DESCRIBING SOIL HYDRAULIC-PROPERTIES WITH SUMS OF SIMPLE FUNCTIONS

DESCRIBING SOIL HYDRAULIC-PROPERTIES WITH SUMS OF SIMPLE FUNCTIONS
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DOI:
10.2136/sssaj1993.03615995005700010006x
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发表时间:
1993-01-01
影响因子:
2.9
通讯作者:
SMETTEM, KRJ
SMETTEM, KRJ
中科院分区:
农林科学3区
文献类型:
--
作者:
ROSS, PJ;SMETTEM, KRJ

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简单的功能不足以描述许多领域的土壤,特别是那些大量的大孔隙度的水力特性。考虑与有效饱和度S(psi)= SIGMA(i=1)N phi(i)S(i)(psi)相对应的土壤孔隙尺寸分布f(psi)= SIGMA(i=1)N phi(i)F(i)(psi),其中psi为基质压头,phi(i)为有效孔隙度分数,S(i)(psi)为常用的简单持水函数,f(i)(psi)= S(i)′(psi),根据Mualem模型,我们发现相对水力传导系数为K(r)(psi)= S(p)[SIGMA(i=1)N phi(i)g(i)(psi)/SIGMA(i=1)N phi(i)g(i)(0)2,其中g(i)(psi)= integral-psi/-xpsi-1f(i)(psi)dpsi,p是孔隙相互作用指数。如果分布的孔隙不相互作用,则适当的关系为K(psi)= SIGMA(i=1)N K(si)K(ri)(psi),其中K(si)是分布i的饱和电导率,并且K(ri)= S(p)[g(i)(psi)/g(i)(0)]2。我们注意到,当m = 1 - 1/n时,货车范希滕函数S(psi)= [1 +(-ψ)n]-m导致在psi = 0处的斜率K '(psi)为无穷大,除非n大于或等于2,如果考虑大范围的基质压头,这对于野外土壤是不现实的。饱和附近的渗透系数通常表示为K(psi)= K(s)exp(apsi)。我们引入函数S(psi)=(1 -ε apsi)exp(ε apsi),根据Mualem的模型,它给出了电导率K(psi)= K(s)(1 -ε apsi)p exp[(p + 2)ε apsi],如果a = 2alpha,则接近饱和,如果p = 0,则完全相等。作为一个例子,一个函数使用此模型的一个孔径分布和货车van Eschchten模型的另一个进行了比较,一个函数使用两个货车Eschchten分布。后者给了一个稍微改进的适合聚合土壤的含水量和电导率数据。
Simple functions do not adequately describe the hydraulic properties of many field soils, particularly those with substantial macroporosity. By considering the soil pore-size distribution f(psi) = SIGMA(i=1)N phi(i) F(i)(psi) corresponding to the effective saturation S(psi) = SIGMA(i=1)N phi(i) S(i)(psi), where psi is matric pressure head, the phi(i) are fractions of effective porosity, the S(i)(psi) are simple water retention functions in common use, and f(i)(psi) = S(i)'(psi), we show that the relative hydraulic conductivity according to the Mualem model is K(r)(psi) = S(p)[SIGMA(i=1)N phi(i) g(i)(psi)/SIGMA(i=1)N phi(i) g(i)(0)2, where g(i)(psi) = integral-psi/-x psi-1 f(i)(psi) dpsi and p is a pore interaction index. If the pores of the distributions do not interact, the appropriate relation is K(psi) = SIGMA(i=1)N K(si)K(ri)(psi), where K(si) is the saturated conductivity of distribution i and K(ri) = S(p)[g(i)(psi)/g(i)(0)]2. We note that the van Genuchten function S(psi) = [1 + (-alphapsi)n]-m with the restriction m = 1 - 1/n leads to an infinite slope K'(psi) at psi = 0 unless n greater-than-or-equal-to 2, which is unrealistic for field soils if a wide range of matric pressure heads is considered. Hydraulic conductivity near saturation is often expressed as K(psi) = K(s) exp(apsi). We introduce the function S(psi) = (1 - alphapsi) exp(alphapsi), which gives, according to Mualem's model, a conductivity K(psi) = K(s)(1 - alphapsi)p exp[(p + 2)alphaphi] that approximates K(s) exp(apsi) near saturation if a = 2alpha and is exactly equal if p = 0. As an example, a function using this model for one pore-size distribution and the van Genuchten model for the other was compared with a function using two van Genuchten distributions. The latter gave a slightly improved fit to water content and conductivity data for an aggregated soil.