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Allometry and evaluation of in situ optical LAI ... - Tree Physiology

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determ<strong>in</strong>es shoot clump<strong>in</strong>g as the ratio <strong>of</strong> the projected area <strong>of</strong><br />

the needles with<strong>in</strong> the shoot to the vertically projected shoot<br />

area. This technique was further developed by Fassnacht et al.<br />

(1994) <strong>and</strong> corrected by Chen (1996) to <strong>in</strong>clude a greater number<br />

<strong>of</strong> shoot projections for the calculation <strong>of</strong> needle-to-shootarea<br />

ratio, γe. The shoot area is <strong>in</strong>terpreted as the imag<strong>in</strong>ary surface<br />

area <strong>of</strong> a sphere envelop<strong>in</strong>g the leaf-clump <strong>and</strong> is calculated<br />

as a weighted mean ratio <strong>of</strong> the projected shoot silhouette<br />

area (Ap) for different projection angles. Chen (1996) found<br />

good agreement between results <strong>of</strong> shoot analysis for three projection<br />

(camera <strong>in</strong>cidence) angles <strong>and</strong> shoot analysis for 21 <strong>and</strong><br />

39 projection angles, respectively, <strong>and</strong> thus recommended the<br />

use <strong>of</strong> the method by which each shoot from a calibration sample<br />

is imaged <strong>and</strong> analyzed from three camera <strong>in</strong>cidence angles<br />

to estimate the correction parameter (Chen 1996):<br />

with:<br />

<strong>LAI</strong>c = <strong>LAI</strong>eγ<br />

e<br />

(1)<br />

γ e = An/ As<br />

(2)<br />

A<br />

s<br />

(0 ° , 0 ° )cos (15 ° ) (45 ° ,0 ° )cos (45 ° ) (90 ° , 0 ° )cos(75 ° )<br />

A p + A p + A p<br />

= 2<br />

cos(15 ° ) + cos(45 ° ) + cos(75 ° )<br />

where <strong>LAI</strong> c is <strong>LAI</strong> corrected for shoot-level clump<strong>in</strong>g, <strong>LAI</strong> e is<br />

effective <strong>LAI</strong> as estimated by the <strong>optical</strong> devices, γe is the ratio<br />

<strong>of</strong> needle-to-shoot area, An is half the total needle area for all<br />

the needles <strong>of</strong> a shoot, As is half the total shoot imag<strong>in</strong>ary surface<br />

area, <strong>and</strong> Ap (θ, φ) is the projected area for given angles <strong>of</strong><br />

θ <strong>and</strong> φ, where θ <strong>and</strong> φ are the azimuth <strong>and</strong> zenith projection<br />

angles <strong>in</strong> relation to the ma<strong>in</strong> axis <strong>of</strong> the shoot, respectively.<br />

Ten <strong>in</strong>tact shoot samples were taken from each model tree<br />

<strong>and</strong> different model branches to obta<strong>in</strong> the with<strong>in</strong>-shoot clump<strong>in</strong>g<br />

factor. Half the total needle area <strong>in</strong> the shoot (An) was<br />

measured as the projected area <strong>of</strong> needles multiplied by a correction<br />

factor dependent on the hemi-cyl<strong>in</strong>drical shape <strong>of</strong> the<br />

needles. Projected area for the needles <strong>of</strong> the shoots was determ<strong>in</strong>ed<br />

with a Li-Cor planimeter, <strong>and</strong> the correction factor <strong>of</strong><br />

1+π/2 (Bond-Lamberty et al. 2003) was applied. The imag<strong>in</strong>ary<br />

shoot area was obta<strong>in</strong>ed from the projected shoot area<br />

(Ap) at three view<strong>in</strong>g angles (0, 45 <strong>and</strong> 90°) with a Kodak DCS<br />

660 digital camera. The correspond<strong>in</strong>g images were digitally<br />

analyzed accord<strong>in</strong>g to the methodology developed by Chen<br />

(1996) to assess the shoot silhouette area. Mean γe (= 2.001)<br />

was calculated as the arithmetic mean <strong>of</strong> the shoot samples.<br />

St<strong>and</strong>-level clump<strong>in</strong>g To correct for clump<strong>in</strong>g with<strong>in</strong> a st<strong>and</strong><br />

at all scales greater than the shoot, <strong>in</strong>clud<strong>in</strong>g with<strong>in</strong>-crown<br />

clump<strong>in</strong>g, Ωe was obta<strong>in</strong>ed from TRAC (Leblanc 2002) as:<br />

Ω e<br />

⎛ ( Fm − Fmr)<br />

⎞ lnF<br />

= ⎜1<br />

+ ⎟<br />

⎝ 1−<br />

F ⎠ lnF<br />

m<br />

ALLOMETRY AND EVALUATION OF OPTICAL <strong>LAI</strong> DETERMINATION 727<br />

where Fm is the measured total canopy gap fraction <strong>and</strong> Fmr is<br />

the gap fraction <strong>of</strong> an imag<strong>in</strong>ary canopy with the same <strong>LAI</strong> as<br />

the clumped canopy, but where the foliage elements are considered<br />

spatially r<strong>and</strong>om. We measured Fm with TRAC along<br />

transects <strong>in</strong> the st<strong>and</strong> on October 7, 2002, (see Figure 1 for<br />

m<br />

mr<br />

(3)<br />

(4)<br />

sampl<strong>in</strong>g strategy) as the transmittance <strong>of</strong> direct or diffused radiation<br />

at the zenith angle <strong>of</strong> 57.5°. We derived Fmr from the<br />

measured gap size distribution by a gap removal approach. All<br />

transects were analyzed with the TRACW<strong>in</strong> s<strong>of</strong>tware provided<br />

with the <strong>in</strong>strument. The calculated value for Ωe was 0.836.<br />

We calculated <strong>LAI</strong>B as (Chen <strong>and</strong> Cihlar 1995):<br />

<strong>LAI</strong> = <strong>LAI</strong> / Ω<br />

(5)<br />

B e e<br />

where <strong>LAI</strong> B is <strong>LAI</strong> corrected for branch- <strong>and</strong> tree-level clump<strong>in</strong>g<br />

<strong>and</strong> <strong>LAI</strong> e is the effective <strong>LAI</strong> as estimated by the <strong>optical</strong><br />

devices.<br />

Plant area <strong>in</strong>dex To correct for clump<strong>in</strong>g at the with<strong>in</strong>-shoot<br />

<strong>and</strong> above-shoot levels <strong>and</strong> account for the contribution <strong>of</strong><br />

non-photosynthetic components <strong>of</strong> the canopy <strong>in</strong> the <strong>optical</strong><br />

measurements, we calculated the <strong>LAI</strong> associated specifically<br />

with foliage (<strong>LAI</strong>F) as did Chen et al. (1997):<br />

<strong>LAI</strong><br />

F<br />

( 1 − α) <strong>LAI</strong> γ<br />

=<br />

Ω<br />

e<br />

e e<br />

where <strong>LAI</strong> F is <strong>LAI</strong> corrected for with<strong>in</strong>-shoot <strong>and</strong> above-shoot<br />

level clump<strong>in</strong>g <strong>and</strong> α is the woody-to-total area ratio. The<br />

value <strong>of</strong> α was derived from destructive sampl<strong>in</strong>g (Chen et al.<br />

1997): α = W/<strong>LAI</strong>total, where W is the woody area <strong>in</strong>dex <strong>and</strong><br />

<strong>LAI</strong>total is the total <strong>LAI</strong> from woody <strong>and</strong> green foliar material<br />

comb<strong>in</strong>ed.<br />

Our calculation <strong>of</strong> α was based on <strong>in</strong> <strong>situ</strong> measurements <strong>of</strong><br />

foliage <strong>and</strong> woody area per tree, derived from destructive measurements<br />

<strong>of</strong> the branches <strong>and</strong> measured total tree height,<br />

bole length, crown dimensions <strong>and</strong> crown length, <strong>and</strong> plotted<br />

aga<strong>in</strong>st DBH. We applied these relationships to determ<strong>in</strong>e the<br />

mean α <strong>of</strong> the whole st<strong>and</strong> <strong>and</strong> obta<strong>in</strong>ed a value <strong>of</strong> 0.18, which<br />

is consistent with the analysis <strong>of</strong> the digital hemispherical images,<br />

where the amount <strong>of</strong> woody material was estimated by<br />

means <strong>of</strong> image classification, assum<strong>in</strong>g the stems <strong>and</strong><br />

branches seen on the photographs were simple cone shapes<br />

(Barclay et al. 2000).<br />

Results<br />

TREE PHYSIOLOGY ONLINE at http://heronpublish<strong>in</strong>g.com<br />

Allometric relationships<br />

Allometric relationships at the branch <strong>and</strong> tree levels Regression<br />

equations at the branch <strong>and</strong> tree levels were derived from<br />

measurements <strong>of</strong> the six experimental trees (Table 5). The relationships<br />

<strong>in</strong> Table 5 are the best fits <strong>of</strong> the fitted regressions <strong>and</strong><br />

were <strong>in</strong> all cases significant at P < 0.001. They were applied <strong>in</strong><br />

this study to calculate canopy cover <strong>and</strong> PLA at the st<strong>and</strong> level<br />

(Table 5). Allometric relationships between tree height <strong>and</strong><br />

bole length <strong>and</strong> between tree height <strong>and</strong> tree diameter were established<br />

by means <strong>of</strong> the Rayleigh equation (Table 6).<br />

At the branch level, a good relationship was found between<br />

branch cross-sectional area <strong>and</strong> needle leaf area (as well as<br />

needle dry mass) (r 2 ≥ 0.80) (Figure 2). In agreement with<br />

other studies (e.g., Mencucc<strong>in</strong>i <strong>and</strong> Grace 1995), significant<br />

regression relationships were found at the tree level between<br />

basal area <strong>and</strong> DBH as <strong>in</strong>dependent variables, <strong>and</strong> needle area,<br />

(6)<br />

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