CN119164836B - A method for predicting capillary water flux by capillary water rise height - Google Patents
A method for predicting capillary water flux by capillary water rise heightInfo
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- CN119164836B CN119164836B CN202411338548.7A CN202411338548A CN119164836B CN 119164836 B CN119164836 B CN 119164836B CN 202411338548 A CN202411338548 A CN 202411338548A CN 119164836 B CN119164836 B CN 119164836B
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- G01N13/00—Investigating surface or boundary effects, e.g. wetting power; Investigating diffusion effects; Analysing materials by determining surface, boundary, or diffusion effects
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- G—PHYSICS
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- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
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- G01N15/082—Investigating permeability by forcing a fluid through a sample
- G01N15/0826—Investigating permeability by forcing a fluid through a sample and measuring fluid flow rate, i.e. permeation rate or pressure change
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
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Abstract
The invention belongs to the field of capillary water rising flux test, and discloses a novel method for predicting capillary water rising flux based on capillary water rising height, and estimating capillary water rising flux by acquiring a soil air outlet value h a, a soil saturation permeability coefficient K s, a correction coefficient lambda of the model capillary water rising height and a fitting parameter beta', and combining the deduced mechanism model. The invention divides the capillary water rising into two stages, derives and establishes a new mechanism model of the capillary water rising flux along with the height change based on Darcy's law under the unsaturated condition, the model covers the whole rising process of the water level, compared with an empirical model, the model has wider application range, and the model fitting value has better matching degree with an observed value.
Description
Technical Field
The invention belongs to the field of capillary water rising flux test, and particularly relates to a method for predicting capillary water rising flux based on capillary water rising height.
Background
Soil capillary water refers to liquid water held and moved by capillary force in the pores of the soil capillary, and is one of main sources of water required by plant growth.
Two predictive models are commonly employed in existing methods of predicting capillary water flux. One is a mechanism model, which focuses on the capillary water part rise interval, and predicts poor accuracy when the range is exceeded. The other is an empirical model, which is suitable for specific conditions, and when the actual situation deviates from the condition according to the model, the prediction of the model will have errors.
Disclosure of Invention
Based on the problems existing in the prior art, the invention divides the capillary water rising process into two stages by taking the soil air outlet value as a threshold value, and derives a new mechanism model of capillary water rising flux along with the change of height according to Darcy's law under the unsaturated condition, which is used for predicting capillary water rising flux under different rising heights of capillary water.
The invention is realized in that a method for predicting capillary water flux by capillary water elevation comprises the steps of:
Step one, obtaining a soil air outlet value h a.
And step two, obtaining a soil saturation permeability coefficient K s.
And thirdly, obtaining a correction coefficient lambda and a fitting parameter beta' of the capillary water rising height of the model.
And step four, predicting capillary water rising flux according to the parameters and the deduced mechanism model.
In the first step, soil to be measured is taken for a soil moisture absorption experiment. And before the experiment starts, drying the soil sample to be tested until the water content of the soil is reduced to 0. Then slowly adding a certain volume of water into the soil, measuring the volume water content and the matrix suction force in the soil after the water is fully diffused, and then repeating the processes of adding water and measuring the volume water content and the matrix suction force until the volume water content reaches saturation, reducing the matrix suction force to 0Kpa, and finishing the soil moisture absorption experiment. And (3) converting the suction force of the soil matrix measured by the experiment into the height of a centimeter water column, drawing a moisture absorption curve of a soil moisture characteristic curve by taking the matrix potential as an x axis and the volume moisture content as a y axis.
The Gardner model (Gardner, 1958) was used as a fitted model for the earth-water characteristic curve:
Wherein θ and θ S are average volume water content and saturated volume water content respectively, h is matrix suction force, cm, θ r is residual water content, and c and m are model shape parameters.
And drawing a tangent line at the saturation volume water content and a tangent line of an inflection point by using the soil moisture characteristic curve fitted by the model, and prolonging the two tangent lines, wherein the abscissa of the intersection point of the two tangent lines is expressed as the soil air outlet value height h a, and the unit is cm.
In the second step, the soil is filled into the columnar container, and the soil density in the soil column is reduced to the original soil density by knocking the column wall. The column was immersed in water. And taking out the water after the water saturation time is reached, fixing the soil column by using an iron frame table, placing a beaker below the soil column, adding water above the soil column by using a Marshall bottle, keeping a certain thickness of a water layer, and keeping a constant water level.
Starting timing when the first drop of water appears below the soil column, measuring the water seepage amount at intervals, and recording the water temperature. The cumulative water seepage V measured each time is set as a y axis, the time t spent by the cumulative water seepage is set as an x axis, and a change curve of the soil cumulative water seepage along with time is obtained. The change curve of the soil infiltration amount along with the time gradually shows a linear correlation, which means that the soil infiltration amount is the same in a certain time, and a stable state is achieved.
The permeability coefficient is calculated according to the darcy formula:
Wherein the method comprises the steps of
Wherein V is the water quantity penetrating through the soil column sectional area A (cm 2) within the time t (h), cm 3, I is the hydraulic gradient, K is the permeability coefficient, namely the permeability speed when the hydraulic gradient is 1, cm/h, L is the water penetration distance of two points designated in the soil column, cm, and Deltah is the total water head difference between the two points designated.
Further, in the third step, a new dry soil column is prepared, and a Marshall bottle is utilized to provide stable groundwater level and sufficient water source. When the experiment starts, water is supplied from a Marshall bottle to enable water to flow into the soil column, when the water level in the soil column rises to a stable underground water level, the rising height of capillary water at the moment is recorded to be 0cm, the rising time is 0h, and the rising water volume is 0cm 3. In the first stage of capillary water rising (the rising height of the capillary water is smaller than the soil air outlet value h a), the rising time and the graduation of the water tank are recorded once when the capillary water rises to a certain height until the capillary water rises to 1/3h a, and a plurality of discrete data points are acquired. The capillary water rising flux (q 0) is obtained by utilizing the rising water volume and the rising time estimation, and then the capillary water rising height (z T) is combined with a plurality of discrete values, the soil air outlet value h a and the soil saturation permeability coefficient K s, and the correction coefficient lambda of the capillary water rising height can be obtained by substituting the following formula:
In the formula (3), q 0 is capillary water rising flux, cm/h, K s is saturation permeability coefficient (cm/h), z T is capillary water rising height, cm, lambda is correction coefficient of capillary water rising height, and h a is soil air outlet value.
In the second stage of capillary water rising (the rising height of the capillary water is larger than the soil air outlet value h a), the rising time and the graduation of the water tank are recorded once when the capillary water rises to a certain height until the capillary water rises to 4/3h a, and a plurality of discrete data points are acquired. The capillary water rising flux is estimated by utilizing the rising water volume and the rising time, and then a plurality of discrete values of the capillary water rising height, the soil air outlet value h a and the soil saturation permeability coefficient K s are combined and substituted into the following formula to obtain the model fitting parameter beta':
In the formula (4), beta' is a model fitting parameter.
In the fourth step, the model parameters estimated in the first to third steps and formulas (3) and (4) are used to estimate the capillary water rising flux at other heights in the capillary water rising process.
In summary, the invention has the advantages and positive effects that:
The capillary water rising is divided into two stages, and a new mechanism model of the capillary water rising flux changing along with the height is deduced and established based on Darcy's law under the unsaturated condition. The model covers the whole rising process of the water level, has wider application range compared with an empirical model, and has better matching degree between a model fitting value and an observed value.
Drawings
FIG. 1 is a schematic flow chart of a method for predicting capillary water flux;
FIG. 2 is a graph showing a first stage of capillary water rise flux prediction (capillary water rise height less than h a);
FIG. 3 is a graph of a second stage of capillary water rise flux prediction (capillary water rise height greater than h a).
Detailed Description
In order to make the objects, technical solutions and advantages of the present invention more apparent, the present method will be described in further detail with reference to the following examples.
The method for predicting capillary water flux through the capillary water elevation provided by the embodiment of the invention comprises the following steps:
Step one, obtaining a soil air outlet value h a.
And step two, obtaining a soil permeability coefficient K s.
And thirdly, obtaining a correction coefficient lambda and a fitting parameter beta' of the capillary water rising height of the model.
And step four, predicting capillary water rising flux according to the parameters and the deduced mechanism model.
In the first step, 0.075mm quartz sand is taken for soil moisture absorption experiments. Before the experiment starts, the quartz sand sample is dried until the water content of the soil is reduced to 0. Then slowly adding a certain volume of water into the soil, measuring the volume water content and the matrix suction force in the soil after the water is fully diffused, and then repeating the processes of adding water and measuring the volume water content and the matrix suction force until the volume water content reaches saturation, reducing the matrix suction force to 0Kpa, and finishing the soil moisture absorption experiment. And (3) converting the suction force of the soil matrix measured by the experiment into the height of a centimeter water column, drawing a moisture absorption curve of a soil moisture characteristic curve by taking the matrix potential as an x axis and the volume moisture content as a y axis.
The Gardner model (Gardner, 1958) was used as a fitted model for the earth-water characteristic curve:
Wherein θ and θ S are average volume water content and saturated volume water content respectively, h is matrix suction force, cm, θ r is residual water content, and c and m are model shape parameters.
And drawing a tangent line at the saturation volume water content and a tangent line of an inflection point by using the soil moisture characteristic curve fitted by the model, and prolonging the tangent line, wherein the abscissa of the intersection point of the two tangent lines is expressed as the height of the soil air outlet value, h a is 69, and the unit is cm.
In the second step, quartz sand with the thickness of 0.075mm is filled into a columnar container, and the soil density in the soil column is reduced to the original soil density by knocking the columnar wall. The soil column is immersed in water, taken out after the water saturation time is reached, the soil column is fixed by an iron frame table, water is added above the soil column by a Marshall bottle, a beaker is placed below the soil column, the thickness of a water layer is kept to be 5cm, and meanwhile, the constant water level is kept. Starting timing when the first drop of water appears from the lower part of the soil column from the beginning of the water supply of the Marshall bottle, measuring the water seepage amount every 5 minutes, and simultaneously recording the water temperature. The cumulative water seepage V measured each time is set as a y axis, the time t spent by the cumulative water seepage is set as an x axis, and a change curve of the soil cumulative water seepage along with time is obtained.
The permeability coefficient was calculated according to the Darcy formula to give K s of 3.23cm/h.
Wherein the method comprises the steps of
Wherein V is the water quantity penetrating through the soil column sectional area A (cm 2) within the time t (h), cm 3, I is the hydraulic gradient, K is the permeability coefficient, namely the permeability speed when the hydraulic gradient is 1, cm/h, L is the water penetration distance of two points designated in the soil column, cm, and Deltah is the total water head difference between the two points designated.
In the third step, a new dry earth pillar is prepared, a Marshall bottle is used for providing stable groundwater level and sufficient water source, water is supplied to the earth pillar by the Marshall bottle when an experiment starts, when the water level in the earth pillar rises to the stable groundwater level, the rising height of capillary water at the moment is recorded to be 0cm, the rising time is 0h, and the rising water volume is 0cm 3. In the first stage of capillary water rising (capillary water rising height is smaller than soil air outlet value h a), rising time and graduation of the water tank are recorded at a distance of rising by 2cm until capillary water rises to 1/3h a, and a plurality of discrete data points are acquired. And estimating by utilizing the rising water volume and the rising time to obtain capillary water rising flux (q 0), combining a plurality of discrete values of the capillary water rising height (z T), the soil air outlet value h a and the soil saturation permeability coefficient K s, and substituting the discrete values into the following formula to obtain the correction coefficient lambda of the capillary water rising height which is 0.7475.
In the formula, q 0 is capillary water rising flux, cm/h, z T is capillary water rising height, cm, lambda is correction coefficient of capillary water rising height, and beta' is fitting parameter.
In the second stage of capillary water rising (the rising height of the capillary water is larger than the soil air outlet value h a), the rising time and the graduation of the water tank are recorded once every 2cm of capillary water rising until the capillary water rises to 4/3h a, and a plurality of discrete data points are acquired. And estimating by using the rising water volume and the rising time to obtain the capillary water rising flux, and substituting the capillary water rising flux, the soil air outlet value h a and the soil saturation permeability coefficient K s into the following formula to obtain the model fitting parameter beta' of 0.086.
In the fourth step, the model parameters and formulas (7) and (8) estimated in the first to third steps are used to estimate the capillary water rising flux of other heights in the capillary water rising process.
The above embodiments are only for illustrating the technical concept and features of the present invention, and are intended to enable those skilled in the art to understand the content of the present invention and to implement the same, but are not intended to limit the scope of the present invention, and all equivalent changes or modifications made according to the spirit of the present invention should be included in the scope of the present invention.
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| CN108458961A (en) * | 2018-03-28 | 2018-08-28 | 江西理工大学 | A kind of ion type rareearth leaching solution capillary rise pilot system and experimental method |
| CN115436235A (en) * | 2022-09-07 | 2022-12-06 | 成都理工大学 | Laboratory permeability coefficient determination method based on capillary water rise |
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| CN204694602U (en) * | 2015-06-17 | 2015-10-07 | 成都理工大学 | A kind of measurement capillary soil water climbing height test unit |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| CN108458961A (en) * | 2018-03-28 | 2018-08-28 | 江西理工大学 | A kind of ion type rareearth leaching solution capillary rise pilot system and experimental method |
| CN115436235A (en) * | 2022-09-07 | 2022-12-06 | 成都理工大学 | Laboratory permeability coefficient determination method based on capillary water rise |
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