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Proceedings e report - Firenze University Press

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IN THE HEART OF THE LIMBA TREE: DETECTION METHODS FOR HEART ROT AND FALSE HEARTWOOD<br />

below the measuring point. Notes on the health status of trees were written down. The general study<br />

took place on 87 trees in the plantation. None of them showed signs of limba noir. Next to limba trees,<br />

other tree species were analysed with the acoustic method to investigate the influence of density and<br />

diameter (n = 10 trees per species).<br />

The detailed study is reconstructing the inside of the tree, providing two-dimensional visualisations.<br />

This more intensive case study was performed on freshly cut stem disks, where disk surface and<br />

detection measurements could be compared. In total, 8 disks from 5 trees were analysed.<br />

2.3. Detection methods<br />

Both detection methods are standard methods for the detection of cavities and wood anomalies.<br />

However, these two methods are not often used on tropical tree species.<br />

All resistance measurements were performed with a resistograph of the type IML-Resi B400. This<br />

instrument has a needle that penetrates the wood and has a precision of 0.04 mm. Sound wood has a<br />

higher resistance than infected wood. The measurement is semi-destructive, leaving only a small<br />

channel where the needle passed. The result is a resistance profile from the outside of the tree (without<br />

bark for the general study, with bark for the detailed study) to the pith.<br />

A cheaper method consists of the determination of the velocity of sound within stems. Two sensors<br />

were placed upon the tree on opposite sides. With a small hammer, one of the sensors was hit,<br />

transmitting a sound pulse to the opposite sensor. The result has a precision of 1 μs. Every travel time<br />

is the result of five repetitions that were recorded with the Fakopp Microsecond Timer. This<br />

measuring device only leaves two small holes in the tree where the sensors were placed and is less<br />

destructive than the resistograph. When the distance between the two ends of the sensors is measured<br />

with a calliper (precision of 0.5 cm), the velocity can be calculated. The result is one velocity value<br />

per measurement.<br />

2.4. Data analysis<br />

Comparing one velocity value with a complete resistance profile is complicated. After the first trials, a<br />

transformation of the resistance profiles into variables that are comparable with velocity values, took<br />

place. These variables are all values instead of profiles which makes comparison easier. Every<br />

resistance curve shows a similar pattern (Fig. 1): an increasing trend as the needle enters the stem<br />

(zone A) followed by a more stable trend within the main stem (zone B). Using a double linear<br />

regression, we converted the resistance profiles into point values: the breakpoint or C (distance from<br />

the start of the profile to the intersection of the two linear regressions with the best cumulated<br />

determination coefficient, R²), the slope of the first (zone A) and second linear regression (zone B), the<br />

maximum, minimum and range of resistance values after the breakpoint (within zone B, zone A is not<br />

taken into account since resistance values are still in the transition stage after entering the stem). All<br />

these values were compared with velocity and diameter values with special attention for the outliers of<br />

velocity (wood anomalies!).<br />

Fig. 1 – Example of the transformation of resistance profiles to point values.<br />

The result is a breakpoint at point 407, corresponding with a distance of 16.28 mm.<br />

During the detailed study, interpolation of the resistance profiles in order to visualize the internal<br />

distribution of resistances is based on the principle of inverse distance weighing. For every unknown<br />

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