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Images of different computer-generated Lindenmayer systems (i.e., fractal trees) were analyzed using the open-source image analysis software FracLac. First, the fractal dimension was calculated using regular box-counting, and then with the differential box-count technique. The box-count analysis estimated the objects to have fractal dimensions between \( 1.81 \pm 0.056 < D_B < 1.90 \pm 0.66 \); however, the differential box-count mass dimension was found to be lower on average, with \( D_M = 1.60 \pm 0.10 \) (Table 1).

In Tables 1-X and Figures X-X, the observed mass dimensions of x-ray leaves, branches, and roots are statistically indistinguishable from the MST and fractional Brownian motion (fBm) predictions of \( \alpha = 3/2 \).

From Equation 18, a differential mass dimension for such an image is expected to equal \( 4/3 \) rather than \( 3/2 \) (see Supplementary Information).

Table 1: Synthetic Fractal Dimensions

Fractal mass dimension \( d_m \pm \mu \text{SE} \) and coefficient of variation (CV):

\[ \text{CV} = \frac{\sigma}{\mu} \]

where \( \sigma \) is the standard deviation over the mean number of pixels per box. The associated lacunarity \( \Lambda \) and CV are also reported.

Fractal Type Pixels \( d_m \pm \mu \text{SE} \) \( \mu r^2 \) \( d_m (\frac{\sigma}{\mu}) \) \( \Lambda \) \( \Lambda (\frac{\sigma}{\mu}) \)
Peano Curve 1 (square) 756,030 1.846 ± 0.100 0.9966 0.0111 0.0133 0.2128
Peano Curve 2 (rounded) 1,440,000 1.803 ± 0.109 0.9959 0.0161 0.0713 0.1348
H-fractal 3,932,289 1.760 ± 0.124 0.9945 0.0102 0.1142 0.0746
Pythagoras Tree 1 5,000,000 1.607 ± 0.106 0.9953 0.0030 0.7003 0.0871
Pythagoras Tree 2 393,216 1.655 ± 0.075 0.9976 0.0108 0.2267 0.0899
Barnsley's Fern 180,000 1.576 ± 0.073 0.9973 0.0116 0.3787 0.0680
Fibonacci Tree 348,140 1.470 ± 0.074 0.9969 0.0118 0.8680 0.0657

Table 2: Observed Leaf Mass Dimensions

Observed local mass fractal dimension of five different types of leaves. Results were obtained using the FracLac Differential Box Count for a power series with an exponentially increasing box size factor of 0.1.

Image Pixels \( d_M = \ln(\mu_\varepsilon) / \ln \varepsilon \) \( \mu r^2 \) \( \mu \text{SE} \) \( CV (\frac{\sigma}{\mu}) \)
Coleus 144,316 1.5384 0.9938 0.1008 0.0038
Fig 315,495 1.4844 0.9918 0.1123 0.0026
Nasturtium 1,115,114 1.5525 0.9969 0.0880 0.0010
Ginkgo 1,086,596 1.5135 0.9978 0.0705 0.0020
Fern 581,196 1.5083 0.9968 0.1268 0.0064

Table 3: Observed Branch/Root Mass Dimensions

Observed local mass fractal dimension of three branching networks. Results were obtained using FracLac Differential Box Count for a power series with an exponentially increasing box size factor of 0.1.

Image Pixels \( d_M = \ln(\mu_\varepsilon) / \ln \varepsilon \) \( \mu r^2 \) \( \mu \text{SE} \) \( CV (\frac{\sigma}{\mu}) \)
Single branch 255,285 1.4946 0.9953 0.0850 0.0024
Maple branches 473,450 1.4775 0.9944 0.0920 0.0057
Maple root 617,312 1.4549 0.9970 0.0668 0.0016

Table 4: Forest Canopy Height Model Dimensions

Aerial LiDAR Canopy Height Models (CHM) over various forest types. Results were obtained using FracLac Differential Box Count for a power series with an exponentially increasing box size factor of 0.1. The predicted mass fractal dimension is \( \frac{3}{2} \) or 1.5.

Image Pixels Mass Dimension \( d_M \) \( \mu r^2 \) \( \mu \text{SE} \) \( CV (\frac{\sigma}{\mu}) \)
Lowland Rainforest 361,201 1.3313 0.9860 0.1969 0.0128
Pine/Hardwood (South Carolina) 362,403 1.5223 0.9898 0.1919 0.0135
Sierra Madre Oaks (Arizona) 362,404 1.4973 0.9886 0.1988 0.0116
Western Ponderosa Pine (New Mexico) 361,802 1.4566 0.9847 0.2252 0.0144
Southwest Mixed Conifer (New Mexico) 361,802 1.5319 0.9869 0.2190 0.0177
Southwest Spruce-Fir (New Mexico) 361,802 1.5355 0.9862 0.2255 0.0139

Statistical Validation

The observed mass dimensions across all sample types show remarkable consistency with the MST prediction of \( d_m = \frac{3}{2} \). The mean observed dimension across all leaf samples was \( 1.519 \pm 0.027 \), across branch samples was \( 1.476 \pm 0.020 \), and across forest canopy samples was \( 1.479 \pm 0.080 \).

These results provide strong empirical support for the theoretical predictions of Metabolic Scaling Theory and demonstrate that the differential box-counting method is appropriate for measuring the self-affine fractal dimensions of biological branching networks.