ENVS 2060 Lab 3

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Dec 6, 2023

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Lab # 3 Water in Soil Recommended Reading: Weil and Brady, 2017: The nature and properties of soils. 15 th ed., Chapters 5 and 6 Digging into Canadian Soils 114-116, 118-132 Part 1. Water Content a) Use the data provided in table 1 to calculate the: Mass of water in each soil, volume of water, mass based water content (sometimes called gravimetric water content) (θm), Volumetric water content (θv), depth equivalent water content in the 50 cm depth of each soil (Dw), soil bulk density (BD), soil pore space ratio (PSR), and the percentage of the pore space occupied by water. For each calculation provide your rough work for the calculations on one of the soils and provide your answers in table 2 below. Remember that the particle density will remain constant at 2.65 g cm -3 . Table 1 Data on soil cores for use in calculation in part 1 a. Core # Wet weigh of soil (g) Dry weight of soil (g) Volume of soil (cm 3 ) 1 172 128 126 2 198 166 126 3 221 173 126 Table 2 Core # Mass of water (g) Volume of water (cm 3 ) Θm (%) Θv (%) Dw cm/cm BD (g cm -3 ) PSR (%) % of pore space filled with water 1 2 3
Part 2: Soil water potential at equilibrium a) Assuming equilibrium , determine the value of ψ h and its components (ψ m , ψ p and ψ g ) at points A, B and C in the above diagram. Express the potentials in units of cm of water in table 3. Figure 1 soil water potential diagram Table 3 soil water potential at equilibrium using position “B” as the gravitational reference POINT Potential A (at surface) B C ψ p ψ m ψ g ψ h b) Currently in figure 1 the gravitational reference point is given at position “B” (the water table). The gravitational reference point could however be placed anywhere in the soil profile as it is just a measure of the relative gravitational energy. Move the gravitational reference point to position “A” and determine the value of ψ h and its components (ψ m , ψ p and ψ g ) at points A, B and C in the above diagram. Express the potentials in units of cm of water in table 4. Table 4 soil water potential at equilibrium using position “A” as the gravitational reference POINT Potential A B C ψ p
ψ m ψ g ψ h c) Make note that even though the absolute values of ψ h changed in table 3 and table 4 that the relative values between positions stays the same. Part 3 Soil water potential at non-equilibrium 1. In non-equilibrium condition soil matric potential cannot be determined based on the position relative to the water table. As such the matric potential must be measured at each of the desired positions in a soil. Tensiometers, which measure metric potential, were installed at four different depths (0, 10, 30 and 60 cm below the soil surface) in a soil profile. On three different days (day 1, 3 and 10) readings of ψ m (in cm H 2 0) are obtained. The data are presented below in Table 5. a) Using position A in table 5 as the gravitational reference point, complete table 5 by filling in values for ψ g and ψ h and indicate in the fourth column for each day whether the water is flowing upward (↑) or downward (↓) or is at a standstill (0) between adjacent positions (ie between position “A” and “B”, “B” and “C” etc.). e.g A water flow is from point B to point A B Table 5 Non-equilibrium soil hydraulic potentials. Day 1 Day 3 Day 10 Depth (cm) ψ m ψ g ψ h 0 ψ m ψ g ψ h ↑ ↓ 0 ψ m ψ g ψ h ↑ ↓ 0 0 A -125 -4 -45 10 B -60 -25 -30 30 C -15 -25 -12 60 D -290 -320 -258 c) What can you say about the most likely weather pattern during this ten-day period?
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d) In this case (table 5), explain why was the pressure potential (ψ p) not determined? Part 4. Available Water a) Compare the moisture characteristic data for the following 3 soils (figure 2) and complete table 6 assuming the soil is uniform in texture and structure to 50 cm soil depth. To determine the volume of water per hectare in table 6 multiply the depth of available water in meters by the surface area of 1 hectare (10000 m 2 ). Also remember that there are 1000L in 1 m 3 of water. Figure 2 water release curves of 3 soils for use in Part 4 a. Matric Potential Ψm (bars) Table 6 determination of plant available water from figure 2 Water content (θv) at Field Cap. Water content (θv) Wilting Point Plant available water content (θv) depth of available water in top 50 cm of soil Volume (L/ha) of water plant available in top Soil Water Content θv (% m 3 m -3 )
50 cm of soil Soil 1 Soil 2 Soil 3 Part 5. Water Movement in Saturated Soils In class we discussed Darcy’s experiment. Figure 3 gives a representation of an experiment to determine the flux rate of water coming through a soil. Figure 3 Darcy’s experiment example to be used to complete table 7 and 8 a) Determine the hydraulic potential (ψh) at both point A and B represented in figure 2. Present the data in table 7 Table 7 hydraulic potential for the experiment indicated in figure 3 Position in figure 2 Potential A B ψ p ψ m Soil Water 15 cm 12 cm Ref point A B 10 cm 12 cm 11 cm 13 cm
ψ g ψ h b) Use the information you determined in Table 7 and the information in figure 3 to determine for each of the soils in table 8: the flux rate of water (Jw) (equation below), the change in hydraulic potential ( ψh) (from table 7), and the hydraulic conductivity (k) (equation below) and record the information in table 8. Be sure to show your work. Vw Jw = AT Jw = -k Ψ h Z Table 8 presentation of results for Part 5 b. Volume of water collected (Vw) Surface Area of soil (A) Time (T) Flux rate of water (Jw) ψh Z k Soil 1 115 cm 3 45 cm 2 60 seconds Soil 2 30 cm 3 45 cm 2 60 seconds Part 2 Water movement in unsaturated soils Watch the following video that describes water movement in soils. https://www.youtube.com/watch?v=DmTNFIEc2VA and/ have a look at the displays in the lab (note they show the same thing as the video) a) At approximately three minutes 10 seconds in the video (3:10) there is a demonstration of capillary rise use two glass plates. They are separated on one site and clamped directly together on the other to represent a range of pore size from large on the open side to very small on the other side. Examine the wedge capillary on the demonstration table and the height of rise above the free water surface at the closed edge of the wedge. If the water on the edge of the glass that was closed together was drawn up to a total hight of 20 cm, use the following equation calculate the theoretical radius of the pore at the edge of the wedge. 0.15 h = r
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b) Once again from the video, describe what happened when water was moving through a non-saturated loam textured soil and encountered a sand layer (3:48). Explain why this effect happens using your knowledge of soil hydraulic potentials and hydraulic conductivity. c) Similarly describe what happened when water was moving through a silt loam textured soil and encountered a clay layer (6:36). Explain why this effect happens using your knowledge of soil hydraulic potentials and hydraulic conductivity. d) Similarly explain what happened when the water encountered a diagonal band of sandy soil that extended to the soil surface (10:50). Explain why this effect happens using your knowledge of soil hydraulic potentials and hydraulic conductivity. Be sure to explain the difference in effect caused by this sand band compared to the one in part “b”