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eISSN: 2574-8114

Textile Engineering & Fashion Technology

Research Article Volume 2 Issue 4

Numerical simulation of heat stress in chemical protective clothing

Jie Yang,1 Guowen Song,1 Liwen Wang,1 Yun Su,1,2 Rui Li,1 Chunhui Xiang1

1Department of Apparel, Iowa State University, USA
2College of Fashion and Design, Donghua University, China

Correspondence: Guowen Song, Department of Apparel, Events, and Hospitality Management (AESHM), Iowa State University, Ames, IA 50011, USA, Tel 51 5709 9052

Received: April 17, 2017 | Published: August 4, 2017

Citation: Yang J, Song G, Wang L, et al. Numerical simulation of heat stress in chemical protective clothing. J Textile Eng Fashion Technol. 2017;2(4):418-422. DOI: 10.15406/jteft.2017.02.00064

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Abstract

The aim of the paper is to predict heat stress of human wearing chemical protective clothing (CPC). A proposed human thermal model was applied to simulate the core and skin temperatures with inputs of human activity level, clothing properties, and environmental conditions. Manikin tests were conducted to measure the thermal insulation and evaporative resistance of clothing which were two important inputs of the thermal model. The core temperature was predicted as an indicator of heat stress to evaluate the maximum exposure time. The effects of ambient temperature, relative humidity, and metabolic rate on core temperature, skin temperature, and maximum exposure time were analyzed. It was found that metabolic rate and ambient temperature had a greater effect on the skin temperature, core temperature and maximum exposure time than the relative humidity. Additionally, the effects of ambient temperature and metabolic rate on core and skin temperatures were slightly greater in humid environments than in dry environments. The model is capable of predicting maximum exposure time in different clothing systems under various environmental conditions and can provide an instruction for the design of CPC.

Keywords: heat stress, chemical protective clothing, human thermal model, physiological response, thermal protection

Introduction

Chemical protective clothing (CPC) is designed to effectively eliminate the interaction of hazardous chemical/biological agents with the human body.1 However, thermal protection and thermal comfort are two major conflicting factors for protective clothing.2 CPC with low vapor permeability greatly restricts heat dissipation mechanisms, which creates heavy heat strain burden and reduce task efficiency as well as range-of-motion, especially when wearers are exposed to hot environments with high level of working intensity.3-5 It is therefore necessary to investigate the human physiological responses and heat stress associated with CPC for reducing heat-related illness and improving task efficiency.

Human trials were performed to investigate heat stress through indices such as tolerance time, heart rate, heat storage, and sweating rate.6-8 However, these previous studies dealing with heat stress in CPC focused on specific task, garment, and environment. Additionally, the results of these studies were not transferable to wearers in other garments or environmental conditions.4 It is necessary to develop a systematic approach to evaluate physiological responses under different human-clothing-environment systems and assist the selection and design of CPC. Thus, a mathematical model is proposed in this study to evaluate physiological responses and heat stress level in CPC.

A human thermal model,9 considering wearer characteristics, clothing properties, and environmental conditions, was applied to determine physiological responses under transient conditions. Manikin tests were conducted to measure thermal insulation and evaporative resistance of CPC, which were used as inputs to the thermal model. Based on the recommended upper limit of core temperature, the maximum exposure time of wearers was eventually evaluated taking account of activity level, clothing properties, and environmental conditions. Additionally, the effects of ambient temperature and relative humidity on physiological responses and heat stress were evaluated.

Methods

Manikin test

A ‘Newton’ sweating thermal manikin (Thermetrics, Seattle, USA) was applied to measure thermal insulation and evaporative resistance of clothing strictly following the standard ASTM F129110 and ASTM F2370,11 respectively. The temperature, heat flux, and sweating rate of each zone can be controlled independently through the software Therm DAC8 (Thermetrics, Seattle, USA). The manikin can be operated by temperature/heat flux/thermal comfort mode. For measurements of evaporative resistance, a tight-fitted knitted fabric was dressed as ‘skin’ that wicks water from sweating pores and distribute water throughout the manikin surface.12 The walking motion system of the manikin generated walking movements ranging from 0 to 1.3 m/s. The software Therm DAC8 recorded the ambient temperature, relative humidity, wind speed, manikin temperature, heat flux, sweating rate, and walking speed.

The thermal insulation of clothing was calculated by the following equation:

R c = T s T a H MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGsb qcfa4aaSbaaSqaaKqzadGaam4yaaWcbeaajugibiabg2da9Kqbaoaa laaakeaajugibiaadsfajuaGdaWgaaWcbaqcLbmacaWGZbaaleqaaK qzGeGaeyOeI0IaamivaKqbaoaaBaaaleaajugWaiaadggaaSqabaaa keaajugibiaadIeaaaaaaa@475B@ (1)

Where Rc is the thermal insulation, m2 ˚C/W; Ts is the surface temperature of manikin, ˚C; Ta is the ambient temperature, ˚C; H is the heat flux generated by manikin, W/m2.

The evaporative resistance of clothing was expressed as:

R e = P sat P amb H[ ( T s T a )/ R c ] MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGsb WcdaWgaaqaaKqzadGaamyzaaWcbeaajugibiabg2da9Kqbaoaalaaa keaajugibiaadcfajuaGdaWgaaWcbaqcLbmacaWGZbGaamyyaiaads haaSqabaqcLbsacqGHsislcaWGqbWcdaWgaaqaaKqzadGaamyyaiaa d2gacaWGIbaaleqaaaGcbaqcLbsacaWGibGaeyOeI0scfa4aamWaaO qaaKqbaoaabmaakeaajugibiaadsfalmaaBaaabaqcLbmacaWGZbaa leqaaKqzGeGaeyOeI0IaamivaSWaaSbaaeaajugWaiaadggaaSqaba aakiaawIcacaGLPaaajugibiaac+cacaWGsbWcdaWgaaqaaKqzadGa am4yaaWcbeaaaOGaay5waiaaw2faaaaaaaa@5C68@ (2)

Where Re is the evaporative resistance, Pa ˚C/W; P sat MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGqb qcfa4aaSbaaSqaaKqzadGaam4CaiaadggacaWG0baaleqaaaaa@3C14@ is the saturation vapor pressure at skin, Pa; P amb MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGqb WcdaWgaaqaaKqzadGaamyyaiaad2gacaWGIbaaleqaaaaa@3B6E@ is the ambient vapor pressure, Pa.

A type of CPC was selected to measure the clothing properties by a sweating thermal manikin in climate chamber. The thermal insulation and evaporative resistance of the CPC were 0.098 m2 ˚C/W and 22.7 Pa ˚C/W, respectively.

Human thermal model

A human thermal model proposed by Yang et al.9 was applied to predict the physiological responses such as core temperature, skin temperature, sweating rate, and blood flow rate under various conditions. The model divided the human body into 20 segments, and each segment was comprised of four layers including core, muscle, fat, and skin layer. The central blood compartment exchanged heat with all other nodes through convection. The thermal model contained three systems: a passive system predicted heat transfer within the human body and that with its environment through evaporation, radiation, convection, and conduction; an active system simulated human thermoregulation through sweating, shivering, vasoconstriction, and vasodilation; a clothing system calculated the effect of clothing properties on heat exchange between human body and environment.

The heat balance equation of each node except for the central blood compartment was given by following.13

C i,j d T i,j dt = Q i,j B i,j + D i,j1 D i,j Re s i,j (Ra d i,4 +Co n i,4 +Ev a i,4 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGdb WcdaWgaaqaaKqzadGaamyAaiaacYcacaWGQbaaleqaaKqbaoaalaaa keaajugibiaadsgacaWGubWcdaWgaaqaaKqzadGaamyAaiaacYcaca WGQbaaleqaaaGcbaqcLbsacaWGKbGaamiDaaaacqGH9aqpcaWGrbWc daWgaaqaaKqzadGaamyAaiaacYcacaWGQbaaleqaaKqzGeGaeyOeI0 IaamOqaKqbaoaaBaaaleaajugWaiaadMgacaGGSaGaamOAaaWcbeaa jugibiabgUcaRiaadsealmaaBaaabaqcLbmacaWGPbGaaiilaiaadQ gacqGHsislcaaIXaaaleqaaKqzGeGaeyOeI0IaamiraSWaaSbaaeaa jugWaiaadMgacaGGSaGaamOAaaWcbeaajugibiabgkHiTiaadkfaca GGLbGaam4CaSWaaSbaaeaajugWaiaadMgacaGGSaGaamOAaaWcbeaa jugibiabgkHiTiaacIcacaWGsbGaamyyaiaadsgalmaaBaaabaqcLb macaWGPbGaaiilaiaaisdaaSqabaqcLbsacqGHRaWkcaWGdbGaam4B aiaad6galmaaBaaabaqcLbmacaWGPbGaaiilaiaaisdaaSqabaqcLb sacqGHRaWkcaWGfbGaamODaiaadggalmaaBaaabaqcLbmacaWGPbGa aiilaiaaisdaaSqabaqcLbsacaGGPaaaaa@80F0@ (3)

Where i is the number of body segments; j is the number of node layers; C is the heat capacity, Wh/˚C; T is the temperature, ˚C; t is the time, h; Q is the heat production, W; B is the heat exchange between each node and central blood compartment, W; D is the conductive heat exchange to neighbor layers within the segment, W; Res MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsaciGGsb Gaaiyzaiaadohaaaa@392E@ , Rad MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGsb Gaamyyaiaadsgaaaa@391B@ , Con MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGdb Gaam4Baiaad6gaaaa@3924@ , and Eva MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGfb GaamODaiaadggaaaa@3920@  are the heat loss through respiration, radiation, convection, and evaporation, respectively, W.

C 81 d T 81 dt = i=1 20 j=1 4 B i,j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGdb WcdaWgaaqaaKqzadGaaGioaiaaigdaaSqabaqcfa4aaSaaaOqaaKqz GeGaamizaiaadsfalmaaBaaabaqcLbmacaaI4aGaaGymaaWcbeaaaO qaaKqzGeGaamizaiaadshaaaGaeyypa0tcfa4aaabCaOqaaKqbaoaa qahakeaajugibiaadkealmaaBaaabaqcLbmacaWGPbGaaiilaiaadQ gaaSqabaaabaqcLbmacaWGQbGaeyypa0JaaGymaaWcbaqcLbmacaaI 0aaajugibiabggHiLdaaleaajugWaiaadMgacqGH9aqpcaaIXaaale aajugWaiaaikdacaaIWaaajugibiabggHiLdaaaa@5BE1@ (4)

Where C18 and T81 are the heat capacity and temperature of the central blood node, respectively.

The evaporation at skin surface was comprised of heat exchange by water vapor diffusion and sweat evaporation, the details of the calculation can be found in the literature.14 The sensible heat exchange including convection and radiation between the skin and environment was calculated by the following.14

Q cl = ( T t o )A I cl + 1 ( h c + h r ) f cl MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacaWGrb WcdaWgaaqaaKqzadGaam4yaiaadYgaaSqabaqcLbsacqGH9aqpjuaG daWcaaGcbaqcfa4aaeWaaOqaaKqzGeGaamivaiabgkHiTiaadshalm aaBaaabaqcLbmacaWGVbaaleqaaaGccaGLOaGaayzkaaqcLbsacaWG bbaakeaajugibiaadMeajuaGdaWgaaWcbaqcLbmacaWGJbGaamiBaa WcbeaajugibiabgUcaRKqbaoaalaaakeaajugibiaaigdaaOqaaKqb aoaabmaakeaajugibiaadIgalmaaBaaabaqcLbmacaWGJbaaleqaaK qzGeGaey4kaSIaamiAaSWaaSbaaeaajugWaiaadkhaaSqabaaakiaa wIcacaGLPaaajugibiaadAgajuaGdaWgaaWcbaqcLbmacaWGJbGaam iBaaWcbeaaaaaaaaaa@5E91@ (5)

Where T is the skin temperature, ˚C; t0 is the operative temperature, ˚C; A is the surface area of the segment, m2; Icl is the thermal insulation of clothing, m2 ˚C/W; hc and hr are the convective and radiative heat transfer coefficient, respectively, W/ m2 ˚C; fcl is the clothing area factor, NA.

Active system calculated the human thermoregulation including vasoconstriction, vasodilation, shivering, and sweating. Warm and cold signals from the receptors arrived at the hypothalamus and then appropriate effector commands were issued.15 In the work of Stowijk,13 the warm and cold signals were calculated through temperature difference between each node and its set-point. The detailed information of the calculation of vasoconstriction, vasodilation, shivering, and sweating can be found in the literature.13,14

Heat stress prediction

Core temperature is one of the most important physiological response parameters and is a critical indicator of heat stress. Maximum exposure time can be evaluated by the core temperature reaching a defined maximum value. The ISO 793316 recommended a maximum core temperature of 38.0˚C. Some studies17-19 used 38.5˚C as the maximum core temperature, and Xu et al.20 applied 39.0˚C as the threshold value. In this work, the endurance time was calculated by the length of time until the core temperature reaches 38.5˚C.

Results and discussion

The thermal model required inputs of human/clothing/environment parameters such as metabolic rate, thermal insulation, evaporative resistance, ambient temperature, relative humidity, and wind speed. Different environmental conditions and metabolic rate were selected to simulate human thermal responses, shown in Table 1.

Cases

Ta (˚C)

RH (%)

Q (W/m2)

V (m/s)

Case 1

30

40

300

0.5

Case 2

30

70

300

0.5

Case 3

40

40

300

0.5

Case 4

40

70

300

0.5

Case 5

30

40

400

0.5

Case 6

30

70

400

0.5

Case 7

40

40

400

0.5

Case 8

40

70

400

0.5

Table 1 Environmental conditions and activity intensities for simulation

Effects of environmental conditions on physiological responses and heat stress

The mean skin temperatures were simulated by the human thermal model under different ambient temperature and relative humidity at the metabolic rate of 300 W/m2 (Case 1-4), shown in Figure 1. It was clear that the mean skin temperatures showed a positive correlation with the ambient temperature and humidity. The model predicted higher mean skin temperatures at the relative humidity of 70% than those at the relative humidity of 40% under both 30˚C and 40˚C ambient temperatures, which was in consistent with the results from Nicol21 where high humidity increased discomfort. The effect of humidity is particularly important in hot environments in which the evaporative heat loss predominates. Besides, it can be explained by the fact that evaporative heat loss was determined by the vapor pressure difference between the skin and the environment.1 When the environment temperature was higher than the skin temperature, evaporation would become the only way to dissipate heat from the human body to the environment. The higher the ambient humidity, the less evaporative heat exchanged with the environment. The mean skin temperatures significantly increased when the ambient temperature rose from 30˚C to 40˚C, and the peak value of mean skin temperature difference between the 30˚C and 40˚C environment was 0.69˚C (RH=40%) and 0.72˚C (RH=70%), respectively. The mean skin temperature at the ambient temperature of 40˚C increased at a rate much higher than that at the ambient temperature of 30˚C, which was 0.039, 0.044, 0.093, and 0.097˚C/min during the first 15 min for case 1 to case 4. At the ambient temperature of 30˚C, the skin temperature was higher than the environment temperature leading to heat dissipation to the environment. When the human body was exposed to the ambient temperature of 40˚C, the human body absorbed heat from the environment by radiation and convection.

Figure 1 Mean skin temperatures simulated for case 1 to case 4.

The model predicted the core temperature for case 1 to case 4, displayed in Figure 2. Similar to the mean skin temperature, the simulated core temperatures showed a positive correlation with the ambient temperature and relative humidity. At the ambient temperature of 30˚C, the simulated core temperatures at the humidity of 70% were slightly higher than those at 40%, and the similar trend was observed at the ambient temperature of 40˚C. However, a larger difference of peak core temperature between case 3 and case 4 was observed compared with that of case 1 and case 2. It was probably due to the sweat evaporation which played an important role in human thermoregulation, particularly in the hot environment.

Figure 2 Core temperatures simulated for case 1 to case 4.

The core temperatures increased quickly in the first 30 min, it approximately increased by 1.0˚C for case 1 and case 2, and 1.2˚C for case 3 and case 4, respectively. At the end of the exposure, the core temperature was 38.44, 38.49, 38.80, and 38.89˚C, respectively. The core temperature in case 1 and case 2 did not exceed the 38.5˚C, while that in case 3 and case 4 exceeded the threshold value of 38.5˚C recommended in the literature.17,18 Therefore, the ambient temperature was a major factor affecting the heat stress. On the one hand, the human body gains heat from ambient through convection and radiation in the hot environment. On the other hand, the rate of metabolic heat production in the hot environment was higher than that in the normal environment.9 Based on the recommended core temperature limit, the maximum exposure time was 60 min for case 3 and 57 min for case 4. It can be concluded that the maximum exposure time should be longer when exposed to the dry environment than to the humid environment.

Effects of metabolic rate on physiological responses and heat stress

The model predicted the mean skin temperatures for case 5 to case 8, displayed in Figure 3. It was obvious that the simulated mean skin temperatures for case 5-8 was much larger than those in corresponding case 1-4. The heat storage in human body increased with the increasing of metabolic rate, causing the rise of mean skin temperature. In the first 15 min, the increase rate of mean skin temperature for the case 5 to case 8 was 0.060, 0.067, 0.11, and 0.12˚C/min, respectively. The case 8 had the highest increase rate of mean skin temperature caused by the high ambient temperature and humidity. Compared with the mean skin temperature increase rate in case 1 to case 4, the mean skin temperature increase rate at metabolic of 400 W/m2 approximately increased by 50% and 20% at the ambient temperature of 30˚C and 40˚C, respectively. The peak value of mean skin temperature occurred at the end of the exposure, and the difference of mean skin temperature peak value between case 1 and case 5, case 2 and case 6, case 3 and case 7, and case 4 and case 8 was 0.43, 0.47, 0.40, and 0.42˚C, respectively. Thus, the mean skin temperature increase rate in a more humid environment (RH=70%) was slightly higher than that in a less humid environment (RH=40%) when the metabolic rate increased from 300 to 400 W/m2. According to (Figure 1) (Figure 3), the ambient temperature and metabolic rate greatly influenced the mean skin temperatures than the ambient humidity did.

Figure 3 Mean skin temperatures simulated for case 5 to case 8.

The model predicted the core temperatures for case 5 to case 8, displayed in Figure 4. The core temperatures increased sharply during the first 30 min, and the increase rate of core temperature was 0.043, 0.046, 0.046, and 0.053˚C/min, respectively. The case 8 had the highest increase rate of core temperature, which displayed the same trend with case 4. The temperature difference between case 5 and case 6 was much lower than that between case 7 and case 8, which can be explained by the sweating evaporation of human body. The maximum core temperature during the exposure for case 5 to case 8 was 38.95, 39.02, 39.31, and 39.42˚C, respectively. When the metabolic rate increased from 300 to 400 W/m2, the maximum core temperature in case 5 to case 8 was nearly 0.5˚C larger than that in case 1 to case 4 regardless of the change of ambient temperature and humidity.

The maximum exposure time was evaluated based on the parameters in case 1 to case 8, shown in Figure 5. The longest exposure time was observed for case 1 with 129 min, followed by the case 2 with 126 min, and the shortest exposure time was found for case 8 with only 36 min. It can be concluded that the maximum exposure time was mostly influenced by the ambient temperature and metabolic rate. Therefore, working in a hot environment with heavy activity level can greatly reduce maximum exposure time. Although the maximum exposure time was affected by the relative humidity, the increased relative humidity from 40% to 70% caused approximately 3-6 min decreased in maximum exposure time. Therefore, intolerable heat strain would easily occur in a hot environment. Additionally, the physical load could further enhance heat stress raising the risk of danger to wearers’ health and safety.20

Figure 4 Core temperatures simulated for case 5 to case 8.
Figure 5 Maximum exposure time under the parameters for case 1 to case 8.

Conclusion

A human thermal model was applied to evaluate physiological responses under different environmental conditions and activity intensities when wearing a typical CPC. Based on the recommended core temperature threshold, the maximum exposure time of wearer was evaluated. The results indicated that the ambient temperature and metabolic rate significantly increase heat stress, while relative humidity only slightly affects the physiological responses and heat stress. The current model was capable of predicting maximum exposure time under different environmental conditions, which can be used for human safety assessment.

Many factors such as activity intensity, clothing properties, air gap size, and environmental conditions affect physiological responses and heat stress. The CPC should be designed not only to offer chemical protection but also to improve thermal comfort. In this work, the effects of activity intensity and environmental conditions were analyzed. In the future work, the effects of clothing properties and air gap size on heat stress will be investigated to improve the understanding of thermal comfort of CPC and wearer performance. A 3-D body scanning system will be applied to measure the air gap between skin and clothing, and the influence of air gap thickness on heat transfer and heat stress will be analyzed.

Acknowledgements

None.

Conflict of interest

Author declares there is no conflict of interest in publishing the article.

References

  1. McLellan TM, Pope JI, Cain JB, et al. Effects of metabolic rate and ambient vapour pressure on heat strain in protective clothing. Eur J Appl Physiol Occup Physiol. 1996;74(6):518‒527.
  2. Sun G, Yoo HS, Zhang XS, et al. Radiant protective and transport properties of fabrics used by wildland firefighters. Textile Research J. 2000;70(7):567‒573.
  3. Lee S, Obendorf SK. A statistical model to predict pesticide penetration through nonwoven chemical protective fabrics. Textile Research J. 2002;71(11):1000‒1009.
  4. Adams PS, Slocum AC, Monroe Keyserling W. A model for protective clothing effects on performance. International J Clothing Science & Technology. 1994;6(4):6‒16.
  5. Pandolf KB, Allan AE, Gonzalez RR, et al. Chemical warfare protective clothing: identification of performance limitations and their possible solution. Army Research Institute of Environmental Medicine. Natick, USA; 1987. p. 1‒8.
  6. McLellan TM. Sex-related differences in thermoregulatory responses while wearing protective clothing. Eur J Appl Physiol Occup Physiol. 1998;78(1):28‒37.
  7. Cadarette BS, Cheuvront SN, Kolka MA, et al. Intermittent microclimate cooling during exercise-heat stress in US army chemical protective clothing. Ergonomics. 2006;49(2):209‒219.
  8. Johnson RF, Kobrick JL. Effects of wearing chemical protective clothing on rifle marksmanship and on sensory and psychomotor tasks. Military Psychology. 1997;9(4):301‒314.
  9. Yang J, Weng WG, Zhang BT. Experimental and numerical study of physiological responses in hot environments. J Therm Biol. 2014;45:54‒61.
  10.  ASTM F 1291. Standard test method for measuring the thermal insulation of clothing using a heated manikin. American Society for Testing and Materials. USA; 2005.
  11. ASTM F 2370. Standard test method for measuring the evaporative resistance of clothing using a sweating manikin. American Society for Testing and Materials. USA; 2005.
  12. Ueno S, Sawada SI. Correction of the evaporative resistance of clothing by the temperature of skin fabric on a sweating and walking thermal manikin. Textile Research J. 2012;82(11):1143‒1156.
  13. Stolwijk JAJ. A mathematical model of physiological temperature regulation in man.USA: NASA Technical Report; 1921. p. 1‒82.
  14. Tanabe S, Kobayashi K, Nakano J, et al. Comprehensive combined analysis with multi-node thermoregulation model (65mn), radiation model and CFD for evaluation of thermal comfort. Energy Buildings. 2002;34(6):637‒646.
  15. Parsons K. Human thermal environments: the effects of hot, moderate and cold environments on human health, comfort and performance. 2nd ed. Taylor & Francis, London & New York, USA; 2003. p. 1‒560.
  16. ISO 7933. Ergonomics of the thermal environment-analytical determination and interpretation of heat stress using calculation of the predicted heat strain. 2nd ed. International Standard Organization. Geneva, Europe; 2004.
  17. Yang Y, Chan AP. Perceptual strain index for heat strain assessment in an experimental study: an application to construction workers. J Therm Biol. 2015;48:21‒27.
  18. McLellan TM. The importance of aerobic fitness in determining tolerance to uncompensable heat stress. Comp Biochem Physiol A Mol Integr Physiol. 2001;128(4):691‒700.
  19. Havenith G. Heat balance when wearing protective clothing. Ann Occup Hyg. 1999;43(5):289‒296.
  20. Xu XJ, Gonzalez JA, Santee WR, et al. Heat strain imposed by personal protective ensembles: quantitative analysis using a thermoregulation model. Int J Biometeorol. 2016;60(7):1065‒1074.
  21. Nicol F. Adaptive thermal comfort standards in the hot-humid tropics. Energy & Buildings. 2004;36(7):628‒637.
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