz. Water and protein T1 data were also obtained at 100 and 200 MHz for hemoglobin in H2O/D2O mixtures by using commercial Fourier-transform instruments. The T1 data conform to a simple model of two well-mixed spin systems with single intrinsic relaxation times and an average spin-transfer rate, with each phase recovering from a radio-frequency excitation with a biexponential time dependence. At low frequencies, protein T1 and T2 agree reasonably with a model of dipolar relaxation of an array of fixed protons tumbling in solution, explicitly calculating methyl and methylene relaxation and using a continuum approximation for the others. Differing values in H2O and D2O are mainly ascribed to solvent viscosity. For water-proton relaxation, T1, T2, and spin transfer were measured for H2O and HDO, which enabled a separation of inter-and intramolecular contributions to relaxation. Despite such detail, few firm conclusions could be reached about hydration water. But it seems clear that few long-lived hydration sites are needed to explain T1 and T2, and the spin-transfer value mandates fewer than five sites with a lifetime longer than 10(-8) s.     

Proton magnetic relaxation studies in normal and cancerous breast tissues

Proton magnetic resonance (PMR) relaxation times were measured for dissected malignant and normal tissue derived from breast cancer patients. Relaxation time measurements (T1, T2) were carried out at a RF frequency of 20 MHz and at a temperature of 27 degrees C with a Brucker PC 120 NMR Process analyser. The tissue types were confirmed by histopathological examination. In general T1 values were found to be longer for malignant tissues as compared to normal tissues which is in agreement with the earlier observations. The measured T2 values do not exhibit the malignant tissues above. The percentage of water content was also measured in both normal and malignant tissue and was found to be considerably larger in tumour tissue as compared to normal tissue. These results are discussed on the basis of two fraction fast exchange models of water molecules and confirm that PMR relaxation time measurement plays an important role in the differentiation of cancerous tissues from that of normal.     

Theory of relaxation of mobile water protons induced by protein NH moieties, with application to rat heart muscle and calf lens homogenates.

Kimmich and co-workers (cf., Winter, F., and R. Kimmich. 1982. Biochim. Biophys. Acta. 719:292-298) discovered peaks in the magnetic field-dependent longitudinal relaxation rate (1/T1) of water protons of muscle tissue, cells, and dehydrated protein in the field range 0.5-5 MHz (proton Larmor frequency), and argued that the peaks resulted from cross relaxation associated with quadrupolar splittings of the 14N nuclei of protein NH groups. More recently, analogous peaks were found in homogenates of calf eye lens (Beaulieu, C.F., J.I. Clark, R.D. Brown III, M. Spiller, and S. H. Koenig, 1987. Abstr. Soc. Magn. Res. Med., 6th, New York. 598-599), which are essentially concentrated protein solutions, and were measured with sufficient precision to allow resolution of the relaxation spectra into several peaks and the intrinsic linewidths to be determined. Here, we analyze these relaxation spectra, as well as earlier data on rat heart (Koenig, S. H., R. D. Brown III, D. Adams, D. Emerson, and C. G. Harrison. 1984. Invest. Radiol. 19:76-81) in some detail, and suggest a specific pathway for the cross relaxation to which we apply the theory of relaxation quantitatively. The view that emerges is that, at fields such that the proton Zeeman energy of the NH protons matches an 14N quadrupolar splitting, relaxation of these protons is by cross relaxation to the 14N nuclei which in turn transfer excess energy to the protein. The correlation time for the NH proton interaction is the T2 of the 14N nuclei, approximately 10(-6) s, whereas T1 of the NH protons is approximately 1.25 ms.(ABSTRACT TRUNCATED AT 250 WORDS)     

1H and 31P Fourier transform magnetic resonance studies of the conformation of enzyme-bound propionyl coenzyme A on the transcarboxylase.

The relaxation rates of the carbon-bound protons and of the three assigned phosphorus resonances of propionyl-CoA were measured in solutions of free propionyl-CoA and of the transcarboxylase-propionyl-CoA complex. In free propionyl-CoA, analysis of the 1/T1 values of 15 protons at 100 and 220 MHz and of 1/T1 and 1/T2 of the three phosphorus atoms at 40.5 MHz indicated free rotation of the propionyl region (taur approximately 3 x 10(-11) sec) but hindered motion of the remainder of the molecule with correlation times of 1-3. 5 x 10(-10) sec, approaching the tumbling time of the entire molecule (taur - 6 x 10(-10) sec. The correlation times of the three phosphorus atoms were indistinguishable from those of their nearest neighbor protons. The effects of three homogeneous enzyme preparations with varying contents of Zn(II), Co(II), and Cu(II) on 1/T1 of 12 protons and 3 phosphorus atoms of prionyl-CoA were analyzed with the help of simultaneous equations to yield the individual contributions at the three metal sites. Only diamagnetic effects were detected on the relaxation rates of the three phosphorus atoms. From the diamagnetic effects it was calculated that the motions of the prionyl side chain and of the terminal pantetheine methylene protons were hindered on the enzyme by an order of magnitude (taur approximately 6 x 10(-10) sec) and that the phosphorus atoms were hindered by two orders of magnitude (taur approximately 1 x 10(-8) sec) over the taur values found in free propionyl-CoA, but that these taur values remained well below that of the entire protein molecule (taur =6 x 10(-7) sec)...     

Nuclear magnetic resonance studies of amino acids and proteins. Rotational correlation times of proteins by deuterium nuclear magnetic resonance spectroscopy

We show that measurement of the spin-lattice (T1) and spin-spin (T2) relaxation times (or line widths) of irrotationally bound 2H nuclei in macromolecules undergoing isotropic rotational motion outside of the extreme narrowing limit (i.e., for the case omega 02 tau R2 much greater than 1) permits determination of both the rotational correlation time (tau R) of the macromolecule and the electric quadrupole coupling constant (e2qQ/h) of the 2H label. The technique has the advantage over 13C nuclear magnetic resonance (NMR) that no assumptions about bond lengths (which appear to the sixth power in 13C relaxation studies) or relaxation mechanisms need to be made, since relaxation will always be quadrupolar, even for aromatic residues at high field. Asymmetry parameter (eta) uncertainties are shown to cause negligible effects on tau R determinations, and in any case it is shown that both e2qQ/h and eta may readily be determined in separate solid-state experiments. By way of example, we report 2H NMR results on aqueous lysozyme (EC 3.2.1.17) at 5.2 and 8.5 T (corresponding to 2H-resonance frequencies of 34 and 55 MHz). Interpretation of the results in terms of the isotropic rigid-rotor model yields e2qQ/h values of approximately equal to 170 or approximately equal to 190 kHz, respectively, for the imidazolium and free-base forms of [epsilon 1-2H] His-15 lysozyme in solution, in excellent agreement with e2qQ/h values of approximately 167 and approximately 190 kHz obtained for the free amino acids in the solid state. In principle, the method may in suitable cases permit comparison between the dynamic structures of proteins in solution and in the crystalline solid state.     

Transfer RNA structure by carbon NMR: C2 of adenine, uracil and cytosine.

Fourier transform 13C NMR spectra of E. coli tRNA enriched on 13C in either position 2 of adenine (60 atom % 13C) or in position 2 of uracil (82%) and cytosine (63%) were taken at 25.16 MHz over the temperature range 10 degrees - 76 degrees. For C2 of adenine the peak as initially 5 ppm wide, but narrowed to 0.5 ppm as the molecule unfolded. C2 of uracil displayed behavior similar to that of adenine while the cytosine peak, initially relatively narrow at low temperature, sharpened less dramatically. Comparison of spectra at 26.16 MHz and 67.9 MHz showed that the peak widths for folded tRNA were determined largely by chemical shift non-equivalence. T2 T2 measurements suggested that intrinsic line widths of most cytosine C2 peaks were 4 Hz and 2-3 Hz for uracil. Adenine C2 with a directly bonded proton had resonances of about 40 Hz line width. T1 values were measured for C2 of adenine and the ribose carbons of tRNA. Consideration of dipolar relaxation and chemical shift anisotrophy led to a calculated rotational correlation time of 1.6 +/- 0.4 x 10(-8) sec for the adenines and 1.3 +/- 0.3 x 10(-8) sec for the ribose carbons.     

Effect of calcium on the dynamic behavior of sialylglycerolipids and phospholipids in mixed model membranes. A 2H and 31P NMR study

DTSL, a sialic acid bearing glyceroglycolipid, has been deuteriated at the C3 position of the sialic acid headgroup and at the C3 position of the glycerol backbone. The glycolipid was studied as a neat dispersion and in multilamellar dispersions of DMPC (at a concentration of 5-10 mol % relative to phospholipid), using 2H and 31P NMR. The quadrupolar splittings, delta v Q, of the headgroup deuterons were found to differ in the neat and mixed dispersion, suggesting different headgroup orientations in the two systems. In DTSL-DMPC liposomes, two quadrupolar splittings were observed, indicating that the axial and equatorial deuterons make different angles with respect to the axis of motional averaging. The splittings originating from the equatorial and axial deuterons were found to increase and decrease with increasing temperature, respectively, indicating a temperature-dependent change in average headgroup orientation. Longitudinal relaxation times, T1Z, were found to be short (3-6 ms). The field dependence of T1Z suggests that more than one motion governs relaxation. At 30.7 MHz a T1Z minimum was observed at approximately 40 degrees C. At 46.1 MHz the T1Z values were longer and increased with temperature, demonstrating that the dominant rigid-body motions of the headgroup at this field are in the rapid motional regime (greater than 10(8) s-1). DTSL labeled at the glycerol C3 position was studied in DMPC multilamellar dispersions. Whereas two quadrupolar splittings have been observed for other glycolipids labeled at this position, only a single delta nu Q was observed. This shows that the orientation of the C2-C3 segment of DTSL relative to the bilayer normal differs from that of other glycolipids.(ABSTRACT TRUNCATED AT 250 WORDS)     

Study of anisotropy in nuclear magnetic resonance relaxation times of water protons in skeletal muscle.

The anisotropy of the spin-lattice relaxation time (T1) and the spin-spin relaxation times (T2) of water protons in skeletal muscle tissue have been studied by the spin-echo technique. Both T1 and T2 have been measured for the water protons of the tibialis anterior muscle of mature male rats for theta = 0, 55, and 90 degrees, where theta is the orientation of the muscle fiber with respect to the static field. The anisotropy in T1 and T2 has been measured at temperatures of 28, -5 and -10 degrees C. No significant anisotropy was observed in the T1 of the tissue water, while an average anisotropy of approximately 5% was observed in T2 at room temperature. The average anisotropy of T2 at -5 and -10 degrees C was found to be approximately 2 and 1.3%, respectively.     

NMR in cancer. VII. Sodium-23 magnetic resonance of normal and cancerous tissues.

Sodium-23 magnetic resonance was performed on four types of cancers and six types of normal tissues of rats and mice. The spin-lattice relaxation time of the tumors was generally longer than that of the normal tissues, with the most marked difference occurring between rat liver (T1 = 6.5 msec) and Novikoff hepatoma (T1 =23.7 msec). Estimation of tissue sodium from the signal intensity of the resonance indicated that all four types of tumors contained more sodium than any of the normal tissues.