Exercise & Sport Sciences Reviews:
Effect of Thermal Stress on Cardiac Function
Wilson, Thad E.1,2; Crandall, Craig G.3,4
1Institute for Neuromusculoskeletal Research, Ohio University; 2Departments of Biomedical Sciences and of Specialty Medicine, Ohio University College of Osteopathic Medicine, Athens, OH; 3Institute for Exercise and Environmental Medicine, Presbyterian Hospital of Dallas; and 4Department of Internal Medicine, University of Texas Southwestern Medical Center, Dallas, TX
Address for correspondence: Thad E. Wilson, Ph.D., Ohio University-COM, 228 Irvine Hall, Athens, OH 45701 (E-mail: firstname.lastname@example.org).
Accepted for publication: September 20, 2010.
Associate Editor: Scott J. Montain, Ph.D., FACSM
Whole-body heating decreases pulmonary capillary wedge pressure and cerebral vascular conductance and causes an inotropic shift in the Frank-Starling curve. Whole-body cooling increases pulmonary capillary wedge pressure and cerebral vascular conductance without changing systolic function. These and other data indicate that factors affecting cardiac function may mechanistically contribute to syncope during heat stress and improvements in orthostatic tolerance during cold stress.
Heat and cold stresses have direct impacts on many of the fundamental control mechanisms of stroke volume, such as preload, afterload, diastolic function or compliance, and systolic function or inotropy. The purpose of this review is to integrate a recent series of thermal physiology studies performed by the authors (2,4,10,29,32,35) that identify the mechanisms by which heat and cold stresses alter cardiac mechanics and function. These data and mechanisms will then be applied to our understanding of thermal-induced changes in orthostatic tolerance, where heat stress increases and cold stress decreases the likelihood of syncope during an orthostatic challenge in humans. The importance of thermal-induced changes in orthostatic tolerance is evident in occupations where workers are in hot ambient conditions while in the upright position and thus are at risk for heat syncope or where a countermeasure such as skin-surface cooling may need to be used to increase orthostatic tolerance.
In this review, heat and cold stresses are delimited, unless otherwise mentioned, to human passive-thermal stresses where human subjects are exposed to a warm or cool environment via a water-perfused garment (fitted suit that covers the body except the hands, feet, neck, and head) rather than a stress that also induces a significant change in metabolism (e.g., occupational tasks, exercise, or shivering). This important distinction of passive-thermal stress versus exercise-thermal stress allows for the determination of direct thermal effects or physiological responses to the thermal stress independent of increases in cardiac output needed to perfuse working muscles or other changes associated with exercise-heat (28) or exercise-cold (25) stress. The water-perfused garment method of passive-thermal stress clamps skin temperature at an elevated temperature that then increases internal temperature during whole-body heating, whereas during whole-body (or skin-surface) cooling, skin temperature is clamped at a lower temperature but does not change internal temperature. These passive-thermal stresses cause large redistributions of blood flow, especially in the skin, but these blood flow redistributions are different from those seen during exercise and some other passive-thermal stress models such as water immersion.
CONTROL AND REGULATION OF STROKE VOLUME
Cardiac output increases during whole-body heating but does not significantly change during whole-body cooling (17,31,34,35). In contrast, stroke volume is maintained or slightly increased by both thermal stressors (17,34,35). Hyperbolic Frank-Starling relations (plotting stroke volume to left ventricular filling pressure) can be used to explore the control and regulation of stroke volume during thermal stresses (Fig. 1A). In healthy humans, left ventricular filling pressure can be indexed with pulmonary capillary wedge pressure obtained via a Swan-Ganz catheter. Data from our studies (4,29) indicate that whole-body heating shifts the operating point to a steeper portion of a Frank-Starling curve compared with the relatively plateaued location of the operating point on a normothermic Frank-Starling curve (Fig. 1B). This shift results in a larger reduction in stroke volume per reduction in left ventricular end-diastolic pressure indexed from pulmonary capillary wedge pressure ((29) Fig. 1C). In contrast, during whole-body cooling, the operating point shifts upward on the plateau portion of a Frank-Starling curve compared with normothermia; this shift results in a relatively small reduction in stroke volume per reduction in left ventricular end-diastolic pressure during a subsequent orthostatic challenge ((29) Fig. 1B, C). The downward shift of the operating point to a steeper portion of a Frank-Starling curve during heat stress and the upward shift to a flatter portion of a Frank-Starling curve during cold stress demonstrate direct thermal effects on the control and regulation of stroke volume. However, other physiological parameters affect the Frank-Starling relation and are modified by thermal stress, including preload, afterload, compliance, and inotropy.
Whole-body heating decreases right-sided preload (right atrial pressure and central venous pressure (8,10,18,19,21,22,35)), as well as left-sided preload (left ventricular end-diastolic volume and pulmonary capillary wedge pressure (35)). In healthy humans exposed to heat stress, right- and left-sided preloads decrease by a similar magnitude (35). This indicates that central venous pressure can be used to predict changes in left ventricular filling pressure during thermal stress. The reason for this decrease in preload during heat stress is likely multifactoral, being related to blood volume distribution, cardiac output/venous return, and systemic vascular conductance. Heat stress increases cutaneous vascular volume (14) and translocates blood volume out of the splanchnic, renal, and central reservoirs ((10) Fig. 2). Decreases in central blood volume (10) along with decreases in left ventricular end-diastolic volume (29) lead to a scenario where preload is decreased initially and further changes in preload, such as that which occurs during an orthostatic challenge, could lead to large reductions in stroke volumes, as predicted and identified in Figure 1.
Cold stress marginally increases both right (central venous pressure (12,35))- and left (pulmonary capillary wedge pressure (35))-sided preload. In healthy humans, right- and left-sided preloads increase by a similar magnitude and thus indicate that central venous pressure can be used to predict changes in left ventricular filling pressure during cold stress (35). However, despite these changes in pressure, corresponding changes in left ventricular end-diastolic volumes are often not observed in young healthy individuals, but are in older individuals (29,32). Central blood volume assessments during whole-body cooling have been measured only indirectly via impedance, with mixed results (5,12). Thus, in the supine/prone position, cold stress increases pulmonary capillary wedge pressure without altering stroke volume, and subsequent reductions in stroke volume for a given reduction in pulmonary capillary wedge pressure during an orthostatic stress are attenuated. This is consistent with shifts in the operating point to a flatter portion of a Frank-Starling curve (Fig. 1).
Heat stress does not change, or slightly decreases, mean arterial pressure despite large increases in cardiac output, whereas systemic vascular conductance increases substantially, primarily because of large increases in cutaneous vascular conductance (17). In contrast to the cutaneous circulation, renal and splanchnic vascular conductance decreases during heat stress (18,22,27). Increases in muscle sympathetic nerve activity by this thermal condition (7,13,24) indicate that a greater vasoconstrictor signal is sent to muscle blood vessels, but it is currently unclear if muscle vascular conductance is altered in these conditions. Mean pulmonary artery pressure decreases during heat stress, and this, coupled with the increase in cardiac output, results in no significant alteration in pulmonary vascular conductance (35).
Cold stress increases mean arterial pressure and decreases systemic vascular conductance (11,12,15,16,31,32,35). This increase in mean arterial pressure is related to decreases in vascular conductance in both glabrous and nonglabrous cutaneous vasculature and in the brachial, renal, celiac, and superior mesenteric arteries ((34) Fig. 3). Decreases in brachial vascular conductance are believed to be confined primarily to the skin because muscle sympathetic nerve activity does not appreciably change during whole-body cooling (11). The increase in mean arterial pressure in response to whole-body cooling is related to age and to central arterial stiffness, where individuals with stiffer arteries experience greater increases in arterial blood pressure (16). Pulmonary vascular conductance does not significantly change during whole-body cooling likely because there is little to no change in cardiac output coupled with both mean pulmonary artery pressure and pulmonary capillary wedge pressure increasing by a similar magnitude (35).
Compliance and Diastolic Function
No significant alteration in left ventricular compliance is observed during acute thermal perturbations, as represented when we express pulmonary capillary wedge pressure to left ventricular end-diastolic volume (29). During whole-body heating, indices of diastolic function (e.g., the ratio of blood velocity/mitral annular tissue velocity during the early phase of diastole and rate of untwisting) are preserved despite decreases in preload, thus indicating that subtle improvements in diastolic function may be occurring (2,23). During whole-body cooling, variables associated with diastolic function are not significantly altered in young healthy individuals or in older individuals with already reduced diastolic functions (32).
Heat stress decreases preload, yet stroke volume is maintained or slightly increased (17). Radionucleotide multigated acquisition and echocardiography data indicate increases in ejection fraction (10,29) and isovolumic acceleration of the septal and lateral mitral annuli (2) with the imposition of a heat stress. Also identifying a positive inotropy effect during whole-body heating, Nelson et al. (23) observed increases in left ventricular twist rates. During recent studies to more fully characterize the impact of heat stress on the Frank-Starling relation, we included colloid volume loading (12 mL·kg−1 Voluven) during whole-body heating (4). The intent of the colloid volume loading was to increase preload to identify if there was a leftward shift in the Frank-Starling relation or if the volume loading just further extended the normothermic curve. Our data identify a leftward shift in the Frank-Starling relation and provide further support that positive inotropy is present during whole-body heating (Fig. 1B).
Whole-body cooling does not significantly change ejection fraction or tissue Doppler-derived values of systolic function (32). This finding was important to identify because it is possible that a rightward shift in the Frank-Starling relation, caused by afterload, could have been masking positive inotropy changes (leftward shifts in the Frank-Starling relation). Because whole-body cooling increases mean arterial pressure and central venous pressure, it is possible that loading of arterial and cardiopulmonary baroreceptors is inhibiting a positive inotropy response to cold stress.
CONTROL AND REGULATION OF HEART RATE
Cardiac output increases to values often well above 10 L·min−1 during whole-body heating (17). Because stroke volume is maintained or only slightly increased during heat stress, the increase in heart rate is the primary driving force behind these increases in cardiac output. The control and regulation of heart rate during heat stress may be related to 1) direct effects of temperature on the sinoatrial node and 2) sympathetic and parasympathetic effects on the heart caused by either the baroreflexes or a global hyperadrenergic state. During cold stress, heart rate does not significantly change (29,35).
The efferent arm of the arterial baroreflexes may participate in increasing heart rate during whole-body heating if mean arterial pressure trends downward during the heat stress (6). In contrast, during cooling, baroreflexes could be acting to suppress heart rate, as there is loading of carotid, aortic, and cardiopulmonary baroreceptors. The absence of a change in heart rate during whole-body cooling suggests that other factors are counteracting this baroreflex suppression of heart rate. Heat stress can be described as a global hyperadrenergic state (26), resulting in both increased noradrenergic signaling and circulating catecholamines. It is unknown if cold stress results in a global hyperadrenergic state, although increases in plasma norepinephrine are observed (15).
IMPLICATION FOR ORTHOSTATIC TOLERANCE
Thermal stress alters the cardiovascular response to postural changes, where heat stress decreases (1,19,20,30,31) and cold stress in the absence of shivering increases (15,31) orthostatic tolerance. We have identified decreases in resting cerebral blood velocity during heat stress and even greater changes during gravitational perturbations such as lower body negative pressure (LBNP (3,30); Fig. 4). Slight increases in cerebral blood velocity during cold stress are observed, and these increases are maintained during heat-up tilt (15,31). Alterations in orthostatic tolerance and cerebral blood flow caused by thermal stress seem to be independent of the gain of other neural-induced postural reflexes (13,33) but rather, in part, are related to previously alluded-to alterations in cardiac function and mechanics.
Heat stress requires an increase in cardiac output to perfuse the cutaneous vasculature for heat dissipation purposes. The combination of heat and orthostatic stress can lead to instances where cardiac output, albeit higher than normothermic values, is not adequate for the vascular conductance needs of the body. To prevent syncope in this condition, either cutaneous vascular conductance needs to be reduced, or orthostatic-induced decreases in cardiac output need to be attenuated. Leading up to the point of syncope, the reduction in cutaneous vasculature only is approximately 15% from peak heat stress values and thus is not sufficient to prevent a fall in mean arterial pressure (Fig. 5 (9)). Highlighting this issue, if brief skin cooling is performed on hyperthermic individuals, causing pronounced decreases in cutaneous vascular conductance, mean arterial pressure and cerebral blood velocity are maintained during head-up tilt despite a similar decrease in cardiac output (31). An alternate method to prevent heat syncope is to attenuate orthostatic-induced decreases in cardiac output. In our experiments, heat stress exacerbates the reduction in stroke volume during an orthostatic challenge (29). This inability to maintain adequate stroke volume, leading to compromised mean arterial pressure and cerebral blood velocity, is likely caused by the decrease in preload, because volume loading increases orthostatic tolerance time (19) and moves the operating point from a steep to a plateau portion of the Frank-Starling relation (Fig. 1C).
The mechanisms by which cold stress improves orthostatic tolerance may be the opposite of what is problematic during heat stress. Whole-body cooling causes peripheral and visceral vasoconstriction to allow for adequate control of systemic vascular conductance during orthostatic stress. The resultant increase in mean arterial pressure by this thermal provocation ensures adequate cerebral blood flow during orthostatic stress in otherwise heat-stressed and normothermic individuals (15,31). Whole-body cooling also increases preload and attenuates the reduction in stroke volume and cardiac output to orthostatic stress (12,35). This response may be caused by cold stress moving the operating point of a Frank-Starling curve to a flatter portion, where decreases in preload result in relatively small reductions in stroke volume (Fig. 1C).
In summary, during heat stress, preload and afterload decrease, whereas inotropy increases to maintain or increase stroke volume (Table). Heart rate increases through a direct effect of local heat on the sinoatrial node, in combination with withdrawal of parasympathetic neural activity, coupled with increases in cardiac sympathetic neural activity. These combined stroke volume and heart rate responses result in large increases in cardiac output during the heat stress. During cold stress, preload and afterload increase, with no quantifiable change in inotropy (Table). Heart rate does not change possibly because of a baroreflex suppression, with the net result being no significant changes in cardiac output during cold stress. Changes in cardiac output and function are proposed to mechanistically contribute to decreases in orthostatic tolerance during heat stress and improvements in orthostatic tolerance during cold stress.
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The authors express their appreciation to the many collaborators at the Institute for Exercise and Environmental Medicine, Texas Health Presbyterian Hospital Dallas; Heart and Vascular Institute, Penn State College of Medicine; and Rigshospitalet, University of Copenhagen, who contributed to the studies discussed in this review. The authors also thank the Office of Communication at the Ohio University College of Osteopathic Medicine for the aid in developing Figure 1.
This work was supported by the National Heart, Lung, and Blood Institute (HL-10488, HL-61388, HL-67422, and HL-84072) and the American Heart Association.
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