Soil, Water and Atmospheric Processes 2h Tutorial – Evaporation Simulation of Evaporation. This tutorial will help reinforce some of the lecture material on water vapour, evaporation and turbulent transfer processes. You will use a simulation model of the evaporation process (essentially the Penman-Monteith equation we covered in Lecture #8) to answer a small number of questions. By doing so, you should begin to appreciate how sensitive the evaporation process is to its driving parameters e.g. solar radiation, vapour pressure gradient, atmospheric turbulence and vegetation-related factors. Your answers to the questions form part of the continuous assessment for this course. You will be given a worksheet to record your answers and you should hand in the completed worksheet by next Wednesday (7 March) to Helen McKeating. Activities Log on to the university network and use the FireFox browser to navigate to one of the pages on the micrometeorology site: http://www.geos.ed.ac.uk/abs/research/micromet/java/ and select the first Applet for the SWAP course (click on the Web Start (gold) icon) When you enter this web page you will see text explaining what you have to do plus the image below. You can control the simulation by altering the scrollbars labeled ‘Solar radiation’, vapour pressure’ etc. this will change the driving variables for evaporation. The model was demonstrated to you briefly at the end of Lecture #8 in JBM’s lecture series. It is important you are confident with the model before you attempt the worksheet- you should ask the demonstrators to help if you are unsure of anything before you start. The model has a default set of weather conditions which are restored whenever the ’reset’ button is pressed. You can alter the sliders to explore the sensitivity of the model to changes in solar radiation, vapour pressure, wind speed etc. You can also choose different types of vegetation and explore how sensitive they are to changes in the weather conditions. The different surface types will differ in their albedo, roughness length and canopy resistance. 1 of 4 Soil, Water and Atmospheric Processes 2h Tutorial – Evaporation About the Penman-Monteith model Surface In lecture #8, we discussed roughness the advance that Monteith term made to the Penman equation when he introduced n p z o a resistances to water vapor transport that were c associated with the vegetation. You can think of resistances in an analogous a Surface form to Ohm’s Law – for a wetness given potential difference term (voltage), current will flow at a rate determined by the electrical resistance of the circuit (I=V/R). The aerodynamic roughness of the vegetation will influence the ease with which water vapour can be removed from leaves, hence the ‘surface roughness term’, introduces the aerodynamic resistance (ra) which is a function of wind speed and roughness length (see the tutorial web page for the formula). The taller and rougher the vegetation, the smaller will be ra (all else being equal). See Oke (1987) BoundaryLayer Climates, page 70 for more details. LE = 'R + *c (e ( e ) / r & r ' + ) $$1 + % r # !! " It was recognized in the 1960’s that plants were not merely ‘passive wicks’ in the evaporation process but were able to control their loss of water to some extent by opening and closing their stoma. The degree of closure of the stomatal aperture can be a function of solar radiation, internal CO2 concentration, soil water availability and other factors as discussed in the lecture. The P-M equation treats canopies comprised of individual leaves as one big leaf with canopy (or surface) resistance (rc) being a measure of stomatal movement. Liquid water sitting on the surface of leaves, of course, is readily available for evaporation and wet leaves in the model should be given a surface resistance of 0. Some things to note about the model. SVP 1. You can determine the relationship (mbar) between air temperature and saturation vapour pressure (svp) and plot it here. Simply record the svp at any temperature (take 5 ºC steps from 0 ºC to 40 ºC) and plot it. You should recognize this curve as describing equilibrium evaporation. 2. Note the relative Humidity value whenever you change T or VP – it can never be allowed to exceed 100% (this will be indicated by the text turning red 10 20 30 40 in the RH textbox. 3. The questions on the worksheet are just Air temperature ( ºC) a start - you should make use of such simulation models to perform your own ‘what if?’ experiments. You can gain greater understanding of the subject by just ‘playing around’ with such models. 2 of 4 Soil, Water and Atmospheric Processes 2h Tutorial – Evaporation WORKSHEET for TUTORIAL #1 (Evaporation) Mark (out of 50) NAME (CAPITAL LETTERS) …………………… Matriculation No. …………………….. Q1. Use the model to determine the evapotranspiration rate for both dry and wet (i.e. just after rain) surfaces using the default meteorological conditions. Wet surfaces have an r s of zero. Fill in the gaps in this Table. Some values have been pre-calculated - you should be able to re-create these results to convince yourself that you are using the model correctly. Surface Bare soil Grass Cereal Coniferous forest Upland Water Evapotranspiration rate (Wm-2) Dry (use the default Wet values) ... 268 213 ... ... ... 465 157 ... ... ... [16] Q2. It has been hypothesized that the conversion of a catchment from grassland to coniferous plantation would reduce the discharge rate of the river which drained it and that the mean annual number of days of rain would be an important factor to take into account. What comments do you have on this, bearing in mind the results in the Table above? [8] Q3. Studies have shown that for surfaces like grass which are poorly coupled to the atmosphere, the humidity immediately above the canopy is higher than above a rougher canopy such as a coniferous plantation. What effect would this have on evapotranspiration from the two contrasting surfaces? [8] 3 of 4 Soil, Water and Atmospheric Processes 2h Q4. Tutorial – Evaporation The model can be used to examine the sensitivity of wet and dry grassland and wet and dry coniferous forest to solar radiation, humidity, wind speed and temperature. Do this by filling in the blanks in the Table below. You should record the difference in latent heat flux between the maximum and minimum values for each factor in turn while keeping the other factors constant. (again, some example values are included – make sure you can re-create them. You need to keep an eye on the RH value – it can never exceed 100% so you may find when you alter T or vpd that the slider need not go all the way to the minimum position!) Difference in latent heat flux (W m-2) Surface solar radiation wet grassland Dry grassland wet coniferous forest Dry coniferous forest (508-44) temperature vpd (keep air wind speed temperature fixed at default value) 464 (270-167) 103 (784-190) 594 (227-179) 48 [12] Q5. What can you conclude from these estimates? -----------End of Problems------------------- 4 of 4 [6]
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