Protein Brownian Rotation at the Glass Transition Temperature of a Freeze-Concentrated Buffer Probed by Superparamagnetic Nanoparticles

For applications from food science to the freeze-thawing of proteins it is important to understand the often complex freezing behavior of solutions of biomolecules. Here we use a magnetic method to monitor the Brownian rotation of a quasi-spherical cage-shaped protein, apoferritin, approaching the glass transition T_g in a freeze-concentrated buffer (Tris-HCl). The protein incorporates a synthetic magnetic nanoparticle (Co-doped Fe₃O₄ (magnetite)). We use the magnetic signal from the nanoparticles to monitor the protein orientation. As T decreases toward T_g of the buffer solution the protein’s rotational relaxation time increases exponentially, taking values in the range from a few seconds up to thousands of seconds, i.e., orders of magnitude greater than usually accessed, e.g., by NMR. The longest relaxation times measured correspond to estimated viscosities >2 MPa s. As well as being a means to study low-temperature, high-viscosity environments, our method provides evidence that, for the cooling protocol used, the following applies: 1), the concentration of the freeze-concentrated buffer at T_g is independent of its initial concentration; 2), little protein adsorption takes place at the interface between ice and buffer; and 3), the protein is free to rotate even at temperatures as low as 207 K.     

Adverse effect of cake collapse on the functional integrity of freeze-dried bull spermatozoa

Under optimal freeze-drying conditions, solutions exhibit a cake-like porous structure. However, if the solution temperature is higher than the glass transition temperature of the maximally freeze-concentrated phase (T_g′) during drying phase, the glassy matrix undergoes viscous flow, resulting in cake collapse. The purpose of the present study was to investigate the effect of cake collapse on the integrity of freeze-dried bull spermatozoa. In a preliminary experiment, factors affecting the T_g′ of conventional EGTA buffer (consisting of Tris–HCl, EGTA and NaCl) were investigated in order to establish the main experimental protocol because EGTA buffer T_g′ was too low (−45.0 °C) to suppress collapse. Modification of the EGTA buffer composition by complete removal of NaCl and addition of trehalose (mEGTA buffer) resulted in an increase of T_g′ up to −27.7 °C. In the main experiment, blastocyst yields after ooplasmic injection of freeze-dried sperm preserved in collapsed cakes (drying temperature: 0 or −15 °C) were significantly lower than those of sperm preserved in non-collapsed cake (drying temperature: −30 °C). In conclusion, freeze-dried cake collapse may be undesirable for maintaining sperm functions to support embryonic development, and can be inhibited by controlling both T_g′ of freeze-drying buffer and temperature during the drying phase.     

Magnetic resonance study of freezing damage development in rat liver tissue.

Cryolesions were produced by contact cryoprobes on male Wistar rat livers. The development of freezing damage was followed in vivo for 24 hr by morphological examinations, proton spin lattice relaxation times T₁, and paramagnetic center concentration measurements. Significant proton T₁ increase, related to an increased tissue water content, as well as a concentration decrease of the paramagnetic centers, was observed for the cryolesion, as compared to the undamaged liver tissue of the same animal. The concentration decrease was observed for the g = 2.00 free radicals and g = 1.94 reduced state iron protein centers, specified by the parameter g indicating the position of their absorption lines in the electron paramagnetic resonance spectrum.It was also found that the rate of damage development following a single freezethaw cycle depends significantly on the cooling capacity of the cryoprobe. The final changes produced by 6- and 4-mm-diameter liquid nitrogen-cooled cryotips are comparable, but the development of damage was different.     

A broad glass transition in hydrated proteins

We performed Raman and Brillouin scattering measurements to estimate glass transition temperature, T_g, of hydrated protein. The measurements reveal very broad glass transition in hydrated lysozyme with approximate T_g ∼ 180 ± 15 K. This result agrees with a broad range of T_g ∼ 160–200 K reported in literature for hydrated globular proteins and stresses the difference between behavior of hydrated biomolecules and simple glass-forming systems. Moreover, the main structural relaxation of the hydrated protein system that freezes at T_g ∼ 180 K remains unknown. We emphasize the difference between the “dynamic transition”, known as a sharp rise in mean-squared atomic displacement <r²> at temperatures around T_D ∼ 200–230 K, and the glass transition. They have different physical origin and should not be confused.     

Simultaneous Measurements of Solvent Dynamics and Functional Kinetics in a Light-Activated Enzyme

Solvent fluctuations play a key role in controlling protein motions and biological function. Here, we have studied how individual steps of the reaction catalyzed by the light-activated enzyme protochlorophyllide oxidoreductase (POR) couple with solvent dynamics. To simultaneously monitor the catalytic cycle of the enzyme and the dynamical behavior of the solvent, we designed temperature-dependent UV-visible microspectrophotometry experiments, using flash-cooled nanodroplets of POR to which an exogenous soluble fluorophore was added. The formation and decay of the first two intermediates in the POR-catalyzed reaction were measured, together with the solvent glass transition and the buildup of crystalline ice at cryogenic temperatures. We find that formation of the first intermediate occurs below the glass transition temperature (T_g), and is not affected by changes in solvent dynamics induced by modifying the glycerol content. In contrast, formation of the second intermediate occurs above T_g and is influenced by changes in glycerol concentration in a manner remarkably similar to the buildup of crystalline ice. These results suggest that internal, nonslaved protein motions drive the first step of the POR-catalyzed reaction whereas solvent-slaved motions control the second step. We propose that the concept of solvent slaving applies to complex enzymes such as POR.     

The State of Water in Muscle Tissue as Determined by Proton Nuclear Magnetic Resonance

The nuclear magnetic resonance (NMR) of water protons in live and glycerinated muscle, suspensions of glycerinated myofibrils, and solutions of several muscle proteins has been studied. T₁ and T₂, measured on partially hydrated proteins by pulsed spin-echo techniques, decreased as the ratio of water to protein decreased, showing that the water which is tightly bound by the protein has short relaxation times. In live muscle fibers the pulse techniques showed that, after either a 180 or a 90° pulse, the relaxation of the magnetization is described by a single exponential. This is direct evidence that a fast exchange of protons occurs among the phases of the intracellular water. The data can be fitted with a model in which the bulk of the muscle water is in a phase which has properties similar to those of a dilute salt solution, while less than 4-5% of the total water is bound to the protein surface and has short relaxation times. Measurements of T₁ and T₂ in protein solutions showed that no change in the proton relaxation times occurred when heavy meromyosin was bound to actin, when myofibrils were contracted with adenosine triphosphate (ATP), or when globular actin was polymerized.     

Thermal Properties of Freeze-Concentrated Sugar-Phosphate Solutions

In order to understand the effect of phosphate salts on the freeze-concentrated glass-like transition temperature (T _g′) of aqueous sugar solutions, two types of sugar (glucose and maltose) and five types of phosphate salts (Na₃PO₄, Na₄P₂O₇, Na₅P₃O₁₀, K₃PO₄, and K₄P₂O₇) were employed, and the thermal properties of various sugar-phosphate aqueous systems were investigated using differential scanning calorimetry. The T _g′ of glucose increased with increasing sodium phosphates up to a certain phosphate ratio, decreasing thereafter. The maximum T _g′ value was slightly higher in the order of Na₃PO₄ > Na₄P₂O₇ ≥ Na₅P₃O₁₀. Maltose-sodium phosphate also showed a similar trend as glucose-sodium phosphate samples. However, the degree of T _g′-rise of maltose systems was much less than that of glucose. It is thought that the T _g′ elevated by the molecular interaction between sugar and phosphate ions will be reduced by hydrated sodium ions. In comparisons between potassium phosphate and sodium phosphate, it was found that sugar-potassium phosphates showed the lower maximum T _g′ at a lower phosphate ratio than sugar-sodium phosphates. In addition, the T _g′ of potassium phosphates dropped sharply in comparison with sodium phosphates at the high phosphate ratio. These results suggest that potassium phosphates are lower T _g′ than sodium phosphates, and that potassium ion plays a better plasticizer than sodium ion. A certain amount of sodium phosphates (Na₃PO₄ and Na₄P₂O₇) caused devitrification. Potassium phosphates, however, did not show devitrification which can be explained by the fact that potassium ion can be dynamically restricted by sugar.     

Self-association of oxyhaemoglobin. A nuclear magnetic relaxation study in H2O/D2O solutions

The proton and deuterium longitudinal relaxation rates were Studied at room temperature up to the highest protein concentrations in oxyhaemoglobin solutions of different H₂O/D₂O composition. The deuterium relaxation rates followed the experimentally well known single linear dependence on protein concentration, the slopes being little influenced by solvent (D₂O/H₂O) composition. The proton ralaxation rates show two different liner dependences on haemoglobin concentration. The entire concentration range is described by two straight lines with the threshold concentration about 11 mM (in haem), The ratio of the slopes is 1.6 (high-to-low Hb-conc.). Only in the higher concentration range two T₁'s were observed if the solvent contained more than half of D₂O. The slow relaxation phase of protons has T₁'s similar to those measured in solutions with less than half of D₂O. The relaxation of the other phase was ten times faster. The ratio of the proton populations in these two phases was equal to 2 (slow-to-fast) and independent of protein concentration. The fast relaxing protons are attributed to water molecules encaged within two or more haemoglobin molecules which associate for times long enough on the PMR time-scale.     

300 MHz proton NMR study of the differentiation of diploid human epidermal keratinocytes

The nuclear magnetic resonance spin-lattice (T₁) and spin-spin (T₂) relaxation times are closely related to the molecular motions of the molecules in a liquid sample. T₁ and T₂ of human epidermal cells were measured at 300 MHz as functions of harvesting methods (i.e., scraping vs trypsinization) and age in culture. It was found that T₁ and T₂ values have smaller variances when the cell is harvested by trypsinization rather than scraping. The correlation coefficients for both T₁ and T₂, obtained from cells harvested by trypsinization, are much higher than those obtained from cells harvested by scraping. More importantly, this is the first report to monitor in vitro aging through relaxation times measurement. There is a significant increase in the values of T₁ and T₂ from the third to seventh passages. Human keratinocytes slowed down and even ceased to grow the seventh passage. Therefore, the cellular water molecules of human keratinocytes have higher mobility in a more differentiated state. The factors contributing to the change in relaxation times as cells progress toward senescence are discussed.     

Recrystallization of Ice Crystals in Trehalose Solution at Isothermal Condition

An isothermal ice recrystallization behavior in trehalose solution was investigated. The isothermal recrystallization rate constants of ice crystals in trehalose solution were obtained at ?5 °C, ?7 °C, and ?10 °C. Then the results were compared to those of a sucrose solution used as a control sample. Simultaneous estimation of water mobility in the freeze-concentrated matrix was conducted by ¹H spin–spin relaxation time T₂ to investigate mechanisms causing the different ice crystal recrystallization behaviors of sucrose and trehalose. At lower temperatures, lower recrystallization rates were obtained for both trehalose and sucrose solutions. The ice crystallization rate constants in trahalose solution tended to be smaller than those in sucrose solution at the same temperature. Although different ice contents (less than 3.6%) were observed between trehalose and sucrose solutions at the same temperature, the recrystallization behaviors of ice crystals were not markedly different. The ¹H spin–spin relaxation time T₂ of water components in a freeze-concentrated matrix for trehalose solution was shorter than in a sucrose solution at the same temperature. Results show that the water mobility of trehalose solutions in freeze-concentrated matrix was less than that of sucrose solutions, which was suggested as the reason for retarded ice crystal growth in a trehalose solution. Results of this study suggest that the replacement of sucrose with trehalose will not negatively affect deterioration caused by ice crystal recrystallization in frozen foods and cryobiological materials.     

Molecular mobilities in chromaffin granules magnetic field dependence of proton T1 relaxation times

The magnetic field dependence of the NMR spin-lattice relaxation time of water protons in intact bovine chromaffin vesicles has been studied over the range 1.00–23.49 kG. The T₁ relaxation time shows a dispersion a t field values near 20 kG. The observed proton resonance arises mainly from solvent protons (¹H₂O), but the relaxation rate, which is a weighted average over all sites with which the solvent protons rapidly exchange (i.e., NH and OH protons), is dominated by exchangeable protons in the most slowly moving soluble component. The field dependence of the T₁ dispersion demonstrates the existence of a site of exchangeable protons for which τ_r = 1.9±0.5 ns at 3°C. This site is assigned to ATP and cationic groups to which its phosphate esters are complexed, since previously measured correlation times of epinephrine and the chromogranin backbone are nearly an order of magnitude too short to explain the T₁ dispersion. Quantitative estimates of the relative numbers of exchangeable protons on the different soluble components support this interpretation. The temperature dependence of T₁ of the peak due to exchangeable protons has also been measured over a temperature range ?3 to 25°C. T₁ lengthens by about 30% over this range and exhibits no discontinuous behavior, as would be expected if a gel transition or structural alterations in the storage complex occurred. T₁ lengthens by less than 10% in chromaffin granule pastes that have been maintained at 25°C for 24 h, indicating considerable thermal stability in the storage complex. Possible effects on the solvent T₁ due to paramagnetic ions have been considered with the conclusion that they are probably negligible or of minor significance.     

Glass transition behavior of octyl β-D-glucoside and octyl β-D-thioglucoside/water binary mixtures

The lyotropic behavior and glass-forming properties of octyl β-d-glucoside (C8Glu) and octyl β-d-thioglucoside (C8SGlu)/water binary mixtures were evaluated using differential scanning calorimetry (DSC) and polarizing optical microscopy (POM). The results clearly indicate that the mixture forms a glass in the supercooling state of liquid crystalline phases such as cubic, lamellar, and smectic. The glass transition temperature (T_g) of the mixture was strongly dependent on solute concentration, with a higher concentration correlating with a higher T_g. The experimental T_g was consistent with the predicted value calculated using the Couchman-Karasz equation in both the C8Glu and C8SGlu/water mixtures. The change of heat capacity at T_g showed the two bending points under variation of concentrations. And the highest temperature of phase transition from lamellar to isotropic solution was observed at around 50% molar concentration. It was expected that non-percolated state of water existed in extremely higher concentration ranges.     

The amorphous state of spray-dried maltodextrin: sub-sub-Tg enthalpy relaxation and impact of temperature and water annealing

The annealing behaviour of a spray-dried maltodextrin was investigated by differential scanning calorimetry. Special attention was paid to the effect of temperature and humidity on the annealing process. Comparison was also made with the glassy state of the same compound prepared by various cooling processes. The presence of a very pronounced sub-T_g peak upon ageing reveals the specificities of the glass and the complexity of the relaxation spectrum of the spray-dried material. This peak seems actually to correspond to a partial ergodicity recovery that may be attributed to onset of molecular mobility occurring below T_g. The position of the sub-T_g peak with regard to the conventional T_g was systematically studied. It clearly showed the difference between the effect of temperature and water plasticization on the relaxations occurring in the glassy state of materials prepared by spray-drying.     

31P nuclear magnetic resonance studies of the association of basic proteins with multilayers of diacyl phosphatidylserine

Lysozyme, cytochrome c, poly(l-lysine), myelin basic protein and ribonuclease were used to form multilayer dispersions containing about 50% protein (by weight) with bovine brain diacyl phosphatidylserine (PS). ³¹P nuclear magnetic resonance shift anisotropies, spin-spin (T₂) and spin-lattice (T₁) relaxation times for the lipid headgroup phosphorus were measured at 36.44 MHz. At pH 7.5, lysozyme, cytochrome c, poly(l-lysine) and ribonuclease were shown to increase the chemical shift anisotropy of PS by between 12–20%. Myelin basic protein altered the shape of the phosphate resonance, suggesting the presence of two lipid components, one of which had a modified headgroup conformation. The presence of cytochrome c led to the formation of a narrow spike at the isotropic shift position of the spectrum. Of the various proteins or peptides we have studied, only poly(l-lysine) and cytochrome c had any effect on the T₁ of PS (1050 ms). Both caused a 20–30% decrease in T₁ of the lamellar-phase phosphate peak. The narrow peak in the presence of cytochrome c had a very short T₁ of 156 ms. The possibility is considered that the cytochrome Fe³⁺ contributes to the phosphate relaxation in this case. The effect of all proteins on the T₂ of the phosphorus resonance was to cause an increase from the value for pure PS (1.6 ms) to between 2 and 5 ms. The results obtained with proteins are compared with the effects of small ions and intrinsic membrane proteins on the order and motion of the headgroups of lipids in bilayers.     

Anti-plasticization of cassava starch by complexing fatty acids

The effect of adding 1–8% amylose complexing fatty acids (CFA), such as linoleic and oleic acids, on the glass transition temperature (T_g) of cassava starch (CS) with moisture content varying from 5 to 35% (dry basis) was studied. The main relaxation temperature (T_α), associated with the glass transition temperature of the samples (T_g), was determined by dynamic-mechanical-thermal analysis. The plasticizing behavior of water in the blends was evidenced by a decrease of T_α values with moisture content. The effect of CFA on CS was found to be a function of moisture content. At low moisture (<11%) it caused an anti-plasticization effect, while at higher moisture contents it produced plasticization. The anti-plasticizing effect of CFA on CS was attributed to amylose–lipid complex formation.     

The protein glass transition as measured by dielectric spectroscopy and differential scanning calorimetry

The glass transition and its related dynamics of myoglobin in water and in a water–glycerol mixture have been investigated by dielectric spectroscopy and differential scanning calorimetry (DSC). For all samples, the DSC measurements display a glass transition that extends over a large temperature range. Both the temperature of the transition and its broadness decrease rapidly with increasing amount of solvent in the system. The dielectric measurements show several dynamical processes, due to both protein and solvent relaxations, and in the case of pure water as solvent the main protein process (which most likely is due to conformational changes of the protein structure) exhibits a dynamic glass transition (i.e. reaches a relaxation time of 100 s) at about the same temperature as the calorimetric glass transition temperature T_g is found. This glass transition is most likely caused by the dynamic crossover and the associated vanishing of the α-relaxation of the main water relaxation, although it does not contribute to the calorimetric T_g. This is in contrast to myoglobin in water–glycerol, where the main solvent relaxation makes the strongest contribution to the calorimetric glass transition. For all samples it is clear that several proteins processes are involved in the calorimetric glass transition and the broadness of the transition depends on how much these different relaxations are separated in time.     

Physicochemical Investigations and Stability Studies of Amorphous Gliclazide

Gliclazide (GLI), a poorly water-soluble antidiabetic, was transformed into a glassy state by melt quench technique in order to improve its physicochemical properties. Chemical stability of GLI during formation of glass was assessed by monitoring thin-layer chromatography, and an existence of amorphous form was confirmed by differential scanning calorimetry and X-ray powder diffractometry. The glass transition occurred at 67.5°C. The amorphous material thus generated was examined for its in vitro dissolution performance in phosphate buffer (pH 6.8). Surprisingly, amorphous GLI did not perform well and was unable to improve the dissolution characteristics compared to pure drug over entire period of dissolution studies. These unexpected results might be due to the formation of a cohesive supercooled liquid state and structural relaxation of amorphous form toward the supercooled liquid region which indicated functional inability of amorphous GLI from stability point of view. Hence, stabilization of amorphous GLI was attempted by elevation of T_g via formation of solid dispersion systems involving comprehensive antiplasticizing as well as surface adsorption mechanisms. The binary and ternary amorphous dispersions prepared with polyvinylpyrrolidone K30 (as antiplasticizer for elevation of T_g) and Aerosil 200® and/or Sylysia® 350 (as adsorbent) in the ratio of 1:1:1 (w/w) using kneading and spray-drying techniques demonstrated significant enhancement in rate and extent of dissolution of drug initially. During accelerated stability studies, ternary systems showed no significant reduction in drug dissolution performance over a period of 3 months indicating excellent stabilization of amorphous GLI.Key words: amorphous, gliclazide, solid dispersion, stability studies, T_g     

Nuclear magnetic resonance relaxation times and plasmalemma water exchange in ivy bark

Measurement of nuclear magnetic resonance (NMR) relaxation times (transverse [T₂] and longitudinal [T₁]) for Hedera helix L. cv. Thorndale (ivy) bark water indicates the presence of at least two populations of water with different relaxation characteristics. One population of water with short T₂ and T₁ was found to be composed of both hydration water and extracellular free water. The second population of water with long T₂ and T₁ was identified as intracellular bulk water.     

Practical Considerations for Determination of Glass Transition Temperature of a Maximally Freeze Concentrated Solution

Glass transition temperature is a unique thermal characteristic of amorphous systems and is associated with changes in physical properties such as heat capacity, viscosity, electrical resistance, and molecular mobility. Glass transition temperature for amorphous solids is referred as (T _g), whereas for maximally freeze concentrated solution, the notation is (T _g′). This article is focused on the factors affecting determination of T _g′ for application to lyophilization process design and frozen storage stability. Also, this review provides a perspective on use of various types of solutes in protein formulation and their effect on T _g′. Although various analytical techniques are used for determination of T _g′ based on the changes in physical properties associated with glass transition, the differential scanning calorimetry (DSC) is the most commonly used technique. In this article, an overview of DSC technique is provided along with brief discussion on the alternate analytical techniques for T _g′ determination. Additionally, challenges associated with T _g′ determination, using DSC for protein formulations, are discussed. The purpose of this review is to provide a practical industry perspective on determination of T _g′ for protein formulations as it relates to design and development of lyophilization process and/or for frozen storage; however, a comprehensive review of glass transition temperature (T _g, T _g′), in general, is outside the scope of this work.     

Simultaneous Determination of Glass Transition Temperatures of Several Polymers

Aims

A simple and easy optical method is proposed for the determination of glass transition temperature (T_g) of polymers.

Methods & Results

T_g was determined using the technique of microsphere imaging to monitor the variation of the refractive index of polymer microsphere as a function of temperature. It was demonstrated that the method can eliminate most thermal lag and has sensitivity about six fold higher than the conventional method in T_g determination. So the determined T_g is more accurate and varies less with cooling/heating rate than that obtained by conventional methods. The most attractive character of the method is that it can simultaneously determine the T_g of several polymers in a single experiment, so it can greatly save experimental time and heating energy.

Conclusion

The method is not only applicable for polymer microspheres, but also for the materials with arbitrary shapes. Therefore, it is expected to be broadly applied to different fundamental researches and practical applications of polymers.