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Using TDR to Estimate Hydraulic Conductivity and Air Entry in Growing Media and Sand

Jean Caron*,a, Louis-Marie Rivièreb, Sylvain Charpentierb, Pierre Renaultc and Jean-Charles Michelb

a Département des sols et de génie agroalimentaire, Université Laval, Sainte-Foy, QC, Canada G1K 7P4
b SAGAH-Institut national de la recherche agronomique, Centre d'Angers and Institut national d'horticulture, 42 Georges Morel, C.P.57, Beaucouzé 49071 France
c Unité de science du sol. – Domaine St-Paul – Site Agroparc Avignon, 84914 France



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Fig. 1. Possible water content at different locations following wetting, (A) saturation and (B) drainage; t represents different times, x(t), the position of the wetting front at time t, L is the length of the column, and xa is the point of air entry.

 


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Fig. 2. Schematic representation of the sequential water content measurements ({theta}[t],{theta}s,{theta}i,{theta}c) performed to estimate Ks and {psi}a.

 


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Fig. 3. Experimental set-up used to perform the measurements.

 


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Fig. 4. Calibration curves obtained using (A) the CS-615 and (B) the Tektronix 1502-C instruments. Mineral refers to substrates with <0.20 kg kg-1 of organic matter content, and organic, with 0.20 kg kg-1 of organic matter content and more.

 


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Fig. 5. Examples of the relationships obtained between the position of the wetting front [L-x (t)] and time.

 


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Fig. 6. Relationship between the Ks estimates obtained under transient-state conditions with TDR (A.2), under steady-state conditions with an infiltrometer after a rapid resaturation with a pulse of water (A.4), under steady-state conditions with an infiltrometer after prolonged resaturation (B.1), and the Ks estimate obtained under steady-state conditions following wetting under tension (A.3).

 


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Fig. 7. Variations in air pressure recorded for different growing media during desorption in A.5.

 





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