The Role of Electrostatic Interaction in Triggering the Unraveling of Stable Helix 1 in Normal Prion Protein. A Molecular Dynamics Simulation Investigation

Abstract

The conversion of normal prion protein (PrP^C) into scrapie isoform (PrP^Sc) is a key event in the pathogenesis of prion diseases. However, the conversion mechanism has given rise to much controversy. For instance, there is much debate on the behavior of helix 1 (H1) in the conversion. A series of experiments demonstrated that H1 in isolated state was very stable under a variety of conditions. But, other experiments indicated that helices 2 and 3 rather than H1 were retained in PrP^Sc. In this paper, molecular dynamics (MD) simulation is employed to investigate the dynamic behavior of H1. It is revealed that although the helix 1 of Human PrP^C (HuPrP^C) is very stable in the isolated state, it becomes unstable when incorporated into native HuPrP^C, which likely results from the long-range electrostatic interaction between Asp147 and Arg208 located in the helices 1 and 3, respectively. This explanation is supported by experimental evaluation and MD simulation on D147N mutant of HuPrP^C that the mutant becomes a little more stable than the wild type HuPrP^C. This finding not only help to reconcile the existing debate on the role of helix 1 in the PrP^C→PrP^Sc transition, but also reveals a possible mechanism for triggering the PrP^C→PrP^Sc conversion.     

Application of SAIL phenylalanine and tyrosine with alternative isotope-labeling patterns for protein structure determination

The extensive collection of NOE constraint data involving the aromatic ring signals is essential for accurate protein structure determination, although it is often hampered in practice by the pervasive signal overlapping and tight spin couplings for aromatic rings. We have prepared various types of stereo-array isotope labeled phenylalanines (ε- and ζ-SAIL Phe) and tyrosine (ε-SAIL Tyr) to overcome these problems (Torizawa et al. 2005), and proven that these SAIL amino acids provide dramatic spectral simplification and sensitivity enhancement for the aromatic ring NMR signals. In addition to these SAIL aromatic amino acids, we recently synthesized δ-SAIL Phe and δ-SAIL Tyr, which allow us to observe and assign δ-¹³C/¹H signals very efficiently. Each of the various types of SAIL Phe and SAIL Tyr yields well-resolved resonances for the δ-, ε- or ζ-¹³C/¹H signals, respectively, which can readily be assigned by simple and robust pulse sequences. Since the δ-, ε-, and ζ-proton signals of Phe/Tyr residues give rise to complementary NOE constraints, the concomitant use of various types of SAIL-Phe and SAIL-Tyr would generate more accurate protein structures, as compared to those obtained by using conventional uniformly ¹³C, ¹⁵N-double labeled proteins. We illustrated this with the case of an 18.2 kDa protein, Escherichia coli peptidyl-prolyl cis-trans isomerase b (EPPIb), and concluded that the combined use of ζ-SAIL Phe and ε-SAIL Tyr would be practically the best choice for protein structural determinations.     

Alternative SAIL-Trp for robust aromatic signal assignment and determination of the χ<Subscript>2</Subscript> conformation by intra-residue NOEs

Tryptophan (Trp) residues are frequently found in the hydrophobic cores of proteins, and therefore, their side-chain conformations, especially the precise locations of the bulky indole rings, are critical for determining structures by NMR. However, when analyzing [U–¹³C,¹⁵N]-proteins, the observation and assignment of the ring signals are often hampered by excessive overlaps and tight spin couplings. These difficulties have been greatly alleviated by using stereo-array isotope labeled (SAIL) proteins, which are composed of isotope-labeled amino acids optimized for unambiguous side-chain NMR assignment, exclusively through the ¹³C–¹³C and ¹³C–¹H spin coupling networks (Kainosho et al. in Nature 440:52–57, 2006). In this paper, we propose an alternative type of SAIL-Trp with the [ζ2,ζ3-²H₂; δ1,ε3,η2-¹³C₃; ε1-¹⁵N]-indole ring ([¹²C_γ, ¹²C_ε2] SAIL-Trp), which provides a more robust way to correlate the ¹H_β, ¹H_α, and ¹H_N to the ¹H_δ1 and ¹H_ε3 through the intra-residue NOEs. The assignment of the ¹H_δ1/¹³C_δ1 and ¹H_ε3/¹³C_ε3 signals can thus be transferred to the ¹H_ε1/¹⁵N_ε1 and ¹H_η2/¹³C_η2 signals, as with the previous type of SAIL-Trp, which has an extra ¹³C at the C_γ of the ring. By taking advantage of the stereospecific deuteration of one of the prochiral β-methylene protons, which was ¹H_β2 in this experiment, one can determine the side-chain conformation of the Trp residue including the χ₂ angle, which is especially important for Trp residues, as they can adopt three preferred conformations. We demonstrated the usefulness of [¹²C_γ,¹²C_ε2] SAIL-Trp for the 12 kDa DNA binding domain of mouse c-Myb protein (Myb-R2R3), which contains six Trp residues.     

Investigation of exchange couplings in [Fe3S4]+ clusters by electron spin-lattice relaxation

3 S₄]⁺, S=1/2, composed of three, antiferromagnetically coupled high-spin ferric ions) by continuous wave (CW) and pulsed EPR techniques: Azotobacter vinelandii ferredoxin I, Desulfovibrio gigas ferredoxin II, and the 3Fe forms of Pyrococcus furiosus ferredoxin and aconitase. The 35 GHz (Q-band) CW EPR signals are simulated to yield experimental g tensors, which either had not been reported, or had been reported only at X-band microwave frequency. Pulsed X- and Q-band EPR techniques are used to determine electron spin-lattice (T ₁, longitudinal) relaxation times at several positions on the samples' EPR envelope over the temperature range 2–4.2 K. The T ₁ values vary sharply across the EPR envelope, a reflection of the fact that the envelope results from a distribution in cluster properties, as seen earlier as a distribution in g ₃ values and in ⁵⁷ Fe hyperfine interactions, as detected by electron nuclear double resonance spectroscopy. The temperature dependence of 1/T ₁ is analyzed in terms of the Orbach mechanism, with relaxation dominated by resonant two-phonon transitions to a doublet excited state at ∼20 cm⁻¹ above the doublet ground state for all four of these 3Fe proteins. The experimental EPR data are combined with previously reported ⁵⁷Fe hyperfine data to determine electronic spin exchange-coupling within the clusters, following the model of Kent et al. Their model defines the coupling parameters as follows: J ₁₃=J, J ₁₂=J(1+ε′), J ₂₃=J(1+ε), where J _ij is the isotropic exchange coupling between ferric ions i and j, and ε and ε′ are measures of coupling inequivalence. We have extended their theory to include the effects of ε′≠0 and thus derived an exact expression for the energy of the doublet excited state for any ε, ε′. This excited state energy corresponds roughly to ε J and is in the range 5–10 cm⁻¹ for each of these four 3Fe proteins. This magnitude of the product ε J, determined by our time-domain relaxation studies in the temperature range 2–4 K, is the same as that obtained from three other distinct types of study: CW EPR studies of spin relaxation in the range 5.5–50 K, NMR studies in the range 293–303 K, and static susceptibility measurements in the range 1.8–200 K. We suggest that an apparent disagreement as to the individual values of J and ε be resolved in favor of the values obtained by susceptibility and NMR (J≳200 cm⁻¹ and ε≳0.02 cm⁻¹ ), as opposed to a smaller J and larger ε as suggested in CW EPR studies. However, we note that this resolution casts doubt on the accepted theoretical model for describing the distribution in magnetic properties of 3Fe clusters. Received: 23 December 1999 / Accepted: 8 March 2000     

Quantification of protein backbone hydrogen-deuterium exchange rates by solid state NMR spectroscopy

We present the quantification of backbone amide hydrogen-deuterium exchange rates (HDX) for immobilized proteins. The experiments make use of the deuterium isotope effect on the amide nitrogen chemical shift, as well as on proton dilution by deuteration. We find that backbone amides in the microcrystalline α-spectrin SH3 domain exchange rather slowly with the solvent (with exchange rates negligible within the individual ¹⁵N–T ₁ timescales). We observed chemical exchange for 6 residues with HDX exchange rates in the range from 0.2 to 5 s⁻¹. Backbone amide ¹⁵N longitudinal relaxation times that we determined previously are not significantly affected for most residues, yielding no systematic artifacts upon quantification of backbone dynamics (Chevelkov et al. 2008b). Significant exchange was observed for the backbone amides of R21, S36 and K60, as well as for the sidechain amides of N38, N35 and for W41ε. These residues could not be fit in our previous motional analysis, demonstrating that amide proton chemical exchange needs to be considered in the analysis of protein dynamics in the solid-state, in case D₂O is employed as a solvent for sample preparation. Due to the intrinsically long ¹⁵N relaxation times in the solid-state, the approach proposed here can expand the range of accessible HDX rates in the intermediate regime that is not accessible so far with exchange quench and MEXICO type experiments.     

Influence of the pathogenic mutations T188K/R/A on the structural stability and misfolding of human prion protein: Insight from molecular dynamics simulations

Background

Prion diseases are associated with a conformational switch for PrP from PrP^C to PrP^Sc. Many genetic mutations are linked with prion diseases, such as mutations T188K/R/A with fCJD.

Scope of review

MD simulations for the WT PrP and its mutants were performed to explore the underlying dynamic effects of T188 mutations on human PrP. Although the globular domains are fairly conserved, the three mutations have diverse effects on the dynamics properties of PrP, including the shift of H1, the elongation of native β-sheet and the conversion of S2-H2 loop to a 3₁₀ helix.

Major conclusions

Our present study indicates that the three mutants for PrP may undergo different pathogenic mechanisms and the realistic atomistic simulations can provide insights into the effects of disease-associated mutations on PrP dynamics and stability, which can enhance our understanding of how mutations induce the conversion from PrP^C to PrP^Sc.General significanceOur present study helps to understand the effects of T188K/R/A mutations on human PrP: despite the three pathogenic mutations almost do not alter the native structure of PrP, but perturb its stability. This instability may further modulate the oligomerization pathways and determine the features of the PrP^Sc assemblies.     

Synthesis, characterization, and reaction pathways for the formation of a GMP adduct of a cytotoxic thiocyanato ruthenium arene complex

The organoruthenium complex [(η⁶-hmb)Ru(en)(Cl)][PF₆] (hmb is hexamethylbenzene, en is ethylenediamine) undergoes facile aquation and then reacts with KSCN in unbuffered solution to give the S-coordinated thiocyanato product [(η⁶-hmb)Ru(en)(S-SCN)]⁺ which slowly converts to the thermodynamically favored N-bound complex [(η⁶-hmb)Ru(en)(N-NCS)]⁺ (1 ⁺). Complex 1 was synthesized and characterized by X-ray crystallography and mass spectrometry. Despite its lack of hydrolysis over 24 h, complex 1 exhibits moderate cytotoxicity (IC₅₀ 24 μM) towards the human ovarian cancer cell line A2780, comparable with that of the chlorido analogue which is thought to be activated (towards potential target DNA) via a rapid aquation (Wang et. al. in Proc Natl Acad Sci USA 102:18269–18274, 2005). Detailed kinetic studies suggest that complex 1 binds to guanosine 5′-monophosphate (GMP) through direct N7 substitution of the N-bound SCN ligand. In the presence of a high concentration of chloride (104 mM), however, complex 1 may bind partly to GMP via Cl substitution.     

1H, 13C and 15N NMR assignments of the C1A and C1B subdomains of PKC-delta

The Protein Kinase C family of enzymes is a group of serine/threonine kinases that play central roles in cell-cycle regulation, development and cancer. A key step in the activation of PKC is translocation to membranes and binding of membrane-associated activators including diacylglycerol (DAG). Interaction of novel and conventional isotypes of PKC with DAG and phorbol esters occurs through the two C1 regulatory domains (C1A and C1B), which exhibit distinct ligand binding selectivity that likely controls enzyme activation by different co-activators. PKC has also been implicated in physiological responses to alcohol consumption and it has been proposed that PKCα (Slater et al. J Biol Chem 272(10):6167–6173, 1997; Slater et al. Biochemistry 43(23):7601–7609, 2004), PKCε (Das et al. Biochem J 421(3):405–413, 2009) and PKCδ (Das et al. J Biol Chem 279(36):37964–37972, 2004; Das et al. Protein Sci 15(9):2107–2119, 2006) contain specific alcohol-binding sites in their C1 domains. We are interested in understanding how ethanol affects signal transduction processes through its affects on the structure and function of the C1 domains of PKC. Here we present the ¹H, ¹⁵N and ¹³C NMR chemical shift assignments for the Rattus norvegicus PKCδ C1A and C1B proteins.     

Low-frequency resonance Raman studies of the H(M202)G cavity mutant of bacterial photosynthetic reaction centers

Low-frequency (90–435 cm⁻¹) NIR-excitation (875–900 nm) resonance Raman (RR) studies are reported for the H(M202)G cavity mutant of bacterial photosynthetic reaction centers (RCs) from Rb. sphaeroides that was first described by Goldsmith et al. [(1996) Biochemistry 35: 2421–2428]. In this mutant, the His residue that axially ligates the Mg ion of the M-side bacteriochlorophyll (BChl) of the special pair primary donor (P) is replaced by a non-ligating Gly residue. Regardless, the Mg ion of P_M in the H(M202)G RCs remains pentacoordinates and is presumably ligated by a water molecule, although this axial ligand has not been definitively identified. The low-frequency RR studies of the H(M202)G RCs are accompanied by studies of RCs exchanged with D₂O and incubated with imidazole (Im). The RR studies of the cavity mutant RCs reveal the following: (1) The structure of P_M in the H(M202)G RCs is different from that of the wild-type, consistent with an altered BChl core. (2) A water ligand for P_M in the H(M202)G RCs is generally consistent with the low-frequency RR spectra. The Mg-OH₂ stretching vibration is tentatively assigned to a band at 318 cm⁻¹, a frequency higher than that of the Mg-His stretch of the native pigment (∼ ∼235 cm⁻¹). (3) The BChl core structure of P_M in the cavity mutant is rendered similar (but not identical) to that of the wild-type when the adventitious water axial ligand is replaced by Im. (4) Exchange with D₂O results in more global structural changes, likely involving the protein, which in turn affect the structure of the BChls in P. (5) Assignment of the low-frequency vibrational spectrum of P is generally more complex than originally suggested.     

Dynamics of a truncated prion protein,PrP(113–231), from 15N NMR relaxation: Order parameters calculated and slow conformational fluctuations localized to a distinct region

Prion diseases are associated with the misfolding of the prion protein (PrP^C) from a largely α‐helical isoform to a β‐sheet rich oligomer (PrP^Sc). Flexibility of the polypeptide could contribute to the ability of PrP^C to undergo the conformational rearrangement during PrP^C–PrP^Sc interactions, which then leads to the misfolded isoform. We have therefore examined the molecular motions of mouse PrP^C, residues 113–231, in solution, using ¹⁵N NMR relaxation measurements. A truncated fragment has been used to eliminate the effect of the 90‐residue unstructured tail of PrP^C so the dynamics of the structured domain can be studied in isolation. ¹⁵N longitudinal (T₁) and transverse relaxation (T₂) times as well as the proton‐nitrogen nuclear Overhauser effects have been used to calculate the spectral density at three frequencies, 0, ω_N, and 0.87ω_H. Spectral densities at each residue indicate various time‐scale motions of the main‐chain. Even within the structured domain of PrP^C, a diverse range of motions are observed. We find that removal of the tail increases T₂ relaxation times significantly indicating that the tail is responsible for shortening of T₂ times in full‐length PrP^C. The truncated fragment of PrP has facilitated the determination of meaningful order parameters (S²) from the relaxation data and shows for the first time that all three helices in PrP^C have similar rigidity. Slow conformational fluctuations of mouse PrP^C are localized to a distinct region that involves residues 171 and 172. Interestingly, residues 170–175 have been identified as a segment within PrP that will form a steric zipper, believed to be the fundamental amyloid unit. The flexibility within these residues could facilitate the PrP^C–PrP^Sc recognition process during fibril elongation.     

Structure and dynamics of photosynthetic membrane-bound proteins in Rhodobacter Sphaeroides,studied with solid-state NMR spectroscopy

The photosynthetic purple bacteria such as Rb. sphaeroides possesses an intracytoplasmic membrane (ICM) and a variety of pigment-binding membrane proteins located in the ICM, acting as photoreceptor. Such photosynthetic apparatus is concentrated in the ICM. It is composed of three multimeric membrane-bound proteins; light-harvesting complexes (LH 1, LH 2), a reaction center (RC) and a cytochrome b/c1 complex. We have purified these membranes, which are called chromatophores, and characterized the structure and dynamics of the photosynthetic membrane-bound proteins by means of multi-nuclear solid state NMR. First, the isotropic chemical shift of carbonyl carbons in natural abundance and [1-¹³C] Phe labeled chromatophores indicates that the membrane-bound proteins take mainly the helical conformation. Second, the chemical shifts of side-chain resonances of uniformly ¹⁵N-labeled chromatophores indicate the side-chain histidine residue is mainly hydrogen bonded, whereas structural heterogeneity of arginine and lysine side-chains are probed by those wide distribution of ¹⁵N shifts. Thirdly, the [β-²H₃]Ala and [ε-²H₂]Tyr labeling of the chromatophores are performed and dynamics of the [β-²H]Ala and the [ε-²H₂]Tyr labeled chromatophores are studied by means of ²H solid state NMR. The dynamics of [β-²H₃]Ala is found to be a 10⁸Hz three-site jump motion with 10° liberation along the Cα-Cβ bond axis. The ²H-NMR powder pattern spectrum of [ε-²H₂] Tyr labeled chromatophores was interpreted with an averaged correlation time of 5×10⁵ Hz with 180° two-fold flips, the result of the averaging of two kinds of split spectra in terms of motional time scale. This revised version was published online in June 2006 with corrections to the Cover Date.     

Comparing Membrane Simulations to Scattering Experiments: Introducing the SIMtoEXP Software

SIMtoEXP is a software package designed to facilitate the comparison of biomembrane simulations with experimental X-ray and neutron scattering data. It has the following features: (1) Accepts number density profiles from simulations in a standard but flexible format. (2) Calculates the electron density ε(z) and neutron scattering length density ν(z) profiles along the z direction (i.e., normal to the membrane) and their respective Fourier transforms (i.e., F _ε [q _z ] and F _ν [q _z ]). The resultant four functions are then displayed graphically. (3) Accepts experimental F _ε (q _z ) and F _ν (q _z ) data for graphical comparison with simulations. (4) Allows for lipids and other large molecules to be parsed into component groups by the user and calculates the component volumes following Petrache et al. (Biophys J 72:2237–2242, 1997). The software then calculates and displays the contributions of each component group as volume probability profiles, ρ(z), as well as the contributions of each component to ε(z) and ν(z).     

[Pt(dien)]2+ migrates intramolecularly from methionine S to imidazole Nz 2 in the peptides H-His-Gly-Met-OH and Ac-His-Ala-Ala-Ala-Met-NHPh

The pH- and time-dependent reaction of [Pt(dien)(H₂O)]²⁺ with the methionine- and histidine-containing peptides H-His-Gly-Met-OH and Ac-His-Ala-Ala-Ala-Met-NHPh at 313 K has been investigated by HPLC and NMR spectroscopy. For both peptides, initial relatively rapid formation of the kinetically favoured methionine S-bound complex is followed by slow intramolecular migration of the [Pt(dien)]²⁺ fragment to imidazole N_{ε 2} (or, in the case of H-His-Gly-Met-OH, to a much lesser extent to the competing imidazole N_{δ 1}) of the histidine side chain over a period of 500 h. Time-dependent studies for the pentapeptide at pH 8.0 demonstrate that this isomerization can take place by either direct S→N_{ε 2} migration or by a two-step mechanism involving initial N_{ε 2} coordination of a second [Pt(dien)]²⁺ fragment and subsequent cleavage of the orginal Pt-S bond in the resulting dinuclear complex. The rate of κS/κN _{ε 2} isomerization is markedly reduced on lowering the pH to 5.1. Received: 26 February 1999 / Accepted: 14 April 1999     

Smad3 contributes to positioning of proliferating cells in colonic crypts by inducing EphB receptor protein expression

In prion diseases cellular prion protein (PrP^C) undergoes conformational transition into the β-sheet-rich form (PrP^Sc). PrP^C consists of the disordered N-terminal part and a C-terminal globular domain containing three α-helices (H1, H2, H3) and an antiparallel beta sheet (B1, B2). B2–H2 loop, which has a focal role in the species barrier, contains the highest density of asparagine (N) and glutamine (Q) residues in the whole sequence. Q/N-rich domains are essential for the conversion of yeast prions. We investigated the role of Q/N residues in the B2–H2 loop in PrP conversion. We prepared mouse PrP mutants with increasing number of consecutive Q/N residues in the B2–H2 loop. Stability of the mutants decreased with the increasing number of inserted glutamines. In vitro conversion of mutants yielded fibrils of similar morphology as the wild-type PrP. Q/N mutants accelerated fibrillization in comparison to the wild-type PrP, with mutant containing the most glutamines having the shortest lag phase. The effect of Q/N residues was specific for the B2–H2 loop and was not due to simple increase in flexibility as the introduction of Gly-Ser or Ala residues slowed the conversion despite their decreased stability. Our results thus suggest that Q/N residues in the B2–H2 loop of PrP promote protein conversion and may represent a link to conversion of Q/N-rich prions.     

Spectroscopic and computational investigation of three Cys-to-Ser mutants of nickel superoxide dismutase: insight into the roles played by the Cys2 and Cys6 active-site residues

Nickel-dependent superoxide dismutase (NiSOD) is a member of a class of metalloenzymes that protect aerobic organisms from the damaging superoxide radical (O₂ ^·−). A distinctive and fascinating feature of NiSOD is the presence of active-site nickel–thiolate interactions involving the Cys2 and Cys6 residues. Mutation of one or both Cys residues to Ser prevents catalysis of O₂ ^·−, demonstrating that both residues are necessary to support proper enzymatic activity (Ryan et al., J Biol Inorg Chem, 2010). In this study, we have employed a combined spectroscopic and computational approach to characterize three Cys-to-Ser (Cys → Ser) mutants (C2S, C6S, and C2S/C6S NiSOD). Similar electronic absorption and magnetic circular dichroism spectra are observed for these mutants, indicating that they possess nearly identical active-site geometric and electronic structures. These spectroscopic data also reveal that the Ni²⁺ ion in each mutant adopts a high-spin (S = 1) configuration, characteristic of a five- or six-coordinate ligand environment, as opposed to the low-spin (S = 0) configuration observed for the four-coordinate Ni²⁺ center in the native enzyme. An analysis of the electronic absorption and magnetic circular dichroism data within the framework of density functional theory computations performed on a series of five- and six-coordinate C2S/C6S NiSOD models reveals that the active site of each Cys → Ser mutant possesses an essentially six-coordinate Ni²⁺ center with a rather weak axial bonding interaction. Factors contributing to the lack of catalytic activity displayed by the Cys → Ser NiSOD mutants are explored.     

Local Osmosis and Isotonic Transport

Osmotically driven water flow, u (cm/s), between two solutions of identical osmolarity, c_o (300 mM in mammals), has a theoretical isotonic maximum given by u = j/c_o, where j (moles/cm²/s) is the rate of salt transport. In many experimental studies, transport was found to be indistinguishable from isotonic. The purpose of this work is to investigate the conditions for u to approach isotonic. A necessary condition is that the membrane salt/water permeability ratio, ε, must be small: typical physiological values are ε = 10⁻³ to 10⁻⁵, so ε is generally small but this is not sufficient to guarantee near-isotonic transport. If we consider the simplest model of two series membranes, which secrete a tear or drop of sweat (i.e., there are no externally-imposed boundary conditions on the secretion), diffusion is negligible and the predicted osmolarities are: basal = c_o, intracellular ≈ (1 + ε)c_o, secretion ≈ (1 + 2ε)c_o, and u ≈ (1 − 2ε)j/c_o. Note that this model is also appropriate when the transported solution is experimentally collected. Thus, in the absence of external boundary conditions, transport is experimentally indistinguishable from isotonic. However, if external boundary conditions set salt concentrations to c_o on both sides of the epithelium, then fluid transport depends on distributed osmotic gradients in lateral spaces. If lateral spaces are too short and wide, diffusion dominates convection, reduces osmotic gradients and fluid flow is significantly less than isotonic. Moreover, because apical and basolateral membrane water fluxes are linked by the intracellular osmolarity, water flow is maximum when the total water permeability of basolateral membranes equals that of apical membranes. In the context of the renal proximal tubule, data suggest it is transporting at near optimal conditions. Nevertheless, typical physiological values suggest the newly filtered fluid is reabsorbed at a rate u ≈ 0.86 j/c_o, so a hypertonic solution is being reabsorbed. The osmolarity of the filtrate c_F (M) will therefore diminish with distance from the site of filtration (the glomerulus) until the solution being transported is isotonic with the filtrate, u = j/c_F.With this steady-state condition, the distributed model becomes approximately equivalent to two membranes in series. The osmolarities are now: c_F ≈ (1 − 2ε)j/c_o, intracellular ≈ (1 − ε)c_o, lateral spaces ≈ c_o, and u ≈(1 + 2ε)j/c_o. The change in c_F is predicted to occur with a length constant of about 0.3 cm. Thus, membrane transport tends to adjust transmembrane osmotic gradients toward εc_o, which induces water flow that is isotonic to within order ε. These findings provide a plausible hypothesis on how the proximal tubule or other epithelia appear to transport an isotonic solution.     

Entropy budgets of deciduous plant leaves and a theorem of oscillating entropy production

From an energy budget of a deciduous plant leaf in moderate conditions, entropy fluxes into or out of the leaf due to solar radiation, infrared radiation, evaporation of water and heat conduction are calculated. Net entropy flow into the leaf is negative. On the assumption that the entropy in the leaf is in a steady state, the entropy production in the typical deciduous leaf in moderate conditions [the solar energy absorbed by both sides of the leaf isE _solar=0.0602 (J cm⁻² s⁻¹)] becomesS _prod=1.8×10⁻⁴ (J cm⁻² s⁻¹ K⁻¹). The positiveness of the entropy production shows that the Second Law of Thermodynamics certainly holds in the plant leaf. Entropy productions in other conditions are also calculated. The entropy production in the leafS _prod becomes a linear function of the solar energy absorbed by the leafE _solar:S _prod≈-(29.5E _solar)×10⁻⁴. A theorem is presented: the entropy production in plant leaves oscillates during the period of one day, paralleling the daily solar energy absorbed by leaves.     

RNA and CuCl2 induced conformational changes of the recombinant ovine prion protein

Prion diseases are a group of neurodegenerative illnesses caused by conformational conversion of benign, α-helix rich cellular prion protein (PrP^C) into the highly stable, β-sheet rich scrapie prion protein (PrP^Sc) isoform. To date, the role of RNA on the conformational conversion of ovine prion protein in vitro remains unknown. To examine the effect of the interaction between RNA and PrP^C, conformations of recombinant ovine prion protein PrP^23–256 (OvPrP^23–256) binding various concentrations of RNA were analyzed by circular dichroism (CD) spectrum. The results indicated that the conformational conversion of OvPrP^23–256 was triggered by RNA with a decrease in α-helix content and increase in β-sheet. Moreover, the conformation of OvPrP^23–256 interacting with both RNA and CuCl₂ was also examined by CD spectrum, which showed that α-helix content decreased while β-sheet increased dramatically. Proteinase K digestion assay disclosed that the recombinant ovine PrP^C acquired PK resistance after RNA and/or Cu²⁺ treatment. It confirmed that the RNA/Cu²⁺ treatment in vitro altered the biochemical properties of ovine PrP^C. The implication of this finding, with respect to PrP^Sc, is that a dysfunctional state of a normal physiological process possibly facilitates diseases. The information gained from this study may provide useful approaches to study the pathogenesis of prion diseases.     

Thermoluminescence and fluorescence study of changes in Photosystem II photochemistry in desiccating barley leaves

An effect of desiccation (a decrease of relative water content from 97% to 10% within 35 h) on Photosystem II was studied in barley leaf segments (Hordeum vulgare L. cv. Akcent) using chlorophyll a fluorescence and thermoluminescence (TL). The O-J-I-P fluorescence induction curve revealed a decrease of F_P and a slight shift of the J step to a shorter time with no change in its height. The analysis of the fluorescence decline after a saturating light flash revealed an increased portion of slow exponential components with increasing desiccation. The TL bands obtained after excitation by continuous light were situated at about –27°C (Z_v band – recombination of P680⁺Q_A ⁻), –14 °C (A band – S₃Q_A ⁻), +12 °C (B band – S_2/3Q_B ⁻) and +45 °C (C band – TyrD⁺Q_A ⁻). The bands related to the S-states of oxygen evolving complex (A and B) were reduced by desiccation and shifted to higher and lower temperatures, respectively. In accordance with this, the band observed at about +27 °C (S₂Q_B ⁻) after excitation by 1 flash fired at –10 °C and band at about +20 °C (S_2/3Q_B ⁻) after 2 flashes decreased with increasing water deficit and shifted to lower temperatures. A new band around 5 °C appeared in both regimes of TL excitation for a relative water content of under 42% and was attributed to the Q band (S₂Q_A ⁻). It is suggested that under desiccation, an inhibition of the formation of S₂- and S₃-states in OEC occurred simultaneously with a lowering of electron transport on the acceptor side of PS II. The temperature down-shift of the TL bands obtained after the flash excitation was induced at the initial phases of water stress, indicating a decrease of the activation energy for the S_2/3Q_B ⁻recombination. This revised version was published online in June 2006 with corrections to the Cover Date.     

Measurement of 15N relaxation in the detergent-solubilized tetrameric KcsA potassium channel

A set of TROSY-HNCO (tHNCO)-based 3D experiments is presented for measuring ¹⁵N relaxation parameters in large, membrane-associated proteins, characterized by slow tumbling times and significant spectral overlap. Measurement of backbone ¹⁵N R ₁, R _1ρ, ¹⁵N–{¹H} NOE, and ¹⁵N CSA/dipolar cross correlation is demonstrated and applied to study the dynamic behavior of the homotetrameric KcsA potassium channel in SDS micelles under conditions where this channel is in the closed state. The micelle-encapsulated transmembrane domain, KcsA^TM, exhibits a high degree of order, tumbling as an oblate ellipsoid with a global rotational correlation time, τ_c = 38 ± 2.5 ns, at 50 °C and a diffusion anisotropy, , corresponding to an aspect ratio a/b ≥ 1.4. The N- and C-terminal intracellular segments of KcsA exhibit considerable internal dynamics (S ² values in the 0.2–0.45 range), but are distinctly more ordered than what has been observed for unstructured random coils. Relaxation behavior in these domains confirms the position of the C-terminal helix, and indicates that in SDS micelles, this amphiphilic helix does not associate into a stable homotetrameric helical bundle. The relaxation data indicate the absence of elevated backbone dynamics on the ps–ns time scale for the 5-residue selectivity filter, which selects K⁺ ions to enter the channel. Electronic Supplementary Material Supplementary material is available to authorised users in the online version of this article at . An erratum to this article can be found at