Thermal properties of wood and wood composites made from wood waste

IF 2 4区 农林科学 Q2 AGRONOMY International Agrophysics Pub Date : 2021-11-03 DOI:10.31545/intagr/142472
M. Božiková, Petr Kotoulek, Matúš Bilčík, Ľ. Kubík, Z. Hlaváčová, P. Hlaváč
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The velocity of the temperature equalization in a material during non-stationary processes characterizes thermal diffusivity a (m s) which has been defined in the literature (Suleiman et al., 1999; Adl-Zarrabi, 2004). The volume specific heat cρ (J m K) may be expressed as ratio thermal conductivity λ and thermal diffusivity a (Bouguerra et al., 2001; Nakaya et al., 2016). The thermal parameters of wood and wood-based products are affected by many internal and external factors such as: moisture content (Troppova et al., 2014; Glass and Zelinka, 2010), temperature (Zhou et al., 2013), density of the wood, direction of heat flow with respect to the grain (Ružiak et al., 2017; Öner et al., © 2021 Institute of Agrophysics, Polish Academy of Sciences M. BOŽIKOVÁ et al. 252 2009). The thermal properties of wood-based materials are required in applications such as fuel conversion, building construction and other fields of industry (Zi-Tao et al., 2011). The problem of thermal parameter measurements of wood-based panels has already been discussed in a previous study and new results of the property have been delivered by Sonderegger and Niemz (2012), Li et al. (2013). Steadystate methods are used for the detection of wood thermal parameters (Hrčka and Kurjatko, 2006). Transient methods were introduced by Adl-Zarrabi and Boström (2004), Tavman (1996). Avramidis and Lau (1992) which measured the thermal coefficients of wood particles using a transient heat-flow method. The TPS technique is described in detail by Gustafsson (1991) and Wechsler (1992). According Karawacki et al. (1992) the extended dynamic plane source (EDPS) method is convenient for low thermal conductivity materials (Beck and Arnold, 2003; Malinarič, 2004). It was applied to the detection of the thermophysical properties of the solid wood of coniferous trees by authors Krišťák et al. (2019). Knowledge of the thermal properties of wood is essential for determining of its future usage. Based on the presented facts, the main aim of this research was the identification of the selected thermal properties for different types of woods and wood composites made from wood waste in Slovakia using the dynamic plane source (DPS) method. The main benefit of the research were to establish the relationships between the thermal parameters for the different moisture contents of wood and wood composites – oriented strand board (OSB) detected in the tangential and radial direction. MATERIALS AND METHODS The thermal conductivity, thermal diffusivity and the volume specific heat of the wood and the products made in Slovakia were investigated. Measurements were performed on five types of wood samples: softwood – spruce (Picea abies) and black pine (Pinus nigra), hardwood – beech (Fagus silvatic) and oak (Quercus robur) and also on medium hardwood – chestnut (Aesculus hippocastanum). The relative moisture contents of the measured wood samples fell within the following range – 0-35%. The wood samples were prepared in two directions. The tangential direction is perpendicular to the grain but tangent to the growth rings and the radial direction is normal to the growth rings and perpendicular to the grain in the radial direction. For every wood type special OSB samples were taken with tangential and radial directions. For the purpose of taking OSB thermal parameter measurements, samples from of wood-waste were prepared with the majority content of the wood species having a moisture content in the range 22-26% and the final product – samples of the examined OSB had a relative moisture content ranging from 4 to 7%. The dimensions of all of the measured samples were the same (150 x 150 mm) and with a thickness of 15 mm. Experimental identification of the thermal parameters was performed under laboratory conditions with an air temperature of 20°C, an atmospheric pressure of 101.3 kPa and a relative air humidity of 42.5%. The relative moisture content ωrel of the measured samples was calculated as the ratio of the water mass to the mass of the dry sample multiplied by 100% (Glass and Zelinka, 2010). The gravimetric method was used to determine the moisture content. The mass of the wood samples was measured during the drying process using analytical laboratory scales Kern ADB (Kern, Germany) with an accuracy of 0.0001 g. A laboratory oven SLW 32 STD (Intertec Ltd., Germany) with an accuracy of 0.1°C was used for sample drying. The samples were dried with air that had a temperature of 103±2°C. A moisture analyser, MAC 210/WH (Radwag LLC, USA) was also used to compare the detected results. The thermal parameters were measured using thermal analyser Isomet 2104 (Applied Precision Ltd., Slovakia) and a surface probe with a measuring range of 0.04-0.3 W m K. The measurement procedure is based on the DPS method described by Malinarič and Dieška (2009). A mathematical description was presented in detail by Wakeham et al. (1991) and Liang (1995). RESULTS AND DISCUSSION In the first series of measurements the values of thermal conductivity, thermal diffusivity and volume specific heat in the tangential direction were determined. In the second series, the same samples were examined in the radial direction. Each point in the graphical dependencies shown in Figs 1-4 represents the arithmetic average from twenty measurements. All of the experimental results were statistically processed. The calculated relative probable errors were in the range of 0.115-0.365%. Based on the regression analysis results, the regression equations describing the relationship between the measured thermophysical parameters and the relative moisture content were identified. Thermal conductivity as a function of relative moisture content for samples of softwood, medium hardwood, and hardwood with tangential and radial direction of wood fibres can generally be described by the linear function of Eq. (1) with regression coefficients being presented in Table 1.","PeriodicalId":13959,"journal":{"name":"International Agrophysics","volume":" ","pages":""},"PeriodicalIF":2.0000,"publicationDate":"2021-11-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"8","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Agrophysics","FirstCategoryId":"97","ListUrlMain":"https://doi.org/10.31545/intagr/142472","RegionNum":4,"RegionCategory":"农林科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"AGRONOMY","Score":null,"Total":0}
引用次数: 8

Abstract

During the processing of wood for wood-based products mechanical and thermal stresses often occur. The temperature changes affect the level of wood moisture because heat transport cannot be separated from water transport. The mechanism of conduction is the dominant process of heat transfer through wood and wood-based products, but convection and radiation are also included, mainly in the form of boundary conditions. Heat conduction takes place when a temperature gradient exists in a solid medium. It may be described by Fourier ́s Law (Gustafsson, 1991; Sobota, 2014), where λ is the thermal conductivity (W m K). The conduction of heat involves the transfer of energy within a material without any motion of the material as a whole. The velocity of the temperature equalization in a material during non-stationary processes characterizes thermal diffusivity a (m s) which has been defined in the literature (Suleiman et al., 1999; Adl-Zarrabi, 2004). The volume specific heat cρ (J m K) may be expressed as ratio thermal conductivity λ and thermal diffusivity a (Bouguerra et al., 2001; Nakaya et al., 2016). The thermal parameters of wood and wood-based products are affected by many internal and external factors such as: moisture content (Troppova et al., 2014; Glass and Zelinka, 2010), temperature (Zhou et al., 2013), density of the wood, direction of heat flow with respect to the grain (Ružiak et al., 2017; Öner et al., © 2021 Institute of Agrophysics, Polish Academy of Sciences M. BOŽIKOVÁ et al. 252 2009). The thermal properties of wood-based materials are required in applications such as fuel conversion, building construction and other fields of industry (Zi-Tao et al., 2011). The problem of thermal parameter measurements of wood-based panels has already been discussed in a previous study and new results of the property have been delivered by Sonderegger and Niemz (2012), Li et al. (2013). Steadystate methods are used for the detection of wood thermal parameters (Hrčka and Kurjatko, 2006). Transient methods were introduced by Adl-Zarrabi and Boström (2004), Tavman (1996). Avramidis and Lau (1992) which measured the thermal coefficients of wood particles using a transient heat-flow method. The TPS technique is described in detail by Gustafsson (1991) and Wechsler (1992). According Karawacki et al. (1992) the extended dynamic plane source (EDPS) method is convenient for low thermal conductivity materials (Beck and Arnold, 2003; Malinarič, 2004). It was applied to the detection of the thermophysical properties of the solid wood of coniferous trees by authors Krišťák et al. (2019). Knowledge of the thermal properties of wood is essential for determining of its future usage. Based on the presented facts, the main aim of this research was the identification of the selected thermal properties for different types of woods and wood composites made from wood waste in Slovakia using the dynamic plane source (DPS) method. The main benefit of the research were to establish the relationships between the thermal parameters for the different moisture contents of wood and wood composites – oriented strand board (OSB) detected in the tangential and radial direction. MATERIALS AND METHODS The thermal conductivity, thermal diffusivity and the volume specific heat of the wood and the products made in Slovakia were investigated. Measurements were performed on five types of wood samples: softwood – spruce (Picea abies) and black pine (Pinus nigra), hardwood – beech (Fagus silvatic) and oak (Quercus robur) and also on medium hardwood – chestnut (Aesculus hippocastanum). The relative moisture contents of the measured wood samples fell within the following range – 0-35%. The wood samples were prepared in two directions. The tangential direction is perpendicular to the grain but tangent to the growth rings and the radial direction is normal to the growth rings and perpendicular to the grain in the radial direction. For every wood type special OSB samples were taken with tangential and radial directions. For the purpose of taking OSB thermal parameter measurements, samples from of wood-waste were prepared with the majority content of the wood species having a moisture content in the range 22-26% and the final product – samples of the examined OSB had a relative moisture content ranging from 4 to 7%. The dimensions of all of the measured samples were the same (150 x 150 mm) and with a thickness of 15 mm. Experimental identification of the thermal parameters was performed under laboratory conditions with an air temperature of 20°C, an atmospheric pressure of 101.3 kPa and a relative air humidity of 42.5%. The relative moisture content ωrel of the measured samples was calculated as the ratio of the water mass to the mass of the dry sample multiplied by 100% (Glass and Zelinka, 2010). The gravimetric method was used to determine the moisture content. The mass of the wood samples was measured during the drying process using analytical laboratory scales Kern ADB (Kern, Germany) with an accuracy of 0.0001 g. A laboratory oven SLW 32 STD (Intertec Ltd., Germany) with an accuracy of 0.1°C was used for sample drying. The samples were dried with air that had a temperature of 103±2°C. A moisture analyser, MAC 210/WH (Radwag LLC, USA) was also used to compare the detected results. The thermal parameters were measured using thermal analyser Isomet 2104 (Applied Precision Ltd., Slovakia) and a surface probe with a measuring range of 0.04-0.3 W m K. The measurement procedure is based on the DPS method described by Malinarič and Dieška (2009). A mathematical description was presented in detail by Wakeham et al. (1991) and Liang (1995). RESULTS AND DISCUSSION In the first series of measurements the values of thermal conductivity, thermal diffusivity and volume specific heat in the tangential direction were determined. In the second series, the same samples were examined in the radial direction. Each point in the graphical dependencies shown in Figs 1-4 represents the arithmetic average from twenty measurements. All of the experimental results were statistically processed. The calculated relative probable errors were in the range of 0.115-0.365%. Based on the regression analysis results, the regression equations describing the relationship between the measured thermophysical parameters and the relative moisture content were identified. Thermal conductivity as a function of relative moisture content for samples of softwood, medium hardwood, and hardwood with tangential and radial direction of wood fibres can generally be described by the linear function of Eq. (1) with regression coefficients being presented in Table 1.
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木材和由木材废料制成的木材复合材料的热性能
在干燥过程中,使用分析实验室天平Kern ADB(德国Kern)测量木材样品的质量,精度为0.0001g。使用SLW 32 STD(德国Intertec有限公司)实验室烘箱进行样品干燥,精度为0.1°C。用温度为103±2°C的空气干燥样品。湿度分析仪MAC 210/WH(Radwag LLC,USA)也用于比较检测结果。使用热分析仪Isomet 2104(Applied Precision有限公司,斯洛伐克)和测量范围为0.04-0.3 W m K的表面探针测量热参数。测量程序基于Malinarič和Dieška(2009)描述的DPS方法。Wakeham等人(1991)和Liang(1995)详细介绍了数学描述。结果与讨论在第一系列测量中,确定了切向上的热导率、热扩散率和体积比热的值。在第二个系列中,在径向方向上对相同的样品进行了检查。图1-4所示图形相关性中的每个点表示二十次测量的算术平均值。对所有实验结果进行了统计处理。计算的相对可能误差在0.115-0.365%之间。基于回归分析结果,确定了描述测量的热物理参数与相对含水量之间关系的回归方程。软木、中等硬木和具有木纤维切向和径向的硬木样品的热导率作为相对含水量的函数,通常可以通过方程的线性函数来描述。(1)回归系数如表1所示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
International Agrophysics
International Agrophysics 农林科学-农艺学
CiteScore
3.60
自引率
9.10%
发文量
27
审稿时长
3 months
期刊介绍: The journal is focused on the soil-plant-atmosphere system. The journal publishes original research and review papers on any subject regarding soil, plant and atmosphere and the interface in between. Manuscripts on postharvest processing and quality of crops are also welcomed. Particularly the journal is focused on the following areas: implications of agricultural land use, soil management and climate change on production of biomass and renewable energy, soil structure, cycling of carbon, water, heat and nutrients, biota, greenhouse gases and environment, soil-plant-atmosphere continuum and ways of its regulation to increase efficiency of water, energy and chemicals in agriculture, postharvest management and processing of agricultural and horticultural products in relation to food quality and safety, mathematical modeling of physical processes affecting environment quality, plant production and postharvest processing, advances in sensors and communication devices to measure and collect information about physical conditions in agricultural and natural environments. Papers accepted in the International Agrophysics should reveal substantial novelty and include thoughtful physical, biological and chemical interpretation and accurate description of the methods used. All manuscripts are initially checked on topic suitability and linguistic quality.
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