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Table IV

Review of the literature about the relationships between wood density and Hounsfield numbers obtained with medical CT scanners.

Wood density
Reference Species Moisture content (kg m−3) Slope Intercept n R 2 Scanner kVp mA
Radiata pine, Douglas fir,
Benson-Cooper Eucalyptus delegatensis Technicare 120 40–200
et al. (1982) Tasmanian blackwood, Red beech Green wood ~500–1150 0.910 1002 40 0.92 Delta2020 (during 2 s)

Pine, Mahogany, Poplar, Ohio-Nuclear 50
Mull (1984) Maple, Ash, Teak 367–798 7 2010 CT 120
(+ graphite) scanner (during 4 s)

2–96% ~600–1000 (a) 0.876 968 35 0.98
Hattori and Red meranti (b) 1.002 1018 35 0.98

Kanagawa Oven-dry wood ~550–620 (b) 0.973 1040 35 0.74 Toshiba 120 230

(1985)1 2–27% ~430–500 (b) 0.894 966 35 0.94 TCT-20A

Agathis (a) 0.855 948 35
Oven-dry wood ~425–450 (b) 0.894 966 35

Lindgren 6–117% ~350–1000 0.993 1015 50 GE 9800

(1991b) Oven-dry wood 352–619 1.052 1053 11 Quick

Balsa, Treated pine, Radiata
pine, Oregon, Meranti,
Davis and Cypress pine, Merbau,
Wells (1992) NZ pencil pine, Red gum ~100–1100 1.006 1035 13 EMI CT1010 120 20–30
Jarrah, Gray box, Red box,
Red iron bark

Taylor Air-dried wood Medical CT
(2006) West African hardwood (~12%) ~350–1100 1.044 1044 25 0.986 scanner

(a) Without granulated sugar surrounding the wood samples. (b) With granulated sugar surrounding the wood samples.

1

At the opposite of other authors, Hattori and Kanagawa modelled the Hounsfield numbers as a function of density, i.e. H = aρ + b′ instead of ρ = aH + b. We computed the parameters a and b, presented in Table , from their reported values of a′ and b′ as: a = 1 / a′ and b = − b′ / a′. It is slightly different from what would have been obtained by estimating directly a and b parameters by regressions performed on the raw data. In this case, the slope parameter would have been equal to R2 × 1 / a′.