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Anais da Academia Brasileira de Ciências

Print version ISSN 0001-3765

An. Acad. Bras. Ciênc. vol.82 no.3 Rio de Janeiro Sept. 2010

http://dx.doi.org/10.1590/S0001-37652010000300025 

AGRARIAN SCIENCES

 

Use of glass transition temperature for stabilization of board's cracks of Eucalyptus grandis

 

 

Fred W. CalonegoI; Elias T.D. SeveroI; Antonio R. CunhaII; Daiane C. GaiaI

IFaculdade de Ciências Agronômicas, UNESP, Departamento de Recursos Naturais/Ciências Florestais Fazenda Experimental Lageado, Caixa Postal 237, 18610-307 Botucatu, SP, Brasil
IIFaculdade de Ciências Agronômicas, UNESP, Depto de Recursos Naturais/Ciências Ambientais Fazenda Experimental Lageado, Caixa Postal 237, 18610-307 Botucatu, SP, Brasil

Correspondence to

 

 


ABSTRACT

The Eucalyptus grandis logs temperatures were determined and correlated with the board's cracks during steaming. Thermocouples were inserted in the logs center, registering their temperatures during steaming at 90"C. The logs were sawed and the board's cracks measured. It was concluded that: (1) the logistic S-shaped curve explains the logs temperature variation; (2) the logs with diameter of 20 to <25, 25 to <30 and 30 to <35 cm presented, respectively, 84.2"C, 73.1"C and 45.8"C in the steaming; and (3) the cracks lengths significantly decreased in logs that reached the glass transition temperature.

Key words: board's cracks, Eucalyptus grandis, glass transition temperature, logs steaming.


RESUMO

As temperaturas em toras de Eucalyptus grandis, durante a vaporização, foram determinadas e correlacionadas com as rachaduras das tábuas. Nos centros das toras foram inseridos termopares e registradas suas temperaturas durante a vaporização à 90"C. As toras foram desdobradas e as rachaduras das tábuas mensuradas. Concluiu-se que: (1) o modelo estatístico sigmoidal logístico explica a variação da temperatura nas toras; (2) as toras com 20 a <25, 25 a <30 e 30 a <35 cm de diâmetro apresentaram, respectivamente, 84,2"C, 73,1"C e 45,8"C ao final da vaporização; e (3) as rachaduras foramsignificativamente menores nas toras que atingiram a temperatura de transição vítrea.

Palavras-chave: rachaduras de tábua, Eucalyptus grandis,temperatura de transição vítrea, vaporização de toras.


 

 

INTRODUCTION

Growth stresses that occur in Eucalypts wood are responsible for many defects during all the phases of wood processing and imply in yield loss. This characteristic provides problems in sawing process, drying defects and veneer split (McKenzie et al. 2003).

The origin of the growth stress is directly related to the cell walls lignifications, which are responsible for the cell walls transversal swell and cause length reduction. This reduction is avoided by the older wood cells, causing traction longitudinal stress in the stem periphery and compressing the central part (Boyd 1972, Chafe 1979, Sales 1986, Touza 2001).

One of the efficient techniques used to relief the growth stress is heating logs in water or saturated steam (Calonego and Severo 2005, Severo and Tomaselli2000, Skolmen 1967, Tejada et al. 1997). The aim of these treatments is to soften the wood in order to liberate the growth stresses (Forest Products Laboratory 1999).

Studies show 50% of reductions in the growth stress of Eucalyptus saligna logs after 24 hours of treatment in hot water (Skolmen 1967), significant reductions of 44% and 53% for the cracks length and width of Eucalyptus dunnii after steaming during 20 hours (Severo and Tomaselli 2000), and reductions of about 34% and 48% in the cracks length and width of Eucalyptusgrandis logs after 24 hours of steaming at 90C (Calonego and Severo 2005).

In the evaluation of the steaming effects on drying defects of Eucalyptus grandis by submitting logs at a temperature of 90C during 20 hours, it's concluded that the cracks index reduction was 18.4%, 27.7% and 43.4%, respectively, for logs with 30 to 35, 25 to 30 and 20 to 25 cm of diameter (Calonego and Severo 2006). According to the authors, logs with smaller diameters present bigger reduction of defects when compared with the ones with bigger dimensions.

The knowledge on thermal wood properties has a fundamental importance to estimate the logs steaming time (Langrish and Walker 1993).

Charts were developed to determine the heating time considering wood's thermal and physical properties, its anatomical characteristics, as well as the dimensions of the logs and desired temperature inside them, and heating bath temperature (Steinhagen et al. 1980). However, it's noted that the proposed model underestimates the real time that Eucalyptus grandis logs need to reach the desired temperature (Calonego and Severo 2006).

There is a need for specific studies about logs heating time to accurately define steaming time and temperature limits (Severo and Tomaselli 2000, Tejada et al. 1997). Yet, humidity migration and heat transference in wood are critical factors in many industrial processes of wood. But the heat and humidity transport is concerning very complex considering how heterogeneous and porous the material is.

By steaming Fagus sylvatica logs at 60C, it's concluded that the presence of both heartwood and sapwood in a same log does not allow an uniform stream heat in the material (Perré 2004). During the steaming, the sapwood absorbs a bigger moisture content than the heartwood does. The moisture content facilitates theheat flow and, consequently, increases the temperature, which softens the wood and shows the thermal variation differences between the two types of wood (Lenth andHaslett 2003).

The heating in saturated steam results in heating times shorter than the heating environment when filled with dry air. The temperature in the board's center of Pinus resinosa reached 56C after 23 minutes during the steaming at 85C, and reached the same temperature after 47.8 minutes in the environment with 23.7% of relative humidity and 85C. (Simpson and Illman 2004).

Increases in wood temperature and moisture content are useful for physically softening the wood structure (Lenth and Kamke 2001, Romeiro de Aguiar and Perré 2005). In simple terms, the wood cell wall is a composite made of a rigid cellulose polymer in a matrix of lignin and hemicelluloses. The lignin polymer in the middle lamella and S2 layer are thermoplastic; that is, it softens upon heating (Forest Products Laboratory 1999).

Concerning heating, it is desirable to create anenvironment where the amorphous polymers of woodreach its glass transition temperatures and are softened, which allows internal tensions relieves by the molecular and microstructural re-organization of wood (Lenth and Haslett 2003, Nakano 2005, Romeiro de Aguiar and Perré 2005).

In saturated and heated woods there is an increase of their ductibility due to their amorphous components of viscoelastic properties (lignin and hemicelluloses), which are responsible for wood softening and its relief from growth stress levels (Calonego and Severo 2005, Forest Products Laboratory 1999, McKenzie et al. 2003).

Many authors have reported the glass transition of wood and its chemicals components under various conditions. The glass transition temperatures of the chemical components of wood differ. The softening points of about 80C and 100C are attributed to hemicelluloses and lignin, respectively (Hillis and Rozsa 1985). The glass transition temperature of the lignin is about170C (Forest Products Laboratory 1999). The glasstransition temperature is 40C for hemicelluloses, 50C to 100C for lignin, above 100C for cellulose (Furuta et al. 1997), and around 60C to 70C for wood lignin (Kelley et al. 1987).

The glass transition temperature of wood is the same as the lignin, which is found to be between 60C and 200C, and the decrease of the moisture content of wood increases the glass transition temperature (Lenth and Kamke 2001). In general, for green wood lignin, the glass transition is around 60C (Nakano 2006).

For Couratari guianensis wood, with its moisture content above the fiber saturation point, the glass transition temperature is around 95C (Romeiro de Aguiar and Perré 2005). For Eucalyptus grandis wood, with the same moisture content, the glass transition temperature is around 82C (Quirino and Vale 2002).

The glass transition range of lignin is used to relief the residual growth stress of trees and the one resulted from the drying process (Romeiro de Aguiar and Perré 2005).

The aim of this work was to determine the temperature variation in the Eucalyptus grandis logs center during steaming, and its correlation with cracks in the sawing process.

 

MATERIALS AND METHODS

MATERIAL COLLECTION

In this study, thirty-year-old Eucalyptus grandis logs from São Paulo Forest Institute, located in Manduri, São Paulo, Brazil, were used.

Five trees were randomly selected within 2.2 ha stand. After felling, the trees were sectioned in thirty three logs with 2.9 m length and classified into three diameter classes (20 to 25; 25 to 30; 30 to 35 cm).

Two grooves were machined at a depth equal to one third of the radius of each log at 10 cm from the cross-cut section of the logs, according to the methodology proposed by some authors (Kubler 1987, Sales 1986).

DENSITY AND MOISTURE CONTENT MEASURE FROM LOGS

It was taken a 5 cm disk between each log to determine the moisture content based on the ovendry mass of the material and its specific gravity by applying the equations 1 and 2. A balance with 0.1 g of accuracy and an oven at were used.

(1)

(2)

where:

LOG'S STEAMING AND TEMPERATURE DETERMINATIONS

Logs with 2.9 m length were steamed during 20 hours at 90C and 100% relative humidity in a dry kiln with 3.0 1.6 1.6 m of internal dimensions.

The dryer kiln has an electric heating system that allows to reach the maximum temperature of 130C, a humidification system by steam, an electric boiler with 30 kgf h of capacity to produce steam, and 8 kgf cm of work pressure.

Each log received 1 (one) thermocouple in its center to allow the monitoring of temperature with accuracy inside the logs during the steaming. For a more detailed explanation, see Figure 1A.

 


 

The "T-type" thermocouples (Cu-Co) were builtby the union of both thermo elements using an electric founder. Subsequently, the thermocouples were submitted to gauging tests in temperatures of 0C and 100C, which represent the points of glazing and boiling water. The values were 0.31C and 97.40C, respectively.

Holes were carried out in the logs to perfectly accommodate the thermocouples. After fitting in the sensors, the holes were sealed with several layers: sawdust, retreat of the own hole; silicone, a resistant material to elevated temperatures and humidity conditions; thermal insulating epoxy resin; and a silicone film, which is resistant to humidity, mechanical shocks and temperature. Each material was applied with an time-out of 24 hours, to correctly dry and fix in the wood.

The temperature range in each log diameter was monitored by the thermocouple coupled to a Campbell Scientific datalogger (Micrologger 21X) during the steaming.

BOARD'S CRACKS ANALYSIS

After the steaming, the logs were sawed in flat saw boards. Initially, the logs were transformed into blocks using a twin bandsaw and, subsequently, sawed in boards with 28 mm thickness. As the logs were classified in diameter groups of 20 to 25 cm, 25 to 30 cm and 30 to 35 cm, boards widths of 14.0 cm, 17.5 cm and 21.0 cm, respectively, were obtained according to the blocks dimensions.

The flat saw boards allows to evaluate the effect of logs temperature on sawing process quality (boards cracks length) as shown by Figure 1B.

The end-cracks average lengths were evaluated and quantified through the sum of lengths of individualcracks on Eucalyptus grandis boards.

 

RESULTS AND DISCUSSION

The temperature behavior at each class of log diameter of E. grandis, with 0.6 g cm of specific gravity and 75% of moisture content, during the steaming at 90C, was evaluated with accuracy.

At each minute of the 20 hours in the thermal treatment, the center logs and steam temperatures were collected according to the methodology presented in this study (see item 2.2.).

Concerning the data tendency (temperature of 11 logs per class versus time), it was applied a non-lineal model regression for each class of log diameter and for the steam temperature, as shown by Figures 2, 3 and 4.

 

 

 

 

 

 

For the steam temperature during the thermal treatment, an exponential model was chosen:

where: "", "", "", "" and "" are the model constants; "" the logs steaming time, in hours; and "" the steam temperature, in centigrade grade.

For the three classes of logs diameter, a logistic S-shaped curve was chosen:

where: "", "", "" and "" are the model constants; "" the logs steaming time, in hours; and "" the temperature in the logs center, in centigrade grade.

Figures 2, 3 and 4, respectively, present the adjusted model results to calculate Eucalyptus grandis logs center temperature with a diameter from 20 to 25, 25 to 30 and 30 to 35 cm during the first 20 hours of steaming with the temperature around 90C. In this case, the determination coefficients (R) were, respectively, 0.9885, 0.9773 and 0.9298.

The regression model proposed for each class of Eucalyptus grandis logs diameter and its maximumtemperatures achieved after 20 hours of steaming can be seen in Table I.

Through the statistical models application, it's reported that the logs centers of 20 to 25, 25 to 30 and 30 to 35 cm show, respectively, temperatures of 84.2C, 73.1C and 45.8C in the thermal treatment end.

On the applied conditions in the present work, only Eucalyptus grandis logs with diameters from 20 to 25 cm reached the glass transition temperature,which is around 82C (Quirino and Vale 2002), and the glass transition range of lignin must be used to relief the residual growth stress of trees (Romeiro de Aguiar and Perré 2005).

Only logs from 20 to 25cm of diameter reachedthe glass transition temperature because all the threeclasses of log diameters were exposed on steam for 20 hours. The biggest logs hold bigger heartwood thanthe smallest ones. The sapwood has a bigger moisture content than the heartwood has, and the moisturecontent facilitates the heat flow and, consequently, increases the wood temperature and softening (Lenth and Haslett 2003).

Table II shows that logs from 20 to 25 cm of diameter presented a better growth stress relief, showed by the cracks lengths in the central (29.3 cm) and peripheral boards (37.3 cm), and considered statistically equal. This result was expected; thus, the wood internal stress relieve is directly related to the material being softened(Forest Products Laboratory 1999, Romeiro de Aguiar and Perré 2005). This is characterized by lignin glass transition temperature (Lenth and Kamke 2001, Nakano 2005, Romeiro de Aguiar and Perré 2005), which is found between 50C and 100C (Furuta et al. 1997).

 

 

The logs with diameters from 30 to 35 cm presented cracks lengths statistically different in peripheral and central boards, and it was concomitant with the diameter class in which the logs did not reach the necessary temperature to cause the molecular and microstructural re-organization of wood. This is responsible for the internal tensions relief, according to the same authors (Lenth and Haslett 2003, Lenth and Kamke 2001, Nakano 2005, Romeiro de Aguiar and Perré 2005).

Concerning wood quality, Table II shows that there is a straight relationship between the boards crackslength and the steamed logs diameter. Similar results were obtained by another author (Calonego and Severo 2004) by studying the steaming effects on drying defects in Eucalyptus grandis logs, they concluded that the cracks reduction was 18.4%, 27.7% and 43.4%, respectively, for boards with diameters from 30 to 35, 25 to 30 and 20 to 25 cm. This study also showed that logs with smaller diameters presented minors defects when compared with logs of bigger dimensionsthat were steamed in the same conditions.

Reporting the logs temperatures of Eucalyptusgrandis during 20 hours of steaming at 90C led usto the following conclusions: (1) the logistic S-shaped curve is applicable to explain the temperature variation in the logs center; (2) the cracks lengths were significantly decreased in logs that reached the glass transition temperature.

These results could allow the use of steaming optimum time and avoid wasting energy. The models are appropriate for the studied conditions (temperature, time and procedures). However, data simulations may increase the charts range in future studies.

 

ACKNOWLEDGMENTS

The authors thank the Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP), Brazil, for financialsupport to conduct this research work throughgrants 02/05028-6 and 00/02165-7.

 

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Correspondence to:
Fred Willians Calonego
E-mail: fwcalonego@fca.unesp.br

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