Automated temperature control system for vagal cooling

An automated cooling system for vagal cold blockade was developed. A simple electronic circuit is described that enabled regulation of the steady-state nerve or circulant temperature to within +/- 0.1 degree C by alternating the cold circulant between low and high flows (10 and 350 ml/min, respectively). The 90% rise time ranged from 15 to 40 s depending on the desired steady state and the surrounding temperatures. The present apparatus can be conveniently and safely used, especially for differential vagal cold blockade.     

Hypercapnia increases core temperature cooling rate during snow burial.

Previous retrospective studies report a core body temperature cooling rate of 3 degrees C/h during avalanche burial. Hypercapnia occurs during avalanche burial secondary to rebreathing expired air, and the effect of hypercapnia on hypothermia during avalanche burial is unknown. The objective of this study was to determine the core temperature cooling rate during snow burial under normocapnic and hypercapnic conditions. We measured rectal core body temperature (T(re)) in 12 subjects buried in compacted snow dressed in a lightweight clothing insulation system during two different study burials. In one burial, subjects breathed with a device (AvaLung 2, Black Diamond Equipment) that resulted in hypercapnia over 30-60 min. In a control burial, subjects were buried under identical conditions with a modified breathing device that maintained normocapnia. Mean snow temperature was -2.5 +/- 2.0 degrees C. Burial time was 49 +/- 14 min in the hypercapnic study and 60 min in the normocapnic study (P = 0.02). Rate of decrease in T(re) was greater with hypercapnia (1.2 degrees C/h by multiple regression analysis, 95% confidence limits of 1.1-1.3 degrees C/h) than with normocapnia (0.7 degrees C/h, 95% confidence limit of 0.6-0.8 degrees C/h). In the hypercapnic study, the fraction of inspired carbon dioxide increased from 1.4 +/- 1.0 to 7.0 +/- 1.4%, minute ventilation increased from 15 +/- 7 to 40 +/- 12 l/min, and oxygen saturation decreased from 97 +/- 1 to 90 +/- 6% (P < 0.01). During the normocapnic study, these parameters remained unchanged. In this study, T(re) cooling rate during snow burial was less than previously reported and was increased by hypercapnia. This may have important implications for prehospital treatment of avalanche burial victims.     

Optimal temperature control for batch beer fermentation

Optimal control theory was applied to the process of batch beer fermentation. The performance functional considered was a weighted sum of maximum ethanol production and minimum time. Calculations were based on the model of Engasser et al. modified to include temperature effects. Model parameters were determined from isothermal batch fermentations. The fermentor cooling duty was the single available control. Temperature state variable constraints as well as control variable constraints were considered. The optimal control law is shown to be bang-bang control with the existence of a singular arc corresponding to isothermal operation at the maximum temperature constraint. An iterative algorithm is presented for computing appropriate switching times using a penalty-function-augmented performance functional.     

Optimal temperature control policy for a two-stage recombinant fermentation process.

The optimal temperature control policy to be followed in the operation of a two-stage fermentation system in which gene expression is induced by a temperature-sensitive gene switching system was studied. A genetically structured model was used to describe product formation, and kinetic equations based on experimental data were used to quantify the specific gene expression rate and parameters that affect plasmid instability. A constant temperature control policy and temperature profiling control policy including temperature cycling were studied and compared. Maximum average production rate was obtained from a temperature control policy in which the second stage was operated initially at about 40.5 degrees C and the temperature decreased slightly to a constant value at 40.0 degrees C. The maximum average production rate, which corresponds to the optimal temperature control policy, for an operation of 180 h was 29.7 units of protein (mg of cells)-1 h-1.     

A versatile microcomputer-based temperature and cooling/warming rate controller

A microcomputer-based system has been developed for the control of temperature from ?199.9 ° to ?199.9 °C, and rate of change of temperature from 0.01 ° to 99.99 °C/min. A digital thermometer is used to monitor the temperature, and the system can control a variety of heating and cooling equipment. The system is economical, easy to construct, simple to program, and may be extended to perform a wide variety of functions based on the control of temperature.     

Statically controlled cooling rate device.

A new statically controlled cooling rate device consists of metal plates and insulators which can be modified so as to control heat flow and achieve a considerable range of specific cooling rates. It can thus be adapted to give the desired cooling rates for the cryopreservation of various biological materials. The cassette has been used effectively to cryopreserve human platelets and red blood cells. Its potential advantages over commercial instruments include simplicity of operation, improved reproducibility, and low cost.     

Optimal temperature control for a structured model of plant cell culture

This article calculates optimal open-loop temperature trajectories that maximize the average rate of product synthesis of a plant cell culture. It uses a previously published five-state mathematical model which describes the growth and product synthesis of a batch plant cell suspension culture of Catharanthus roseus under temperature control. The optimal open-loop temperatures maximize the final product concentration for predefined fermentation periods. A single switch in temperature is shown by computer simulation to be near optimal, with a 22% increase in final product yield over that obtained at the optimal constant temperature. Examination of the achieved final product yield as a function of fermentation period allows this period also to be chosen optimally. This time is reduced from 16 days in the constant temperature case to 12 days in the switched temperature case.     

Effects of cooling rate and storage temperature on equine spermatozoal motility parameters

Two experiments were conducted to examine the effects of cooling rate and storage temperature on motility parameters of stallion spermatozoa. In Experiment 1, specific cooling rates to be used in Experiment 2 were established. In Experiment 2, three ejaculates from each of two stallions were diluted to 25 x 10(6) sperm/ml with 37 degrees C nonfat dry skim milk-glucose-penicillin-streptomycin seminal extender, then assigned to one of five treatments: 1) storage at 37 degrees C, 2) storage at 25 degrees C, 3) slow cooling rate to and storage at 4 degrees C, 4) moderate cooling rate to and storage at 4 degrees C, and 5) fast cooling rate to and storage at 4 degrees C. Total spermatozoal motility (TSM), progressive spermatozoal motility (PSM), and spermatozoal velocity (SV) were estimated at 6, 12, 24, 48, 72, 96 and 120 h postejaculation. The longevity of spermatozoal motility was greatly reduced when spermatozoa were stored at 37 degrees C as compared to lower spermatozoal storage temperatures. At 6 h postejaculation, TSM values (mean % +/- SEM) of semen stored at 37 degrees C, slowly cooled to and stored at 25 degrees C or slowly cooled to and stored at 4 degrees C were 5.4 +/- 1.1, 79.8 +/- 1.6, and 82.1 +/- 1.6, respectively. Mean TSM for semen that was cooled to 4 degrees C at a slow rate was greater (P<0.05) than mean TSM of semen cooled to 4 degrees C at a moderate rate for four of seven time periods (6, 24, 72 and 120 h), and it was greater (P<0.05) than mean TSM of semen cooled to 4 degrees C at a fast rate for five of seven time periods (6, 12, 24, 72 and 120 h). Mean TSM of semen cooled to 4 degrees C at a slow rate was greater (P<0.05) than mean TSM of semen cooled to 25 degrees C for five of seven time periods (24 to 120 h). A similar pattern was found for PSM. Mean SV of semen cooled to 4 degrees C at a slow rate was greater (P<0.05) than mean SV of semen cooled to 25 degrees C for all time periods. A slow cooling rate (initial cooling rate of -0.3 degrees /min) and a storage temperature of 4 degrees C appear to optimize liquid preservation of equine spermatozoal motility in vitro.     

Optimal conditions for the preservation of mouse lymph node cells in liquid nitrogen using cooling rate techniques

The factors that affect the survival of mouse lymphocytes throughout a procedure for storage at ?196 °C have been studied both for the improvement of recovery and the possible extension to the mouse system of cell selection by freezing. After thawing, the survival of cells cooled at different rates in dimethyl sulphoxide (DMSO, 5 or 10%, $\text{v}\text{v}$) was assessed from the [³H]thymidine incorporation in response to phytohaemagglutinin and concanavalin A. Before freezing the protection against freezing damage increased with time (up to 20 min) in DMSO (5%, $\text{v}\text{v}$) at 0 °C. Superimposed upon this effect was toxicity due to the DMSO. During freezing and thawing the cooling rate giving optimal survival was 8 to 15 °C/min for cells in DMSO (5%) and 1 to 3 °C/min for DMSO (10%). Omission of foetal calf serum was detrimental. Rapid thawing (>2.5 °C/min) was superior to slow thawing. After thawing dilution at 25 or 37 °C greatly improved cell survival compared with 0 °C; at 25 °C survival was optimal (75%) at a moderate dilution rate of 2.5 min for a 10-fold dilution in FCS (10%, $\text{v}\text{v}$) followed by gentle centrifugation (50g).Dilution damage during both thawing and post-thaw dilution may be due to osmotic swelling as DMSO and normally excluded solutes leave the cell. The susceptibility of the cell membrane to dilution damage may also be increased during freezing. The need to thaw rapidly and dilute at 25 °C after thawing is probably due to a decrease in dilution stress at higher temperatures. Optimisation of dilution procedures both maximised recovery and also widened the range of cooling rates over which the cells were recovered. These conditions increase the possibility of obtaining good recovery of a mixed cell population using a single cooling procedure. Alternatively, if cell types have different optimal cooling rates, stressful dilution may allow their selection from mixed cell populations.     

Modulation of arterial baroreflex control of heart rate by skin cooling and heating in humans.

The purpose of this study was to examine the effects of skin cooling and heating on the heart rate (HR) control by the arterial baroreflex in humans. The subjects were 15 healthy men who underwent whole body thermal stress (esophageal temperatures, approximately 36.8 and approximately 37.0 degrees C; mean skin temperatures, approximately 26.4 and approximately 37.7 degrees C, in skin cooling and heating, respectively) produced by a cool or hot water-perfused suit during supine rest. The overall arterial baroreflex sensitivity in the HR control was calculated from spontaneous changes in beat-to-beat arterial pressure and HR during normothermic control and thermal stress periods. The carotid baroreflex sensitivity was evaluated from the maximum slope of the HR response to changes in carotid distending pressure, calculated as mean arterial pressure minus neck pressure. The overall arterial baroreflex sensitivity at existing arterial pressure increased during cooling (-1.32 +/- 0.25 vs. -2.13 +/- 0.20 beats. min(-1). mmHg(-1) in the control and cooling periods, respectively, P < 0.05), whereas it did not change significantly during heating (-1.39 +/- 0. 23 vs. -1.40 +/- 0.15 beats. min(-1). mmHg(-1) in the control and heating periods, respectively). Neither the cool nor heat loadings altered the carotid baroreflex sensitivity in the HR control. These results suggest that the sensitivity of HR control by the extracarotid (presumably aortic) baroreflex was augmented by whole body skin cooling, whereas the sensitivities of HR control by arterial baroreflex remain unchanged during mild whole body heating in humans.     

Determination of temperature and cooling rate which induce cold shock in stallion spermatozoa

Experiments were conducted to determine temperatures between 24 and 4 degrees C at which stallion spermatozoa are most susceptible to cold shock damage. Semen was diluted to 25 x 10(6) spermatozoa/ml in a milk-based extender. Aliquots of extended semen were then cooled in programmable semen coolers. Semen was evaluated by computerized semen analysis initially and after 6, 12, 24, 36 and 48 hours of cooling. In Experiment 1A, semen was cooled rapidly (-0.7 degrees C/minute) from 24 degrees C to either 22, 20, 18 or 16 degrees C; then it was cooled slowly (-0.05 degrees C/minute) to a storage temperature of 4 degrees C. In Experiment 1B, rapid cooling proceeded from 24 degrees C to either 22, 19, 16, or 13 degrees C, and then slow cooling occurred to 4 degrees C. Initiating slow cooling at 22 or 20 degrees C resulted in higher (P<0.05) total and progressive motility over the first 24 hours of cooling than initiating slow cooling at 16 degrees C. Initiation of slow cooling at 22 or 19 degrees C resulted in higher (P<0.05) total and progressive motility over 48 hours of cooled storage than initiation of slow cooling at 16 or 13 degrees C. In Experiment 2A, semen was cooled rapidly from 24 to 19 degrees C, and then cooled slowly to either 13, 10, 7 or 4 degrees C, at which point rapid cooling was resumed to 4 degrees C. Resuming the fast rate of cooling at 7 degrees C resulted in higher (P<0.05) total and progressive motility at 36 and 48 hours of cooled storage than resuming fast cooling at 10 or 13 degrees C. In Experiment 2B, slow cooling proceeded to either 10, 8, 6 or 4 degrees C before fast cooling resumed to 4 degrees C. There was no significant difference (P>0.05) at most storage times in total or progressive motility for spermatozoa when fast cooling was resumed at 8, 6 or 4 degrees C. In Experiment 3, cooling units were programmed to cool rapidly from 24 to 19 degrees C, then cool slowly from 19 to 8 degrees C, and then resume rapid cooling to storage temperatures of either 6, 4, 2 or 0 degrees C. Storage at 6 or 4 degrees C resulted in higher (P<0.05) total and progressive motility over 48 hours of storage than 0 or 2 degrees C.     

Protein dynamics. An overview on flash-photolysis over broad temperature ranges.

Ligand binding kinetics to heme-proteins between 40 and 300 K point to a regulatory role of protein dynamics. A protein-specific susceptibility of the heme-iron reactivity to dynamic fluctuations emerges from the distribution of reaction enthalpies derived from flash-photolysis measurements below ca. 180 K; we quantify it in terms of 'intramolecular viscosity', postulating that narrow low-temperature enthalpy distributions correspond to low internal viscosity and vice versa. The thermal evolution of ligand binding kinetics suggests, with other results, an interplay between high-frequency transitions of the amino acid side chains and low-frequency collective motions as a possible regulatory mechanism of protein dynamics.     

Optimal rate of work for mountaineers

The physiological responses of seven young male highlanders were recorded at high altitude while they were carrying loads (0, 25, 35, 45, and 55 kg) on snow at different speeds, supporting the loads on their backs by circular straps around the forehead. The rates of work calculated from the gross weight (body weight plus actual load in kg) multiplied by the speed of walking, m.min-1, ranged from 4,460 to 8,440 kg.m.min-1. The relationship between the rate of work and energy expenditure was rectilinear within the present range of values. The oxygen consumption (51.6 and 59.7 ml.min-1.kg-1 BW) for 55-kg load (at 4.09 and 4.64 km.h-1) possibly reached maximal aerobic capacity. At higher energy output at high altitude the subjects were exhausted after a short period of work. The proportion of increase of oxygen consumption per kg gross weight carried or per kg.m was almost constant up to a 55-kg experimental load. It is suggested that for day-to-day operations work should not be undertaken at more than 30-40% of maximal work capacity; a rate of work around 4,000 kg.m.min-1 (25-30 kg actual load at 3.0 to 3.5 km.h-1) may be considered as optimal for highlanders and porters at high altitude.