Regional hyperthermia by magnetic induction in a beagle dog model: analysis of thermal dosimetry

We have investigated magnetic induction heating techniques for achieving normal tissue hyperthermia in a beagle dog model to clarify the physics and physiology of "regional heating," to develop an animal model of regional heating in humans, and to develop a method of rapid regional heating in dogs for a normal visceral tissue toxicity study. Heating was done with a concentric coil or a coaxial pair of coils applied to the abdominal region, and with or without surface cooling blankets in each case. Thermometers were placed at multiple visceral and subcutaneous sites including an intraarterial thermocouple at the aortic arch level. With either electrode arrangement and no surface cooling, whole-body hyperthermia ( WBH ) at 42 degrees C was produced within 30 to 55 min with 250 W applied power; the 42 degrees C state could be maintained with 40 to 60 W of power. Thermal gradients in these cases reflected nonuniform power deposition superimposed upon arterial temperature elevation. With surface cooling blankets added, systemic heating was significantly reduced, and temperature gradients again reflected the nonuniform power deposition. Regional heating in a dog produces WBH unless sufficient surface cooling is used to provide a heat dissipation rate balancing the heat absorption rate; this latter case best models the use of inductive techniques in humans. The coaxial pair of coils, without surface cooling, produced rapid WBH and the visceral temperature maximum and minimum were within Tesoph + 0.21 degrees C and Tesoph - 0.07 degrees C, respectively (95% confidence index; Tesoph = esophageal temperature). This is an appropriate technique for the proposed toxicity study.     

Studies on the three-dimensional temperature transients in the canine prostate during transurethral microwave thermal therapy

Thermal therapy of benign prostatic hyperplasia requires accurate prediction of the temperature distribution induced by the heating within the prostatic tissue. In this study, the Pennes bioheat transfer equation was used to model the transient heat transfer inside the canine prostate during transurethral microwave thermal therapy. Incorporating the specific absorption rate of microwave energy in tissue, a closed-form analytical solution was obtained. Good agreement was found between the theoretical predictions and in-vivo experimental results. Effects of blood perfusion and the cooling at the urethral wall on the temperature rise were investigated within the prostate during heating. The peak intraprostatic temperatures attained by application of 5, 10, or 15 W microwave power were predicted to be 38 degrees C, 41 degrees C, and 44 degrees C. Results from this study will help optimize the thermal dose that can be applied to target tissue during the therapy.     

Absence of selective brain cooling in unrestrained baboons exposed to heat

To test whether baboons are capable of implementing selective brain cooling, we measured, every 5 min, the temperature in their hypothalamus, carotid arterial bloodstream, and abdominal cavity. The baboons were unrestrained and exposed to 22 degrees C for 7 days and then to a cyclic environment with 15 degrees C at night and 35 degrees C during the day for a further 7 days. During the latter 7 days some of the baboons also were exposed to radiant heat during the day. For three days, during heat exposure, water was withheld. At no time was the hypothalamus cooler than carotid arterial blood, despite brain temperatures above 40 degrees C. With little variation, the hypothalamus was consistently 0.5 degrees C warmer than arterial blood. At high body temperatures, the hypothalamus was sometimes cooler than the abdomen. Abdominal temperature was more variable than arterial blood and tended to exceed arterial blood temperature at higher body temperatures. Hypothalamic temperature cooler than a warm abdomen is not evidence for selective brain cooling. In species that can implement selective brain cooling, the brain is most likely to be cooler than carotid arterial blood when an animal is hyperthermic, during heat exposure, and also dehydrated and undisturbed by human presence. When we exposed baboons to high ambient temperatures while they were water deprived and undisturbed, they never implemented selective brain cooling. We conclude that baboons cannot implement selective brain cooling and can find no convincing evidence that any primate species can do so.     

Dehydration increases the magnitude of selective brain cooling independently of core temperature in sheep

By cooling the hypothalamus during hyperthermia, selective brain cooling reduces the drive on evaporative heat loss effectors, in so doing saving body water. To investigate whether selective brain cooling was increased in dehydrated sheep, we measured brain and carotid arterial blood temperatures at 5-min intervals in nine female Dorper sheep (41 +/- 3 kg, means +/- SD). The animals, housed in a climatic chamber at 23 degrees C, were exposed for nine days to a cyclic protocol with daytime heat (40 degrees C for 6 h). Drinking water was removed on the 3rd day and returned 5 days later. After 4 days of water deprivation, sheep had lost 16 +/- 4% of body mass, and plasma osmolality had increased from 290 +/- 8 to 323 +/- 9 mmol/kg (P < 0.0001). Although carotid blood temperature increased during heat exposure to similar levels during euhydration and dehydration, selective brain cooling was significantly greater in dehydration (0.38 +/- 0.18 degrees C) than in euhydration (-0.05 +/- 0.14 degrees C, P = 0.0008). The threshold temperature for selective brain cooling was not significantly different during euhydration (39.27 degrees C) and dehydration (39.14 degrees C, P = 0.62). However, the mean slope of lines of regression of brain temperature on carotid blood temperature above the threshold was significantly lower in dehydrated animals (0.40 +/- 0.31) than in euhydrated animals (0.87 +/- 0.11, P = 0.003). Return of drinking water at 39 degrees C led to rapid cessation of selective brain cooling, and brain temperature exceeded carotid blood temperature throughout heat exposure on the following day. We conclude that for any given carotid blood temperature, dehydrated sheep exposed to heat exhibit selective brain cooling up to threefold greater than that when euhydrated.     

Temperature difference between the body core and arterial blood supplied to the brain during hyperthermia or hypothermia in humans

 A vascular heat transfer model is developed to simulate temperature decay along the carotid arteries in humans, and thus, to evaluate temperature differences between the body core and arterial blood supplied to the brain. Included are several factors, including the local blood perfusion rate, blood vessel bifurcation in the neck, and blood vessel pairs on both sides of the neck. The potential for cooling blood in the carotid artery by countercurrent heat exchange with the jugular veins and by radial heat conduction to the neck surface was estimated. Cooling along the common and internal carotid arteries was calculated to be up to 0.87 °C during hyperthermia by high environmental temperatures or muscular exercise. This model was also used to evaluate the feasibility of lowering the brain temperature effectively by placing ice pads on the neck and head surface or by wearing cooling garments during hypothermia treatment for brain injury or other medical conditions. It was found that a 1.1 °C temperature drop along the carotid arteries is possible when the neck surface is cooled to 0 °C. Thus, the body core temperature may not be a good indication of the brain temperature during hyperthermia or hypothermia. Received: 10 January 2002 / Accepted: 7 May 2002 This research was supported by a UMBC Summer Faculty Fellowship.     

Competition for cool nasal blood between trunk and brain in hyperthermic goats

An influence of brain and trunk temperatures controlled independently of each other by means of artificial heat exchangers, on the intensity of natural selective brain cooling (SBC) was studied in 6 conscious goats. Intensity of SBC was markedly enhanced by increasing brain temperature. On the other hand, a rise of trunk temperature with the cerebral temperature clamped at 39 degrees C or 40 degrees C, reduced SBC intensity in spite of a simultaneous increase in the respiratory evaporative heat loss. When brain temperature was clamped at 41 degrees C, the magnitude of SBC was essentially independent of trunk temperature. These results suggest that during hyperthermia a competition exists between trunk and brain for cool nasal blood.     

Local 42 degrees C hyperthermia improves vascular conductance of the R3230Ac rat mammary adenocarcinoma during sodium nitroprusside infusion

The effect of sodium nitroprusside-induced hypotension on the perfusion of the R3230 adenocarcinoma during local 42 degrees C hyperthermia was studied using a combination of intravital microscopy and laser Doppler flowmetry. Fischer 344 rats were implanted with dorsal skin flap window chambers containing the R3230Ac tumor and allocated to three treatment groups (34 degrees C with nitroprusside, 42 degrees C with nitroprusside, and 42 degrees C with 0.9% saline). After baseline observation at 34 degrees C, tumors were locally heated to 42 degrees C using a water bath and either 0.9% saline or nitroprusside sufficient to reduce blood pressure 20% below pretreatment baseline was infused. Nitroprusside at 34 degrees C decreased tumor vascular conductance 40% with no effect on the diameter of arterioles entering the tumor. The diameter of arterioles entering 42 degrees C heated tumors increased 35% independent of blood pressure change. Saline at 42 degrees C had no effect on tumor vascular conductance; however, nitroprusside at 42 degrees C increased tumor vascular conductance 55%. Local 42 degrees C tumor heating, combined with a moderate reduction in blood pressure with nitroprusside, overrides the vascular steal effect associated with reduced perfusion pressure alone and results in improved tumor perfusion. Observations of the effect of vasodilator substances on normothermic tumor perfusion cannot be extrapolated to situations where moderate hyperthermia is used.     

The effect of hyperthermia on radiation-induced carcinogenesis

Ten groups of mice were exposed to either a single (30 Gy) or multiple (six fractions of 6 Gy) X-ray doses to the leg. Eight of these groups had the irradiated leg made hyperthermic for 45 min immediately following the X irradiation to temperatures of 37 to 43 degrees C. Eight control groups had their legs made hyperthermic with a single exposure or six exposures to heat as the only treatment. In mice exposed to radiation only, the postexposure subcutaneous temperature was 36.0 +/- 1.1 degrees C. Hyperthermia alone was not carcinogenic. At none of the hyperthermic temperatures was the incidence of tumors in the treated leg different from that induced by X rays alone. The incidence of tumors developing in anatomic sites other than the treated leg was decreased in mice where the leg was exposed to hyperthermia compared to mice where the leg was irradiated. A systemic effect of local hyperthermia is suggested to account for this observation. In mice given single X-ray doses and hyperthermia, temperatures of 37, 39, or 41 degrees C did not influence radiation damage as measured by the acute skin reactions. A hyperthermic temperature of 43 degrees C potentiated the acute radiation reaction (thermal enhancement factor 1.1). In the group subjected to hyperthermic temperatures of 37 or 39 degrees C and X rays given in six fractions, the skin reaction was no different from that of the group receiving X rays alone. Hyperthermic temperatures of 41 and 43 degrees C resulted in a thermal enhancement of 1.16 and 1.36 for the acute skin reactions. From Day 50 to Day 600 after treatment, the skin reactions showed regular fluctuations with a 150-day periodicity. Following a fractionated schedule of combined hyperthermia and X rays, late damage to the leg was less than that following X irradiation alone. Mice subjected to X rays and hyperthermic temperatures of 41 and 43 degrees C had a lower median survival time than the mice treated with hyperthermia alone. This effect was not associated with tumor incidence.     

Effects of hyperthermia on DNA interstrand crosslinking after treatment with BCNU in 9L rat brain tumor cells

The effects of hyperthermia (42 degrees C) on 1,3-bis(2-chloroethyl)-1-nitrosourea (BCNU)-mediated DNA interstrand crosslink formation were investigated in 9L rat brain tumor cells using the technique of alkaline elution. When cells were treated with 60 microM BCNU for 1 hr at 37 degrees C and incubated for 6 hr in drug-free medium at 42 degrees C, there was a 50% increase in crosslinking; and when cells were treated at 42 degrees C and incubated at 37 degrees C, there was a 45% increase in crosslinking compared with the results for cells treated and incubated at 37 degrees C. When cells were treated and incubated at 42 degrees C, there was a 129% increase in DNA crosslinking. The same relative order of results was found for cell survival. These results suggest that hyperthermia can increase DNA interstrand crosslink formation and the consequent cell death through two independent mechanisms: an increase in the amount of initial alkylation because of the increased rate of hydrolysis of BCNU at higher temperatures, and the effect of heat on DNA structure that leads to an increase in the number of crosslinks formed.     

Circulatory responses to vasoconstrictor agents during passive heating in the rat

The purpose of this study was to determine the actions of several pharmacological agents on the circulatory system, and more specifically on the superior mesenteric vascular bed, in response to environmental heat stress in chloralose-anesthetized rats. Animals were instrumented with Doppler flow probes on the mesenteric and renal arteries and exposed to an ambient temperature of 40 degrees C. Heart rate, mean arterial blood pressure (MAP), and core (Tc) and tail skin temperatures were also monitored. As Tc progressively increased from 37 degrees C during heat exposure, MAP rose to a plateau and then fell precipitously as Tc exceeded 41.5 degrees C. Mesenteric resistance increased throughout the early stages of heating before sharply declining prior to the reduction in MAP. The pressor and mesenteric resistance responses to constant infusions of several adrenergic agonists after MAP began falling (Tc = 41.3 degrees C) were significantly (P less than 0.05) attenuated compared with infusions into normothermic animals. In a second set of experiments, injections of both norepinephrine and angiotensin II were made 30 min before and approximately 10, 30, 50, 70, and 90 min after initiation of heating. These injections increased both MAP and mesenteric resistance; however, at TcS greater than 40 degrees C, the responses to both agonists were progressively and significantly attenuated. In a final group of animals, barium chloride infusions produced similar pressor and regional resistance changes during both normothermia and severe hyperthermia (Tc greater than 42 degrees C). These results indicate that, in the chloralose-anesthetized rat, hyperthermia disrupts adrenoceptor function but does not alter the intrinsic ability of vascular smooth muscle to contract.     

Improvement of tumor oxygenation by mild hyperthermia

There is now abundant evidence that oxygenation in rodent, canine and human tumors is improved during and for up to 1-2 days after heating at mild temperatures. An increase in tumor blood perfusion along with a decline in the oxygen consumption rate appears to account for the improvement of tumor oxygenation by mild hyperthermia. The magnitude of the increase in tumor pO(2), determined with oxygen-sensitive microelectrodes, caused by mild hyperthermia is less than that caused by carbogen breathing. However, mild hyperthermia is far more effective than carbogen breathing in increasing the radiation response of experimental tumors, probably because mild hyperthermia oxygenates both (diffusion-limited) chronically hypoxic and (perfusion-limited) acutely hypoxic cells, whereas carbogen breathing oxygenates only the chronically hypoxic cells. Mild hyperthermia is also more effective than nicotinamide, which is known to oxygenate acutely hypoxic cells, in enhancing the radiation response of experimental tumors. The combination of mild hyperthermia with carbogen or nicotinamide is highly effective in reducing the hypoxic cell fraction in tumors and increasing the radiation response of experimental tumors. A primary rationale for the use of hyperthermia in combination with radiotherapy has been that hyperthermia is equally cytotoxic toward fully oxygenated and hypoxic cells and that it directly sensitizes both fully oxygenated and hypoxic cells to radiation. Such cytotoxicity and such a radiosensitizing effect may be expected to be significant when the tumor temperature is elevated to at least 42-43 degrees C. Unfortunately, it is often impossible to uniformly raise the temperature of human tumors to this level using the hyperthermia devices currently available. However, it is relatively easy to raise the temperature of human tumors into the range of 39-42 degrees C, which is a temperature that can improve tumor oxygenation for up to 1-2 days. The potential usefulness of mild hyperthermia to enhance the response of human tumors to radiotherapy by improving tumor oxygenation merits continued investigation.     

Heat loss from the human head during exercise

Evaporative and convective heat loss from head skin and expired air were measured in four male subjects at rest and during incremental exercise at 5, 15, and 25 degrees C ambient temperature (Ta) to verify whether the head can function as a heat sink for selective brain cooling. The heat losses were measured with an open-circuit method. At rest the heat loss from head skin and expired air decreased with increasing Ta from 69 +/- 5 and 37 +/- 18 (SE) W (5 degrees C) to 44 +/- 25 and 26 +/- 7 W (25 degrees C). At a work load of 150 W the heat loss tended to increase with increasing Ta: 119 +/- 21 (head skin) and 82 +/- 5 W (respiratory tract) at 5 degrees C Ta to 132 +/- 27 and 103 +/- 12 W at 25 degrees C Ta. Heat loss was always higher from the head surface than from the respiratory tract. The heat losses, separately and together (total), were highly correlated to the increasing esophageal temperature at 15 and 25 degrees C Ta. At 5 degrees C Ta on correlation occurred. The results showed that the heat loss from the head was larger than the heat brought to the brain by the arterial blood during hyperthermia, estimated to be 45 W per 1 degree C increase above normal temperature, plus the heat produced by the brain, estimated to be up to 20 W. The total heat to be lost is therefore approximately 65 W during a mild hyperthermia (+1 degrees C) if brain temperature is to remain constant.(ABSTRACT TRUNCATED AT 250 WORDS)     

Predicting effects of blood flow rate and size of vessels in a vasculature on hyperthermia treatments using computer simulation

Background

Pennes Bio Heat Transfer Equation (PBHTE) has been widely used to approximate the overall temperature distribution in tissue using a perfusion parameter term in the equation during hyperthermia treatment. In the similar modeling, effective thermal conductivity (K_eff) model uses thermal conductivity as a parameter to predict temperatures. However the equations do not describe the thermal contribution of blood vessels. A countercurrent vascular network model which represents a more fundamental approach to modeling temperatures in tissue than do the generally used approximate equations such as the Pennes BHTE or effective thermal conductivity equations was presented in 1996. This type of model is capable of calculating the blood temperature in vessels and describing a vasculature in the tissue regions.

Methods

In this paper, a countercurrent blood vessel network (CBVN) model for calculating tissue temperatures has been developed for studying hyperthermia cancer treatment. We use a systematic approach to reveal the impact of a vasculature of blood vessels against a single vessel which most studies have presented. A vasculature illustrates branching vessels at the periphery of the tumor volume. The general trends present in this vascular model are similar to those shown for physiological systems in Green and Whitmore. The 3-D temperature distributions are obtained by solving the conduction equation in the tissue and the convective energy equation with specified Nusselt number in the vessels.

Results

This paper investigates effects of size of blood vessels in the CBVN model on total absorbed power in the treated region and blood flow rates (or perfusion rate) in the CBVN on temperature distributions during hyperthermia cancer treatment. Also, the same optimized power distribution during hyperthermia treatment is used to illustrate the differences between PBHTE and CBVN models. K_eff (effective thermal conductivity model) delivers the same difference as compared to the CBVN model. The optimization used here is adjusting power based on the local temperature in the treated region in an attempt to reach the ideal therapeutic temperature of 43°C. The scheme can be used (or adapted) in a non-invasive power supply application such as high-intensity focused ultrasound (HIFU). Results show that, for low perfusion rates in CBVN model vessels, impacts on tissue temperature becomes insignificant. Uniform temperature in the treated region is obtained.

Conclusion

Therefore, any method that could decrease or prevent blood flow rates into the tumorous region is recommended as a pre-process to hyperthermia cancer treatment. Second, the size of vessels in vasculatures does not significantly affect on total power consumption during hyperthermia therapy when the total blood flow rate is constant. It is about 0.8% decreasing in total optimized absorbed power in the heated region as γ (the ratio of diameters of successive vessel generations) increases from 0.6 to 0.7, or from 0.7 to 0.8, or from 0.8 to 0.9. Last, in hyperthermia treatments, when the heated region consists of thermally significant vessels, much of absorbed power is required to heat the region and (provided that finer spatial power deposition exists) to heat vessels which could lead to higher blood temperatures than tissue temperatures when modeled them using PBHTE.     

Evaluation of the effectiveness of transurethral radio frequency hyperthermia in the canine prostate: temperature distribution analysis

The heating pattern of a transurethral radio frequency (RF) applicator and its induced steady-state temperature field in the prostate during transurethral hyperthermia treatment were investigated in this study. The specific absorption rate (SAR) of the electromagnetic energy was first quantified in a tissue-equivalent gel phantom. It was used in conjunction with the Pennes bioheat transfer equation to model the steady-state temperature field in prostate during the treatment. Theoretical predictions were compared to in vivo temperature measurements in the canine prostate and good agreement was found to validate the model. The prostatic tissue temperature rise and its relation to the effect of blood perfusion were analyzed. Blood perfusion is found to be an important factor for removal of heat especially at the higher RF heating level. To achieve a temperature above 44 degrees C within 10 percent of the prostatic tissue volume, the minimum RF power required ranges from 5.5 W to 36.4 W depending on the local blood perfusion rate (omega = 0.2-1.5 ml/gm/min). The corresponding histological results from the treatment suggest that to obtain better treatment results, either higher RF power level or longer treatment time (> 180 minutes) is necessary. This is consistent with the predictions from the theoretical model developed in this study.     

The contribution of carotid rete variability to brain temperature variability in sheep in a thermoneutral environment

The degree of variability in the temperature difference between the brain and carotid arterial blood is greater than expected from the presumed tight coupling between brain heat production and brain blood flow. In animals with a carotid rete, some of that variability arises in the rete. Using thermometric data loggers in five sheep, we have measured the temperature of arterial blood before it enters the carotid rete and after it has perfused the carotid rete, as well as hypothalamic temperature, every 2 min for between 6 and 12 days. The sheep were conscious, unrestrained, and maintained at an ambient temperature of 20-22 degrees C. On average, carotid arterial blood and brain temperatures were the same, with a decrease in blood temperature of 0.35 degrees C across the rete and then an increase in temperature of the same magnitude between blood leaving the rete and the brain. Rete cooling of arterial blood took place at temperatures below the threshold for selective brain cooling. All of the variability in the temperature difference between carotid artery and brain was attributable statistically to variability in the temperature difference across the rete. The temperature difference between arterial blood leaving the rete and the brain varied from -0.1 to 0.9 degrees C. Some of this variability was related to a thermal inertia of the brain, but the majority we attribute to instability in the relationship between brain blood flow and brain heat production.     

Sensitivity of mice to systemic hyperthermia: effect of ascites tumor cell transplants

The effect of a transplantation of mastocytoma cells in the abdominal cavity on the sensitivity of mice to a systemic hyperthermia was studied. The systemic hyperthermia was induced by exposing whole-body of animals to 2,450 MHz waves under anesthesia. Core body temperature was raised up to 42.0 +/- 0.2 degrees C in 15 min and maintained constant at the temperature for variable length of time. Thermosensitivity of animal was expressed with LD50, 42 degrees which was the length of heating time at the temperature of 42 degrees C lethal for 50% of the animals examined. The transplants were mastocytoma FMA3 cells. They were transplanted at a dose of 10(5) cells per mouse. The LD50, 42 degrees observed 3, 12 hrs, 1, 2, 3 and 6 days after the transplantation was 33, 23, 17, 24 and 35 min, respectively. In mice without tumor it was 43 min.     

The effect of rate of heating or cooling prior to heating on tumor and normal tissue microcirculatory blood flow

Single vessel responses to hyperthermia were studied in tumor and normal tissues using a transparent access window chamber. Rates of heating less than or equal to .68 degrees C/minute preserved relatively better vascular function in normal than tumor tissue. A rate of heating of 1.0 degrees C/minute lowered normal tissue statis temperatures so they were no different from tumor. Cooling to 30 degrees C prior to heating slowed normal arteriolar flows to less than 5% of 38 degrees C controls. Heating resulted in increased flow in those vessels, but maximum flows never exceeded 5% of flows achieved in similar vessels which were not cooled first. The implications of this work are that rate of heating and cooling prior to heating can alter normal tissue vascular response to heat in a way that could prove deleterious to maintaining efficient vascular function in that tissue relative to tumor.     

Effect of hyperthermia on TRAIL-induced apoptotic death in human colon cancer cells: development of a novel strategy for regional therapy

Approximately 25% of patients with colorectal cancer will develop metastatic disease exclusively or largely confined to the liver, and the vast majority of these cases are not amenable to surgical resection. These unresectable cases of liver metastatic disease can be treated with isolated hepatic perfusion (IHP), which involves a method of complete vascular isolation of the liver to allow treatment of liver tumors with toxic systemic doses of chemotherapeutic agents. To improve the efficacy of IHP, hyperthermia and biological agents have been applied along with the chemotherapeutic agents. In this study, we investigated whether hyperthermia in combination with tumor necrosis factor-related apoptosis-inducing ligand (TRAIL) enhances mortality in human colorectal carcinoma CX-1 cells. Cells were treated with various concentrations of TRAIL (0-200 ng/ml) at various temperatures (40-46 degrees C) for 1 h and further incubated at 37 degrees C in the presence of TRAIL. We observed that hyperthermia at 42-43 degrees C effectively promoted TRAIL-induced apoptosis, as indicated by cell death, poly (ADP-ribose) polymerase (PARP) cleavage, and activation of caspase-8, -9, and -3. In contrast, hyperthermia at 45-46 degrees C suppressed TRAIL-induced apoptosis. We also observed that mild hyperthermia, but not acute hyperthermia, promoted cytochrome c release during treatment with TRAIL. Our data suggest that promotion of cytochrome c release during mild hyperthermia is responsible for the enhancement of TRAIL cytotoxicity.     

Hemodynamic responses to heat stress in the resting and exercising human leg: insight into the effect of temperature on skeletal muscle blood flow

Heat stress increases limb blood flow and cardiac output (Q) in humans, presumably in sole response to an augmented thermoregulatory demand of the skin circulation. Here we tested the hypothesis that local hyperthermia also increases skeletal muscle blood flow at rest and during exercise. Hemodynamics, blood and tissue oxygenation, and muscle, skin, and core temperatures were measured at rest and during exercise in 11 males across four conditions of progressive whole body heat stress and at rest during isolated leg heat stress. During whole body heat stress, leg blood flow (LBF), Q, and leg (LVC) and systemic vascular conductance increased gradually with elevations in muscle temperature both at rest and during exercise (r(2) = 0.86-0.99; P < 0.05). Enhanced LBF and LVC were accompanied by reductions in leg arteriovenous oxygen (a-vO(2)) difference and increases in deep femoral venous O(2) content and quadriceps tissue oxygenation, reflecting elevations in muscle and skin perfusion. The increase in LVC occurred despite an augmented plasma norepinephrine (P < 0.05) and was associated with elevations in muscle temperature (r(2) = 0.85; P = 0.001) and arterial plasma ATP (r(2) = 0.87; P < 0.001). Isolated leg heat stress accounted for one-half of the increase in LBF with severe whole body heat stress. Our findings suggest that local hyperthermia also induces vasodilatation of the skeletal muscle microvasculature, thereby contributing to heat stress and exercise hyperemia. The increased limb muscle vasodilatation in these conditions of elevated muscle sympathetic vasoconstrictor activity is closely related to the rise in arterial plasma ATP and local tissue temperature.     

Absence of selective brain cooling in pyrogen-induced fever in rabbits

In 9 rabbits the effect of intravenous administration of E. coli pyrogen 0.5 microgram/kg on the reaction of selective brain cooling was studied at ambient temperatures of 20, 30 and 40 degrees C. In the freely moving animals the temperatures of the brain, carotid artery and nuchal muscles were measured with an accuracy down to 0.05 degree C and the temperatures of the ear pinna and nasal mucosa were measured accurate to 0.5 degree C. The respiratory rate was measured as well. It was found that the spontaneous febrile reaction without the component of passive hyperthermia failed to cause selective brain cooling, even if its temperature reached higher values than in case of brain temperature rise caused only by high ambient temperature. On the other hand, when the high ambient temperature caused thermal panting, pyrogen administration at an ambient temperature of 30 degrees C could reduce panting, while at an ambient temperature of 40 degrees C intense panting initiated prior to the appearance of the febrile reaction and was associated with the fever and outlasted it.