Helene Unterwieser 
email: helene.unterwieser@tugraz.atuniv.-prof.
  
Gerhard Schickhofer 
email: gerhard.schickhofer@tugraz.at
  
Di H Unterwieser 
  
Dr G Di 
  
Schickhofer 
  
Influence of moisture content of wood on sound velocity and dynamic MOE of natural frequency-and ultrasonic runtime measurement Einfluss der Holzfeuchte auf die Schallgeschwindigkeiten und den dynamischen E-Modul aus Eigenschwingungs-und Ultraschalllaufzeitmessung

Keywords: Diese Arbeit befasst sich mit der Untersuchung des Einflusses der Holzfeuchte auf die dynamischen Eigenschaften -Schallgeschwindigkeit und dynamischer E-Modul (Berücksichtigung der Rohdichte) -von Schnittholz, mit dem Ziel, für die genannten Eigenschaften durch geeignete überprüfen, ob die zur Thematik bereits publizierten Feuchtekorrekturen, die meist auf Daten aus einer Ultraschalllaufzeitmessung basieren, auch auf die Daten aus Eigenschwingungsmessungen anwendbar sind

This study comprises the analysis of the influence of the moisture content of wood on the dynamic properties -sound velocity and dynamic MOE (considering the density) -of green and dry sawn timber. The main objective was to find applicable functions or factors for the adjustment of the determined properties on the reference condition (moisture content u=12 %) for the moisture content range below and above fiber saturation. Therefore, two dynamic measurement methodsmeasurement of the natural frequency and ultrasonic runtime -were considered. Possible differences in the results, pros and cons of both methods should be identified on the one hand. On the other hand, the applicability of already published moisture adjustments to the given data of both methods should be proved.

Introduction

The determination of dynamic properties -sound velocity v and dynamic modulus of elasticity( MOE) (with consideration of the density) -are significant methods in order to derive mechanical properties of wood like modulus of elasticity and strength. Two procedures are used for the grading of timber, the measurement of the natural frequency and the measurement of the ultrasonic runtime, which differ in the type of vibration -forced or free. In both measurement methods, the sound velocity is dependent on the moisture content u of the sawn wood.

For the ultrasonic runtime measurement, some research has already been performed and corresponding moisture corrections for different wood moisture levels (below and above fiber saturation (FSP)) were published, see [START_REF] Sandoz | Triage et fiabilité des bois de construction -Validité de la méthode ultrason Grading and reliability of timber -Validity of the ultrasonic method (only available in French)[END_REF], [START_REF] Sandoz | Triage et fiabilité des bois de construction -Validité de la méthode ultrason Grading and reliability of timber -Validity of the ultrasonic method (only available in French)[END_REF] and [START_REF] Steiger | Versuche an Fichten-Kanthölzern: Biegemoment-Normalkraft-Interaktion[END_REF]. For example, in [START_REF] Steiger | Versuche an Fichten-Kanthölzern: Biegemoment-Normalkraft-Interaktion[END_REF] the moisture corrections of ultrasonic wave speed for three wood moisture ranges are given as follows: These adjustment functions are based on an investigation by [START_REF] Sandoz | Triage et fiabilité des bois de construction -Validité de la méthode ultrason Grading and reliability of timber -Validity of the ultrasonic method (only available in French)[END_REF] and are also implemented in a modified form in Sylvatest, a device for ultrasonic runtime measurement. The second publication [START_REF] Sandoz | Triage et fiabilité des bois de construction -Validité de la méthode ultrason Grading and reliability of timber -Validity of the ultrasonic method (only available in French)[END_REF] defines two linear functions for the moisture adjustment of the ultrasonic wave speed. They are valid for a moisture content u below and above the threshold value of 32 %. For the moisture content adjustment of the stress-wave speed from natural frequency measurements no publications are known, probably under the assumption that both methods differ only slightly.

The second input parameter for the calculation of the dynamic modulus of elasticity -the density -is influenced by the moisture content of wood as well, especially above fiber saturation. No adequate correction function for density was available when the data of the present investigation was analysed. In the moisture content range below fiber saturation , ON EN 384 (2004) describes a moisture adjustment factor for the range between u = 10 and 18 %. It states a valid change in density of 0.5 % for 1 % change of moisture content. This work comprehends the results of the investigation on the dependence on the parameters density, sound velocity of ultrasonic runtime and natural frequency measurements and the resulting dynamic moduli of elasticity on the moisture content of wood. The objective was the determination of appropriate moisture adjustment functions to compare the mechanical and dynamic properties, determined at a wood moisture u, to the reference moisture of u = 12 %.

Material, methods and procedure

Samples

The investigation was carried out with 310 ungraded spruce boards with a length of 4500 mm and different widths (202 mm and 98 mm) and thicknesses (49 mm and 41 mm), which were supplied in green condition (freshly cut), see also Table 1. The decrease of the cross section by shrinkage during the drying process was considered. 

Methods

Two methods were applied to determine the dynamic properties. Natural frequency was measured with an industrially applied device (ViSCAN). The oscillation excitation was achieved by a steel ball, which was mounted on an air cylinder with a spring. The arising free longitudinal oscillation was measured contactless with a laser vibrometer. The first natural frequency f [Hz] -for calculation of the stress-wave speed -was determined by FFT analysis. The ultrasonic runtime -for calculation of the ultrasonic wave speed -was measured with a laboratory device (Sylvatest) and based on the determination of the run time t [μs] of the ultrasonic wave between transmitter and receiver, which is generated by piezoelectric transducers with a frequency of about 30 kHz.

Procedure

The first recording of cross-sectional dimensions and mass was carried out shortly after delivery of the green boards. Small defect free specimens were cut out for the determination of moisture content in green condition. After measuring the natural frequencies and ultrasonic runtimes, the boards were stored in a stack in a closed building at temperatures between 21°C and 24°C and a relative humidity of about 58 %. Therefore, gentle drying of the boards could be guaranteed in order to reach moisture contents far below the fiber saturation point.

Five measurements were taken in the course of the drying process. Before the final measurement, all boards were kiln-dried within 10 days to reach the reference moisture content of u = 12 %. A second specimen was taken from each board after final measurement of the dynamic properties for re-calculating the moisture content for each measurement period with the given mass differences.

The analysis included the evaluation of the influence of moisture content on density, natural frequency and ultrasonic runtime, the resulting determined sound velocities (ultrasonic wave speed, stress-wave speed) and the associated dynamic moduli of elasticity.

Results

Density, sound velocity and dynamic moduli of elasticity at different moisture contents

Table 2 shows the results of the measurements 1-5 of density, sound velocity and the resulting dynamic moduli of elasticity at different moisture contents.

For measurements 1 to 4, the mean moisture content lies above fiber saturation with individual values ranging from 15 % and 170 %. Because of kiln-drying after measurement 4, a mean reference moisture content of u = 12 % could be reached.

Apart from the continuous decrease in moisture content and thus density, an increase in sound velocity could be measured. In contrast to this fact, the mean dynamic moduli of elasticity remained nearly constant during the measurement periods 1 to 4. A significant increase of the mean values was observed at measurement 5, with a reference moisture content of about 12 %. Influence of the moisture content on the density A significant change in the behaviour of the properties (moisture content to ratio of ρ u /ρ 12 ) was identified around the fiber saturation point. Linear functions can be applied for both moisture content ranges (Eq. 6 and Eq. 7). The threshold value for the moisture content of u = 28 % was determined with a regression analysis.

) 12 ( 0042 . 0 1 , 12 - ⋅ + = ≤ u u FSP u ρ ρ (6) ) 28 ( 0082 . 0 0672 . 1 , 12 - ⋅ - = > u u FSP u ρ ρ (7)
The determined adjustment function for the moisture range below FSP corresponds well with the given moisture adjustment in ON EN 384 (2004), which is applicable for moisture contents between 10 % and 18 %. The comparison of the adjusted density and the density determined at reference conditions (u = 12 %) shows maximum relative deviations of about 5 % (see Table 3). The trends in Fig. 2 lead to the conclusion that a moisture content adjustment of the sound velocity has to be carried out separately for the moisture content ranges below and above fiber saturation. For correct data separation, the threshold moisture content has to be found, where the dependence of the dynamic parameters changes. By means of a regression analysis the threshold moisture contents could be identified: 32 % for the method of natural frequency measurement and 28 % for the method of ultrasonic runtime measurement.

Note: The statistical analysis clearly shows the moisture content threshold values 28 % and 32 %, though the FSP is between 30 % and 34 % according to Niemz (1993). The reason for the different results of the two dynamic measurement methods has not been fully identified yet.

Adjustment of sound velocity below FSP

Linear functions with nearly the same slope k could be determined for both measurement methods. The adjustment method by [START_REF] Steiger | Versuche an Fichten-Kanthölzern: Biegemoment-Normalkraft-Interaktion[END_REF] shows a bi-linear course, separated into two moisture content ranges. Thus, the adjustment function or the constant factor can not be applied to the data of the present investigation. The given data do not show an additional change in the relations between moisture content and sound velocity above FSP on the one hand and exhibit a steeper trend on the other hand.

) 12 ( 0062 . 0 1 , 12 , - ⋅ - = ≤ u v v u FSP u EF (8)
The comparison between adjusted and sound velocity values determined at reference conditions shows a very good adjustment. On the contrary, the significant underestimation by applying the moisture content adjustment proposed by [START_REF] Steiger | Versuche an Fichten-Kanthölzern: Biegemoment-Normalkraft-Interaktion[END_REF] and [START_REF] Sandoz | Triage et fiabilité des bois de construction -Validité de la méthode ultrason Grading and reliability of timber -Validity of the ultrasonic method (only available in French)[END_REF] is shown. In Table 5, Fig. 5 and Fig. 6 the correlation between adjusted and sound velocity determined at reference conditions is given for both measurements . On the one hand, the possibility to adjust the individual properties density and sound velocity (adjustment of both or only one input parameter) exists, on the other hand, it is possible to adjust the dynamic MOE directly by suitable functions or constant factors. These alternatives were applied and compared in this investigation.

Adjustment of dynamic modulus of elasticity below FSP

Direct adjustment of the dynamic MOE

The correlation between moisture content and dynamic MOE of both measurement methods could be fit best by linear trend lines, which have nearly the same slope k. (15) The comparison between adjusted dynamic MOE and MOE determined at reference conditions results in maximum deviations of 7 %. Eq. 15 enables a precise moisture content adjustment of the dynamic MOE on average (see Table 6).

Fig. 8 shows the threshold for the moisture content at u = 28 % and the associated change of (linear) dependence of the dynamic MOE. 

Adjustment of both input parameters

For comparison reasons, the adjusted dynamic MOE is calculated using the adjusted density (Eq. 6), the adjusted sound velocity (Eq. 10) and the moisture content adjustment of Eq. 1.

FSP u FSP u US EF FSP u dyn v E ≤ ≤ ≤ ⋅ = , 12 2 , 12 , , , 12 , ρ (16) FSP u FSP u dyn v E ≤ ≤ ⋅ = , 12 2 12 , 12 , ρ (17)
The maximum deviations between adjusted dynamic MOE according to Eq. 16 and dynamic MOE determined at reference conditions do not exceed 7 %, for moisture content adjustment according to Eq. 17 8 %. The adjustment of both properties with Eq. 16 leads to an underestimation of the mean values of the MOE determined by natural frequency measurement as well as the adjustment by Eq. 17 for the MOE of the ultrasonic runtime measurement, see Table 6.

Adjustment of one input parameter

For comparison reasons, three alternatives -adjustment of sound velocity with Eq. 10 and with Eq. 1 and adjustment of the density with Eq. 6 -were taken into account.

u FSP u US EF FSP u dyn v E ρ ⋅ = ≤ ≤ 2 , 12 , , , 12 , (18) u FSP u dyn v E ρ ⋅ = ≤ 2 12 , 12 , ( 19 
) FSP u u FSP u dyn v E ≤ ≤ ⋅ = , 12 2 , 12 , ρ (20) 
The dynamic MOEs calculated using the adjusted sound velocities are overestimated between 1.5 % and 4.6 % on average. The maximum deviations of adjusted dynamic properties and dynamic MOE determined at reference conditions are 12 %. In contrast, the individual adjustment of the density tends to result in an underestimation of the dynamic MOE between 13 % and 14 % on average (see Table 6).

As expected, the influence of the non-adjusted sound velocities is higher than the influence of the non-adjusted density for the moisture content range below fiber saturation. 

Adjustment of dynamic modulus of elasticity above FSP

Direct adjustment of the dynamic MOE

The correlation between moisture content and dynamic MOE from natural frequency measurements results in a constant adjustment factor. The calculation of the dynamic MOE from ultrasonic runtime measurements results in a linear function (see Fig. 7).

u dyn u dyn FSP u EF dyn E E E , , , 12 , , 15 . 1 868 
. 0 ⋅ ≅ = > (21) ) 28 ( 0017 . 0 868 . 0 , , 12 , , - ⋅ + = > u E E u dyn FSP u US dyn (22)
In contrast to the ultrasonic runtime measurements, which show a positive correlation of the considered properties, no dependence of the dynamic MOE calculated from natural frequency measurements could be determined over the whole moisture content range above fiber saturation (see Fig. 9).

The comparison of the adjusted dynamic MOE from natural frequency measurement with the related dynamic properties determined at reference condition delivers maximum deviations of up to 9 %. The constant factor allows a good moisture adjustment on average. The maximum deviations of the adjusted values for ultrasonic runtime measurements reach 16 % with a resulting overestimation of nearly 2 % in the mean values, see Table 7. 

Adjustment of both input parameters

The adjustment of sound velocity with Eq. 11 and Eq. 12 and density with Eq. 7, respectively,

FSP u FSP u EF FSP u EF dyn v E > > > ⋅ = , 12 2 , 12 , , 12 , , ρ (23) FSP u FSP u US FSP u US dyn v E > > > ⋅ = , 12 2 , 12 , , 12 , , ρ (24) 
delivers maximum deviations of up to 10 % for the dynamic MOE from natural frequency measurement and 14 % for the dynamic MOE from ultrasonic runtime measurement (see Table 7).

Adjustment of one input parameter

Two alternatives -adjustment of sound velocity and adjustment of density -were taken into account. 7). Fig. 10 and Fig. 11 show the correlation between the adjusted dynamic MOEs with various models and the dynamic properties determined at reference conditions for both measurement methods. 

u FSP u EF FSP u EF dyn v E ρ ⋅ = > > 2 , 12 , , 12 , , (25) 
u FSP u US FSP u US dyn v E ρ ⋅ = > > 2 , 12 , , 12 , , (26) 

Conclusion

The present analysis shows, that the input parameters for calculation of the dynamic MOE -density and sound velocity -are substantially influenced by the moisture content of wood. The adjustment of all properties to the reference condition u = 12 % can be carried out by using adjustment functions and constant factors, respectively, whereas a definite threshold moisture content at fiber saturation has to be fixed. Previously published methods for moisture content adjustment of ultrasonic wave speed could be confirmed only in parts by the given data.

All properties, density, sound velocity and dynamic MOE for both measurement methods offer linear dependence on the moisture content below fiber saturation.

The determined linear function for the adjustment of the density confirmed the moisture content adjustment in ON EN 384 (2004). The adjustments of sound velocities and dynamic MOEs could be fixed with average linear functions, which are applicable for both measurement methods. The published moisture adjustments by [START_REF] Steiger | Versuche an Fichten-Kanthölzern: Biegemoment-Normalkraft-Interaktion[END_REF] and [START_REF] Sandoz | Triage et fiabilité des bois de construction -Validité de la méthode ultrason Grading and reliability of timber -Validity of the ultrasonic method (only available in French)[END_REF] could be confirmed for the moisture content range below fiber saturation.

The wood moisture content range above fiber saturation required a different look at the properties of both measurement methods. The adjustment of the ultrasonic wave speed and the resulting dynamic MOE can be accomplished by using linear functions. In contrast, moisture adjustment of the stress-wave speed has to be carried out using a quadratic function, and for the resulting dynamic MOE a constant factor results in the best data fitting. The published adjustment methods for the moisture content range above fiber saturation were only suitable to a limited extent for application on the available data. The best moisture adjustment of density could be achieved by use of a linear function.

The present study shows, that the sound velocities of both measurement methods exhibit a nearly identical behaviour in relation to the influence of moisture content below fiber saturation. Therefore, the influence on both properties can be described by a linear function. The significant change of the influence on both sound velocities above fiber saturation has a massive consequence regarding the resulted dynamic MOEs. While the dynamic MOE of the ultrasonic runtime measurement also delivers a linear dependence of the moisture content, the dynamic MOE based on the stress-wave speed exhibits no moisture content dependency in the whole range above fiber saturation. This fact could be used best in the context of (pre-)grading of green timber for example. The difficult, industrially practicable recording of moisture content above fiber saturation could be omitted because of the moisture independence of the dynamic MOE. This property desired for the grading process at reference condition (u = 12 %) can be determined without knowledge of the moisture content in green condition.

Fig. 1

 1 Fig. 1 shows the relation between moisture content and density below and above fiber saturation.

Fig. 1

 1 Fig. 1 Relation between moisture content and relative density Abb. 1 Zusammenhang zwischen der Holzfeuchte und der relativen Rohdichte

Fig. 2

 2 Fig.2shows the relation between moisture content and sound velocity for both measurement methods. The main differences are found in the trend and the different spread of the data points. An evenly curved data band with a low dispersion in the upper range of moisture content was found for natural frequency measurements. The ultrasonic runtime measurements show a significant change of the data relation in the area of fiber saturation, coupled with a considerably higher dispersion of the data points in the upper range of the moisture content. A linear dependence of the ultrasonic wave speed on the moisture content can be observed over the whole range. The apparent linear dependence of the sound velocity below the fiber saturation point is common for both measurement methods.

Fig. 2

 2 Fig. 2 Relation between moisture content and relative sound velocity of natural frequency and ultrasonic runtime measurement Abb. 2 Zusammenhang zwischen Holzfeuchte und relativen Schallgeschwindigkeiten der Eigenschwingung-und Ultraschalllaufzeitmessung

Fig. 4

 4 Fig. 4 Correlation between moisture content and sound velocity for both measurement methods above FSP: trend lines for adjustment Abb. 4 Schallgeschwindigkeiten beider Messmethoden in Abhängigkeit von der Holzfeuchte über Fasersättigung: Anpassungsfunktionen

Fig. 5

 5 Fig. 5 Correlation between adjusted and at reference condition (u = 12 %) determined stress-wave speed of the natural frequency measurement above FSP Abb. 5 Zusammenhang zwischen den bei der Referenzholzfeuchte (u = 12 %) ermittelten und den korrigierten Schallgeschwindigkeiten aus der Eigenschwingungsmessung für den Bereich über Fasersättigung

Fig. 6

 6 Fig. 6 Correlation between adjusted and at reference condition (u = 12 %) determined ultrasonic wave speed of the ultrasound runtime measurement above FSP Abb. 6 Zusammenhang zwischen den bei der Referenzholzfeuchte (u = 12 %) ermittelten und den korrigierten Schallgeschwindigkeiten aus der Ultraschalllaufzeitmessung für den Bereich über Fasersättigung

Fig. 7

 7 Fig. 7 Relation between moisture content and relative dynamic MOE of natural frequency and ultrasonic runtime measurement Abb. 7 Zusammenhang zwischen der Holzfeuchte und den relativen dynamischen E-Moduln aus der Eigenschwingungs-und Ultraschalllaufzeitmessung

Fig. 8

 8 Fig. 8 Trend lines for the correlation between moisture content and dynamic MOE for both measurement methods below FSP Abb. 8 Anpassungsgeraden für den Zusammenhang zwischen der Holzfeuchte und den dynamischen E-Moduln beider Messmethoden unter Fasersättigung

Fig. 9

 9 Fig. 9 Trend lines for the correlation between moisture content and dynamic MOE for both measurement methods above FSP Abb. 9 Anpassungsgeraden für den Zusammenhang zwischen der Holzfeuchte und den dynamischen E-Moduln beider Messmethoden über Fasersättigung

  MOEs with adjusted sound velocity and non-adjusted density are overestimated by 40 % on average. The maximum deviations reach up to 123 %. The individual adjustment of the density leads to an underestimation of the dynamic MOEs of between approx. 30 % (US) to 35 % (EF) on average (see also Table

  Fig. 10 Correlation between adjusted and at reference conditions (u = 12 %) determined dynamic MOE of the natural frequency measurement above FSP Abb. 10 Zusammenhang zwischen den bei der Referenzholzfeuchte (u = 12 %) ermittelten und den korrigierten dynamischen E-Moduln aus der Eigenschwingungsmessung für den Bereich über Fasersättigung

  Fig. 11 Correlation between adjusted and at reference conditions (u = 12 %) determined dynamic MOE of the ultrasound runtime measurement above FSP Abb. 11 Zusammenhang zwischen den bei Referenzholzfeuchte (u = 12 %) ermittelten und den korrigierten dynamischen E-Moduln aus der Ultraschalllaufzeitmessung für den Bereich über Fasersättigung

  

Table 1

 1 Cross section [mm], sample size and cutting pattern

	Tabelle 1 Querschnittsmaße [mm], Umfang und Einschnitt		
	green condition	dry condition (u = 12 %)	sample	cutting
	w	t	w	t	size	pattern
	202	49	195	47	78	center
	177	47	171	46	78	center
	100	42	95	41	82	side
	98	41	95	40	72	center

Table 2

 2 

		Set of all determined properties (moisture content, density, sound velocity and dynamic
	moduli of elasticity): minimum-, mean-and maximum values and coefficient of variation in % (in
	parenthesis)					
	Tabelle 2 Zusammenfassung der im Verlauf der Messungen ermittelten Kenngrößen der
	Holzfeuchte, Rohdichte, Schallgeschwindigkeiten und dynamischen E-Moduln: Minimal-, Mittel-
	und Maximalwert sowie Variationskoeffzient in % (in Klammer)		
		moisture	density	sound velocity [m/s]	dynamic MOE [N/mm²]
		content [%]	[kg/m³]				
		u		v EF	v US	E dyn,EF	E dyn,US
		29.8	408	3033	3319	5891	7325
	1	65,7 (52.5)	620 (20.4 %)	4165 (12.3 %)	4713 (10.5 %)	10622 (22.7 %)	13747 (23.1 %)
		169	951	5355	5668	17055	22218
		18.8	380	3222	3656	6194	7599
	2	51.9 (58.8 %)	570 (19.8 %)	4371 (12.1 %)	4890 (10.1 %)	10756 (22.1 %)	13557 (22.1 %)
		159	912	5508	5878	17089	21991
		16.7	379	3402	3826	6487	7788
	3	37.7 (64.7 %)	526 (17.7 %)	4607 (11.1 %)	5094 (9.4 %)	11077 (22.1 %)	13603 (20.6 %)
		143	848	5597	5934	17134	21045
		15.0	373	3427	4006	6465	7915

Table 3

 3 Relative deviations of the adjusted density below and above FSP: minimum-, mean-, and

	maximum values in %		
	Tabelle 3 Relative Abweichungen der korrigierten Rohdichten unterhalb und oberhalb
	Fasersättigung: Minimal-, Mittel-, und Maximalwert in %	
		u ≤ 28 %: Eq. 6	u > 28 %; Eq. 7
	ρ 12,u≤/>FSP / ρ 12	-4.5 +0.1	-4.9 +0.3
		+4.6	+4.1

Influence of the moisture content on the sound velocity depending on the measurement method

  

Table 5

 5 Relative deviation of the adjusted sound velocity for both measurement methods above

	FSP: minimum-, mean-and maximum values in %		
	Tabelle 5 Relative Abweichungen der korrigierten Schallgeschwindigkeiten für beide
	Messmethoden über Fasersättigung: Minimal-, Mittel-, und Maximalwert in %	
		Eq. 11 and 12	Eq. 2 and 3	Eq. 5
	EF	-3.6 +0.5	-10.1 -5.4	-29.6 -15.7	-16.1 -6.7
		+6.3	-1.5	-3.2	+1.7
	US	-7.7	-11.6	-24.3	-13.0

Table 6

 6 Relative deviation of the adjusted dynamic MOE for both measurement methods below

	FSP: minimum-, mean-and maximum values in %			
	Tabelle 6 Relative Abweichungen der korrigierten dynamischen E-Moduln aus beiden	
	Messmethoden unter Fasersättigung: Minimal-, Mittel-, und Maximalwert in %	
	direct	v 12 , ρ 12		v 12 , ρ u and v u , ρ u	
	Eq. 15	Eq. 16	Eq. 17	Eq. 18	Eq. 19	Eq. 20

Table 7

 7 Relative deviation of the adjusted dynamic MOE for both measurement methods above FSP: minimum-, mean-and maximum values in %

	Tabelle 7 Relative Abweichungen der korrigierten dynamischen E-Moduln aus beiden
	Messmethoden über Fasersättigung: Minimal-, Mittel-, und Maximalwert in %	
		direct	v 12 , ρ 12	v 12 , ρ u and v u , ρ u
		Eq. 21 and 22	Eq. 23 and 24	Eq. 25 and 26	Eq. 27
	EF	-8.9 +1.1	-7.7 +0.8	+5.5 +39.8	+39.8 -63.5
		+9.2	+9.7	+105.4	-14.1
	US	-11.5 +2.1	-14.1 +0.2	+2.9 +39.2	-53.9 -29.8
		+16.4	+12.2	+122.5	-11.5

Considering the ratios of the adjusted sound velocity and the dynamic properties determined at reference conditions (u = 12 %), maximum deviations of about 5 % can be observed (see also Table 4). The dashed line represents the moisture content adjustment according to [START_REF] Steiger | Versuche an Fichten-Kanthölzern: Biegemoment-Normalkraft-Interaktion[END_REF] and shows a lower slope k of the straight trend line. Thus, the sound velocity is slightly underestimated by this adjustment (see Table 4). This is valid for the linear function proposed by [START_REF] Sandoz | Triage et fiabilité des bois de construction -Validité de la méthode ultrason Grading and reliability of timber -Validity of the ultrasonic method (only available in French)[END_REF] as well. 

Adjustment of sound velocity above FSP

A quadratic function for the natural frequency measurement and a linear adjustment function for the ultrasonic runtime measurement were determined to describe the correlation between moisture content and sound velocity above fiber saturation.