Suppr超能文献

冷水环境中静息及运动男性的体表外壳隔热情况

Superficial shell insulation in resting and exercising men in cold water.

作者信息

Veicsteinas A, Ferretti G, Rennie D W

出版信息

J Appl Physiol Respir Environ Exerc Physiol. 1982 Jun;52(6):1557-64. doi: 10.1152/jappl.1982.52.6.1557.

Abstract

From measurements of subcutaneous fat temperature (Tsf) at known depths below the surface, skin surface temperature (Tsk), and direct skin heat flux (H), the superficial shell isulation (Iss) of the thigh (fat + skin) was calculated as Iss (degrees C.m2.w-1) = (Tsf - Tsk)/H in nine male subjects immersed head out in a well-stirred water bath. Also, at critical water temperature (CWT = 28-33 degrees C), eight of the subjects rested for 3 h, enabling overall maximal tissue insulation (It,max) to be calculated as It,max (degrees C.m2.W-1) = (Tre - Tw)/(0.92 M +/- delta S), where Tre is rectal temperature, Tw is water temperature, M is metabolic rate, and s is loss or gain of body heat. Five subjects performed up to 2 h of mild leg cycling, preceded and followed by 60 min of rest, and both thigh Iss and overall It were measured during exercise. Iss increased from minimal values in Tw greater than 33 degrees C to maximal values (Iss,max) at CWT or below. Iss,max was linearly related to tissue thickness (d) in millimeters of fat plus skin, Iss,max (degrees C.m2.W-1) = 0.0048d-0.0052; r = 0.95, n = 37, and was not influenced by leg exercise up to a metabolic rate of 150 W.m-2 in CWT despite large increases in Tsf and H and large decreases in overall It. The slope of Iss,max vs. depth, 0.0048 degrees C.m2.W-1.mm-1, is almost identical to thermal resistivity of fat in vitro, suggesting that the superficial shell is unperfused in CWT at rest or during mild exercise. When maximal superficial shell insulation (It,ss,max) for the whole body was calculated with allowance for differing fat thicknesses and surface areas of body regions, it could account for only 10-15% of overall It,max at rest and 35-40% of overall It in mild exercise. We suggest that the poorly perfused muscle shell plays a more important role as a defense against cooling at CWT than does the superficial shell (fat + skin), particularly at rest.

摘要

通过测量已知皮下深度的皮下脂肪温度(Tsf)、皮肤表面温度(Tsk)以及直接的皮肤热通量(H),在9名头部露出浸于充分搅拌水浴中的男性受试者身上,计算出大腿(脂肪+皮肤)的浅表外壳隔热值(Iss),计算公式为Iss(℃·m²·W⁻¹)=(Tsf - Tsk)/H。此外,在临界水温(CWT = 28 - 33℃)时,8名受试者休息3小时,从而能够计算出总体最大组织隔热值(It,max),计算公式为It,max(℃·m²·W⁻¹)=(Tre - Tw)/(0.92M ± ΔS),其中Tre为直肠温度,Tw为水温,M为代谢率,S为身体热量的损失或增加。5名受试者进行长达2小时的轻度腿部骑行,前后各休息60分钟,在运动过程中测量大腿的Iss和总体的It。Iss在Tw大于33℃时从最小值增加到CWT及以下时的最大值(Iss,max)。Iss,max与脂肪加皮肤毫米数表示的组织厚度(d)呈线性相关,Iss,max(℃·m²·W⁻¹)= 0.0048d - 0.0052;r = 0.95,n = 37,并且在CWT下,尽管Tsf和H大幅增加且总体It大幅下降,但在代谢率达到150W·m⁻²之前,腿部运动对其没有影响。Iss,max与深度的斜率为0.0048℃·m²·W⁻¹·mm⁻¹,几乎与体外脂肪的热阻相同,这表明在CWT下休息或轻度运动时,浅表外壳未被灌注。当考虑身体各部位不同的脂肪厚度和表面积来计算全身的最大浅表外壳隔热值(It,ss,max)时,它在休息时仅占总体It,max的10 - 15%,在轻度运动时占总体It的35 - 40%。我们认为,在CWT下,灌注不良的肌肉外壳作为抵御寒冷的防御机制比浅表外壳(脂肪+皮肤)发挥着更重要的作用,尤其是在休息时。

文献AI研究员

20分钟写一篇综述,助力文献阅读效率提升50倍。

立即体验

用中文搜PubMed

大模型驱动的PubMed中文搜索引擎

马上搜索

文档翻译

学术文献翻译模型,支持多种主流文档格式。

立即体验