Human plasma fibronectin structure probed by steady-state fluorescence polarization: evidence for a rigid oblate structure

In order to more clearly define the structure of human plasma fibronectin (PFn) under physiologic buffer conditions, we determined the mean harmonic rotational relaxation times (rho H) of PFn and the thrombin-derived 190/170-kDa PFn fragment using steady-state fluorescence polarization. These measurements utilized the long lifetime emission (tau = 1.2 X 10(-7) S) exhibited by 1-pyrenebutyrate, which had been covalently attached to amino groups at random sites on the PFn subunit. Our data analysis assumed that two independent processes depolarize the fluorescence exhibited by the dansylcadaverine and 1-pyrenebutyrate conjugates of PFn: (A) rapid (rho H less than 10(-9) S) "thermally-activated" localized rotational motion of the protein side chains bearing the fluorescent probe [Weber, G. (1952) Biochem. J. 51, 145-154] and (B) slow (rho H approximately 10(-6) S) temperature-independent global rotational motion of the whole PFn molecule. Since only the rho H associated with the latter process is a true hydrodynamic parameter (i.e., sensitive to size and/or shape of the PFn molecule), we utilized isothermal polarization measurements to discriminate against the interfering signal arising from "thermally activated" probe rotation. The rho H (4.4 +/- 0.9 microseconds) derived from an experiment in which pyrene-PFn fluorescence polarization was monitored as a function of sucrose concentration at constant temperature is 7 (+/- 1.4) times longer than that predicted for an equivalent hydrated sphere. We propose that "thermally activated" probe rotation gives rise to the nearly 100-fold shorter PFn rho H values previously reported in the literature. Consequently, our data exclude all previous models which invoke segmental flexibility of the PFn peptide backbone. The simplest hydrodynamic model supported by our fluorescence data is an oblate ellipsoid with an axial ratio of 15:1. All prolate models can be unambiguously excluded by this result. We estimate that the disk-shaped PFn molecule has a diameter and thickness of 30 and 2 nm, respectively. Electron microscopy of negatively stained PFn specimens on carbon also showed PFn to have a compact rounded structure. The much faster rotational relaxation rate of the pyrene-190/170-kDa PFn fragment (rho H = 0.92 +/- 0.11 microseconds) compared to pyrene-PFn indicated that this monomeric PFn fragment, like native PFn, had an oblate shape under physiologic buffer conditions.     

Hydration of clupeine in solution

Spin-lattice relaxation times, T1, of H2(17) O at 25 degrees were measured for aqueous solutions of clupeine and its constituent amino acids, which are serine, threonine, proline and arginine. The dynamic hydration numbers, nDHN, of clupeine and amino acids were determined from a concentration dependence of T1. The coordination numbers nh, and the rotational correlation times, tau ch, of water molecules around clupeine and amino acids were estimated and compared with that of pure water. The tau ch/tau co of clupeine was 1.85 and close to that of arginine. The experimental value of nDHN of clupeine was in good agreement with that calculated from the nDHN values of the constituent amino acids. This means that the clupeine molecule has a random conformation in solution.     

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)...     

Cholesterol dynamics in membranes.

Time-resolved fluorescence anisotropy of the sterol analogue, cholestatrienol, and 13C nuclear magnetic resonance (NMR) spin lattice relaxation time (T1c) measurements of [13C4] labeled cholesterol were exploited to determine the correlation times characterizing the major modes of motion of cholesterol in unsonicated phospholipid multilamellar liposomes. Two modes of motion were found to be important: (a) rotational diffusion and (b) time dependence of the orientation of the director for axial diffusion, or "wobble." From the time-resolved fluorescence anisotropy decays of cholestatrienol in egg phosphatidylcholine (PC) bilayers, a value for tau perpendicular, the correlation time for wobble, of 0.9 x 10(-9) s and a value for S perpendicular, the order parameter characterizing the same motion, of 0.45 s were calculated. Both tau perpendicular and S perpendicular were relatively insensitive to temperature and cholesterol content of the membranes. The T1c measurements of [13C4] labeled cholesterol did not provide a quantitative determination of tau parallel, the correlation time for axial diffusion. T1c from the lipid hydrocarbon chains suggested a value for tau perpendicular similar to that for cholesterol. Steady-state anisotropy measurements and time-resolved anisotropy measurements of cholestatrienol were used to probe sterol behavior in a variety of pure and mixed lipid multilamellar liposomes. Both the lipid headgroups and the lipid hydrocarbons chains contributed to the determination of the sterol environment in the membrane, as revealed by these fluorescence measurements. In particular, effects of the phosphatidylethanolamine (PE) headgroup and of multiple unsaturation in the lipid hydrocarbon chains were observed. However, while the steady-state anisotropy was sensitive to these factors, the time-resolved fluorescence analysis indicated that tau perpendicular was not strongly affected by the lipid composition of the membrane. S perpendicular may be increased by the presence of PE. Both steady-state anisotropy measurements and time-resolved anisotropy measurements of cholestatrienol were used to probe sterol behavior in three biological membranes: bovine rod outer segment (ROS) disk membranes, human erythrocyte plasma membranes, and light rabbit muscle sarcoplasmic reticulum membranes. In the ROS disk membranes the value for S perpendicular was marginally higher than in the PC membranes, perhaps reflecting the influence of PE. The dramatic difference noted was in the value for tau perpendicular. In both the ROS disk membranes and the erythrocyte membranes, tau perpendicular was one-third to one-fifth of tau perpendicular in the phospholipid bilayers. This result may reveal an influence of membrane proteins on sterol behavior.     

Rates of RNA degradation in isolated rat hepatocytes. Effects of amino acids and inhibitors of lysosomal function.

1. RNA degradation in isolated rat hepatocytes was measured as the release of radioactive cytidine from fed rats previously labeled in vivo for 60 h with [6-14C]orotic acid. Rates were determined from the linear accumulation of [14C]cytidine between 30 and 120 min of incubation in the presence of 0.5 mM unlabeled cytidine to suppress reutilization. 2. In the absence of amino acids, rates of RNA degradation in isolated hepatocytes averaged 3.97%/h. A complete mixture of amino acids added at 10-20 times normal plasma concentration inhibited RNA degradation by 65-70%. However, at physiological concentrations of amino acids, RNA degradation in isolated rat hepatocytes was less responsive as compared to perfused rat livers. 3. Numerous and large autophagic vacuoles at various stages of digestion were identified throughout the cytoplasm of isolated hepatocytes after 2 h of incubation in the absence of amino acids. The addition of amino acids at 20 times normal plasma concentration abolished almost completely the appearance of autophagic vacuoles. Furthermore, prophylamine, which accumulates in lysosomes, suppressed RNA degradation by 65% and the inhibitor of autophagic vacuole formation, 3-methyladenine, inhibited 70-80% of the degradation. Taken together, these results strongly suggest a contribution of the lysosomal system in the increase of RNA degradation rates in isolated rat hepatocytes.     

Structure and dynamics of motilin. Time-resolved fluorescence of peptide hormone with single tyrosine residue.

Time-resolved fluorescence and CD spectroscopy were used to characterize the structure and dynamics of the peptide hormone motilin with a single tyrosine residue among its 22 amino acids. CD spectroscopy showed that secondary structure is independent of concentration in the range 1 x 10(-5)-2.6 x 10(-4) M, and of the presence of DOPC lipid vesicles, but is strongly induced by addition of hexafluoroisopropanol. The fluorescence studies with tyrosine as the intrinsic fluorophore, performed at the MAX synchrotron laboratory at Lund, showed that three fluorescence lifetimes (0.4 ns, 1.7 ns and 3.6 ns at 20 degrees C) and two rotational correlation times (0.4 ns and 5 ns at 20 degrees C) were needed to account for the data. The different decay times are interpreted as representing ground-state rotamers interconverting slowly on the ns time scale. The rotational correlation times are ascribed to local angular motion of the tyrosyl ring, and global motion of the whole peptide, respectively.     

13C NMR relaxation times of hepatic glycogen in vitro and in vivo

The field dependence of relaxation times of the C-1 carbon of glycogen was studied in vitro by natural-abundance 13C NMR. T1 is strongly field dependent, while T2 does not change significantly with magnetic field. T1 and T2 were also measured for rat hepatic glycogen enriched with [1-13C]glucose in vivo at 4.7 T, and similar relaxation times were observed as those obtained in vitro at the same field. The in vitro values of T1 were 65 +/- 5 ms at 2.1 T, 142 +/- 10 ms at 4.7 T, and 300 +/- 10 ms at 8.4 T, while T2 values were 6.7 +/- 1 ms at 2.1 T, 9.4 +/- 1 ms at 4.7 T, and 9.5 +/- 1 ms at 8.4 T. Calculations based on the rigid-rotor nearest-neighbor model give qualitatively good agreement with the T1 field dependence with a best-fit correlation time of 6.4 X 10(-9) s, which is significantly smaller than tau M, the estimated overall correlation time for the glycogen molecule (ca. 10(-5) s). A more accurate fit of T1 data using a modified Lipari and Szabo approach indicates that internal fast motions dominate the T1 relaxation in glycogen. On the other hand, the T2 relaxation is dominated by the overall correlation time tau M while the internal motions are almost but not completely unrestricted.     

Tight-binding inhibition of angiogenin and ribonuclease A by placental ribonuclease inhibitor

The dissociation rate constant of the angiogenin-placental ribonuclease inhibitor complex was determined by measuring the release of free angiogenin from the complex in the presence of scavenger for free placental ribonuclease inhibitor (PRI). In 0.1 M NaCl, pH 6, 25 degrees C, this value is 1.3 X 10(-7) s-1 (t1/2 congruent to 60 days). The Ki value for the binding of PRI to angiogenin, calculated from the association and dissociation rate constants, is 7.1 X 10(-16) M. The corresponding values for the interaction of RNase A with PRI, determined by similar means, are both considerably higher: the dissociation rate constant is 1.5 X 10(-5) s-1 (t1/2 = 13 h), and the Ki value is 4.4 X 10(-14) M. Thus, PRI binds about 60 times more tightly to angiogenin than to RNase A. The effect of increasing sodium chloride concentration on the binding of PRI to RNase A was explored by Henderson plots. The Ki value increases to 39 pM in 0.5 M NaCl and to 950 pM in 1 M NaCl, suggesting the importance of ionic interactions. The mode of inhibition of RNase A by PRI was determined by examining the effect of a competitive inhibitor of RNase A, cytidine 2'-phosphate, on the association rate of PRI with RNase A. Increasing concentrations of cytidine 2'-phosphate decrease the association rate in a manner consistent with a competitive mode of inhibition.     

Thermodynamics of the Ca2+ binding to bovine alpha-lactalbumin

Bovine alpha-lactalbumin contains one strong Ca2+-binding site. The free energy (delta G0), enthalpy (delta H0), and entropy (delta S0) of binding of Ca2+ to this site have been calculated from microcalorimetric experiments. The enthalpy of binding was dependent on the metal-free bovine alpha-lactalbumin concentration. At 0.8 mg ml-1, metal-free bovine alpha-lactalbumin delta H0 was -110 +/- 6 kJ mol-1. At this concentration the binding constant was estimated from a mathematical analysis of the titration curves to be greater than 10(7) M-1. This means that delta G0 is smaller than -40 kJ mol-1 and delta S0 is less negative than -235 J.K-1 mol-1. The binding of Ca2+ is therefore enthalpy-driven. From binding experiments as a function of temperature, a delta Cp value of -4.1 kJ.K-1 mol-1 was calculated. This value is dependent on the protein concentration. A tentative explanation for this large value is given.     

Study of molecular dynamics of bovine carbonic anhydrase B by 13C-NMR in two strongly polarizing magnetic fields. I. Intramolecular mobility of polypeptide chains of the native enzyme

The study of the dynamics of enzyme segmental movement is of considerable importance in the understanding of the physics of the catalytic function of these macromolecules, which cannot be adequately described without introduction of intramolecular mobility of their polypeptide chains. At present high resolution [13C]NMR is mostly used as an effective and selective method for the observation of spectral and relaxation parameters that are sensitive to structure, conformation and local motion. The molecular dynamics of bovine carbonic anhydrase B (carbonate hydrolase EC. 4.2.1.1) in the native form was studied. Measurements of the relaxation parameters (T1, T2 and NOE) of the alpha-carbons of the polypeptide chain in two high magnetic fields (4.7 and 11.7 T) were carried out. The model-free approach of Lipari and Szabo to the interpretation of these experimental data show a satisfactory agreement between theory and experiment for these carbon nuclei if an internal degree of motion such as libration or restricted diffusion in a cone with angular amplitude in the 10 degrees less than theta less than or equal to 20 degrees range and an effective correlation time tau e approximately equal to 6 to 7 x 10(-11) S in addition to the tau R = 3 x 10(-8) S reorientation correlation time of the whole molecular is introduced.     

Effects of Li+ transport and intracellular binding on Li+/Mg2+ competition in bovine chromaffin cells

Li(+) transport, intracellular immobilisation and Li(+)/Mg(2+) competition were studied in Li(+)-loaded bovine chromaffin cells. Li(+) influx rate constants, k(i), obtained by atomic absorption (AA) spectrophotometry, in control (without and with ouabain) and depolarising (without and with nitrendipine) conditions, showed that L-type voltage-sensitive Ca(2+) channels have an important role in Li(+) uptake under depolarising conditions. The Li(+) influx apparent rate constant, k(iapp), determined under control conditions by (7)Li NMR spectroscopy with the cells immobilised and perfused, was much lower than the AA-determined value for the cells in suspension. Loading of cell suspensions with 15 mmol l(-1) LiCl led, within 90 min, to a AA-measured total intracellular Li(+) concentration, [Li(+)](iT)=11.39+/-0.56 mmol (l cells)(-1), very close to the steady state value. The intracellular Li(+) T(1)/T(2) ratio of (7)Li NMR relaxation times of the Li(+)-loaded cells reflected a high degree of Li(+) immobilisation in bovine chromaffin cells, similar to neuroblastoma, but larger than for lymphoblastoma and erythrocyte cells. A 52% increase in the intracellular free Mg(2+) concentration, Delta[Mg(2+)](f)=0.27+/-0.05 mmol (l cells)(-1) was measured for chromaffin cells loaded with the Mg(2+)-specific fluorescent probe furaptra, after 90-min loading with 15 mmol l(-1) LiCl, using fluorescence spectroscopy, indicating significant displacement of Mg(2+) by Li(+) from its intracellular binding sites. Comparison with other cell types showed that the extent of intracellular Li(+)/Mg(2+) competition at the same Li(+) loading level depends on intracellular Li(+) transport and immobilisation in a cell-specific manner, being maximal for neuroblastoma cells.     

Evidence for flexibility in the function of ribonuclease A

The dynamic properties of the enzyme ribonuclease A (RNase A) were investigated through the use of solution NMR spin relaxation experiments. As determined by "model-free" analysis, RNase A is conformationally rigid on time scales faster than overall rotational tumbling (picoseconds to nanoseconds). The average order parameter, S(2), for RNase A is 0.910 +/- 0.051. However, 28 of the amino acid residues in RNase A were identified as undergoing chemical exchange on the microsecond to millisecond time scale. For 16 of these residues the microscopic chemical exchange rates, k(ex), were quantitated through the use of the relaxation-compensated CPMG (rcCPMG) experiment. The value of k(ex) was identical for all residues with an average of 1640 s(-1) and is similar to the RNase A k(cat) value of 1900 s(-1). Many of these mobile residues localize to the active site in RNase A and include the catalytically crucial amino acids His119 and Asp121. Additional motion is found in the B1, B2, and P0 subsites, suggesting a coupling of motion between the binding and catalytic sites. The activation energy of the observed millisecond motion was measured by applying the rcCPMG experiment at temperatures of 283, 293, and 298 K and was determined to vary between 3.6 and 7.4 kcal/mol. The measured barrier to conformational motion is similar to the activation barrier for the RNase A catalyzed reaction and thus would not be thermodynamically limiting to catalysis. These studies suggest a correlation of conformational exchange kinetics and thermodynamics derived from NMR measurements with those determined by biochemical means and are suggestive of an important role for flexibility in enzyme function.     

Structural basis for the reaction of 3,5,3''-tri-iodothyronine-specific antibodies with thyroxine-containing thyroglobulin.

A series of human autoantibodies against thyroglobulin (Tg) which exhibit different specificities for iodothyronines were studied. The ability of a thyroxine (T4)-containing peptide (T4P) isolated from human thyroglobulin (Tg) to displace [125I]T3 from human T3-specific autoantisera was 11-50 times greater than that of T4 alone. These antisera therefore strongly recognize amino acids adjacent to T4 in the Tg structure. This was confirmed when a Tg preparation (Tg[0.05]) containing an average of only 0.05 of a T4 residue/molecule and much less T3 had good cross-reactivities with these antisera. Cross-reactivities of other Tg preparations with different T4 contents increased only slowly with increase of T4 content up to a mean of 6.6 residues/molecule and were not proportional to T3 content. In contrast, cross-reactivities with a human T4-specific autoantiserum were strongly dependent on T4 content. Tg[0.05] was 500 times less reactive than T4P and 615 times less than T4. Cross-reactivities rose rapidly as the T4 content of Tg preparations increased from a mean of 0.05 to approx. 1-2 residues/molecule. Thyroxine is therefore a dominant feature of the antigenic site for this antiserum. There was little further increase in cross-reactivities for those Tg preparations containing up to an average of 6.6 residues T4 per molecule, confirming previous conclusions that all T4-containing sites are not immunologically identical and that autoantibodies exhibit a preference for particular sites on Tg. Similar conclusions were reached for a non-specific iodothyronine-binding antiserum. These results indicate that iodothyronine specificity in human autoantisera is not necessarily determined by the iodothyronine present in the immunogenic area, but by the precise site selected by the immune response. T4- or non-specific antibodies have thyroxine as a dominant feature of the antigenic site. T3- specific antibodies have the thyroxine residue as a peripheral feature of the binding site, and it is not necessary to postulate that T3 was part of the immunogen or is required in the epitope. These antisera may have value in mapping the hormonogenic regions in Tg from human and other species.     

Nanosecond fluctuations of the molecular backbone of collagen in hard and soft tissues: a carbon-13 nuclear magnetic resonance relaxation study

We have determined the amplitude of nanosecond fluctuations of the collagen azimuthal orientation in intact tissues and reconstituted fibers from an analysis of 13C NMR relaxation data. We have labeled intact rat calvaria and tibia collagen (mineralized and cross-linked), intact rat tail tendon and demineralized bone collagen (cross-linked), and reconstituted lathyritic (non-cross-linked) chick calvaria collagen with [2-13C]glycine. This label was chosen because one-third of the amino acid residues in collagen are glycine and because the 1H-13C dipolar coupling is the dominant relaxation mechanism. Spin-lattice relaxation times (T1) and nuclear Overhauser enhancements were measured at 15.09 and 62.98 MHz at 22 and -35 degrees C. The measured NMR parameters have been analyzed by using a dynamic model in which the azimuthal orientation of the molecule fluctuates as a consequence of reorientation about the axis of the triple helix. We have shown that if root mean square fluctuations in the azimuthal orientations are small, gamma rms much less than 1 rad, the correlation function decays with a single correlation time tau and T1 depends only upon tau and gamma rms and not the detailed model of motion. Our analysis shows that, at 22 degrees C, tau is in the 1-5-ns range for all samples and gamma rms is 10 degrees, 9 degrees, and 5.5 degrees for the non-cross-linked, cross-linked, and mineralized samples, respectively. At -35 degrees C, gamma rms is less than 3 degrees for all samples. These results show that mineral and low temperature significantly restrict the amplitude of nanosecond motions of the collagen backbone.(ABSTRACT TRUNCATED AT 250 WORDS)     

Carboranyl peptide-antibody conjugates for neutron-capture therapy: preparation, characterization, and in vivo evaluation.

Two model peptides rich in boron and prepared by Merrifield syntheses, dansyl.(nido-CB)2, (1) and dansyl.(nido-CB)10.Lys.Ac (2), where nido-CB represents the alpha-amino acid [nido-7-CH3-8-(CH2)3CH-(NH2)COOH-7,8-C2B9H10]-, were conjugated with the anti-CEA mAb T84.66 using peptide active ester reagents. The dansyl groups provided a means of fluorimetric analysis of mAb conjugates which was augmented by conventional amino acid analyses for nido-CB. The conjugate of 1 contained an average of 63 B atoms per mAb molecule. The mAb conjugate of 2 was chromatographically separated into a strongly fluorescent high molecular weight aggregated fraction (HMW) and a less intensely fluorescent monomeric fraction. Both fractions retained immunoreactivity. The HMW species contained an average of ca. 490 B atoms/mAb molecule, as determined by amino acid analysis. Biodistribution data were collected using nude mice bearing LS174T xenografts and 125I-labeled mAb conjugates. While the lightly B-loaded dipeptide conjugate gave biodistribution results which resembled those of native T84.66 mAb, the undecapeptide conjugate displayed greatly enhanced liver uptake and decreased tumor accretion. These results suggest that as the boron-containing burden on the supporting immunoprotein is greatly increased, as in the case of the T84.66-2 conjugate, loss of circulating conjugate to liver effectively competes with the desired tumor localization. Means which might be taken to circumvent this difficulty have been described elsewhere (ref 15).     

Conformational flexibility of angiotensin II. A carbon-13 spin-lattice relaxation study.

Carbon-13 spin-lattice relaxation times (T1) have been determined for the carbon in the octapeptide hormone [5-isoleucine]-angiotensin II in aqueous solution. Two possible models for molecular motion are considered: isotropic overall motion of the hormone with internal motion of some residues and anisotropic overall molecular motion. The data are interpreted in detail using the former model. The alpha carbons of the peptide backbone are all equally restricted in their motion. The correlation time for overall molecular reorientation, calculated from an everage T1 value of 95 msec for the alpha carbons in the peptide backbone, is ca. 5 times 10-10 sec. The carbons in the side chains are more mobile than those in the peptide backbone, with the exception of the side chain of the Tyr residue which does not undergo rapid segmental motion. We propose that [5-isoleucine]-angiotensin II has a restricted backbone conformation and that the alpha carbons of the N- and C-terminal residues are constrained to nearly the same extent as the remaining alpha carbons in the peptide backbone. Chemical shift data indicate that the Pro residue adopts the trans conformation about the His-Pro bond and that the imidazole ring of His has a strong preference for the N-tau -H tautomer.     

Amino acid and hormonal control of macromolecular turnover in perfused rat liver. Evidence for selective autophagy

The control of RNA degradation by amino acids, insulin, and glucagon was investigated in perfused livers of fed rats previously labeled in vivo with [6-14C] orotic acid; rates were determined from the release of [14C]cytidine in the presence of 0.5 mM cytidine to suppress reutilization. Studies with cyclically perfused livers showed that plasma amino acids at 10 times (10X) normal concentrations inhibited RNA breakdown by 85%. Similar inhibition was obtained with a known regulatory amino acid mixture (Leu, Met, Pro, Trp, and His), whereas leucine alone (0.8 mM) decreased degradation by 47%. Perfusions carried out in the single-pass mode with graded levels of plasma amino acids revealed that the acceleration of RNA degradation over the full range of amino acid deprivation (0 to 10X normal levels) was the same as that for protein breakdown (3.19 and 3.15% h-1, respectively), and both were equally suppressed by insulin (2.4 micrograms h-1). Glucagon (10 micrograms h-1), though, was far less effective in stimulating RNA than protein turnover. A direct comparison of the two dose responses revealed a strong dissociation at 1 and 2 times normal amino acid levels. These findings support the notion that RNA and protein are degraded within a single macroautophagic compartment during amino acid and insulin deprivation. Glucagon, however, appeared to induce a second pathway in which the proportion of sequestered RNA to protein was selectively reduced. Electron micrographs showed that the ratio of vacuoles containing rough as compared with smooth endoplasmic reticulum was decreased by nearly 80% under these conditions.     

RNA degradation in perfused rat liver as determined from the release of [14C]cytidine

The degradation of RNA in the cyclically perfused rat liver was determined from the release of labeled cytidine from RNA that had been previously labeled with [6-14C]orotic acid in vivo. Because cytidine is not appreciably degraded in rat liver (its deamination to uridine is virtually nil) or produced in significant amounts from free 5'-nucleotides, its release will directly reflect net RNA breakdown. This conclusion was substantiated by the fact that the specific radioactivity of released cytidine equaled that of CMP in RNA and remained unchanged for 180 min of perfusion. The initial rate of [14C]cytidine accumulation was slow, but after 10-20 min it increased abruptly by more than 4-fold and remained virtually constant. The addition of 0.5 mM unlabeled cytidine effectively prevented the reutilization of label and increased the rate of labeled cytidine release by an amount representing 13% of the maximal rate of cytidine accumulation. Rates of RNA degradation, measured between 20 and 60 min in the presence of 0.5 mM unlabeled cytidine, averaged 1.00 +/- 0.05 mg h-1 liver-1 (100-g rat), the equivalent of 65% of total RNA per day. This accelerated value, which was about 4-fold larger than the initial rate, is believed to be the direct consequence of amino acid deprivation since, in separate experiments, the increase was completely suppressed by the addition of plasma amino acids (Lardeux, B. R., and Mortimore, G. E. (1987) J. Biol. Chem. 262, 14514-14519). These findings demonstrate the potential value of cytidine as a marker for following moment-to-moment regulatory alterations in RNA degradation in the isolated liver or hepatocyte preparation.     

A detailed analysis of the motions of cholesterol in biological membranes by 2H-NMR relaxation

Spin-lattice relaxation, T1z, measurements of [2,2,3,4,4,6-2H6]cholesterol in model membranes of DMPC were performed as a function of temperature, Larmor frequency and position of labelling in the fused ring system. The results are interpreted according to a hierarchy of motions, such that motion i of correlation time tau i reduces the residual ordering set, characterizing motions i-1, i-2, etc..., by the amount Si = d(2)00(beta i), where beta i is the angle between the axes of motional averaging of motions i and i-1, respectively and d(2)00 is the Wigner rotation matrix element. The appearance of minima in the temperature dependence of T1z for cholesterol, at 46.1 MHz and 30.7 MHz, and the scaling of these T1z (min) according to the orientation of each individual C-2H bond with respect to the axis of motional averaging of cholesterol, allows assignment of the sterol axial rotation to the second fastest motion, characterized by a correlation time of 3.2 X 10(-9) s at 25 degrees C and an activation energy of 32 +/- 5 kJ X mole-1. The fastest motion of cholesterol in DMPC could be a very rapid libration, 'wobbling', which does not contribute significantly to the T1z relaxation of cholesterol at physiological temperatures and Larmor frequencies smaller than 50 MHz, but does reduce the ordering of the cholesterol molecule in DMPC from S0 = 1 to S1 = 0.8, at 25 degrees C.