globals [step time dt L var xbar scale truescale xnewmax xnewmin xnewbar histscale axmin axmax histbars Kx_theory Kx_actual] patches-own [vel] turtles-own [ xc ; unwrapped xcor yc ; unwrapped ycor delx dely xnew Gauss Gx localvel ; local velocity ] to setup ca crt 1000 ask turtles [ set color yellow set heading 90 set xcor -1 * screen-edge-x set xnew -1.0 * screen-edge-x ] ;ask turtle 10 [set color green] if line [ ask turtles with [ who <= 500 ] [ set ycor random (screen-edge-y - 0.5) ] ask turtles with [ who > 500 ] [ set ycor random -1.0 * (screen-edge-y - 0.5)] ] ask turtles [ set yc ycor ] set scale 1 set truescale 1 set axmin 0 set axmax 2 * screen-edge-x set dt 0.5 ;L ^ 2 / 200 ;set U_o 1 set L (screen-edge-y - 0.5) set Kx_theory 8 / 945 * U_o ^ 2 * L ^ 2 / D_y grid-setup end to grid-setup ask patches [ set vel U_o * (1 - (pycor / (screen-edge-y - 0.5) ) ^ 2) set pcolor scale-color blue vel (1.4 * U_o) 0 ] ask patches with [abs pycor = screen-edge-y] [set pcolor red] end to go move-turtles set step step + 1 set time time + dt set var variance values-from turtles [xc] set xbar mean values-from turtles [xc] set Kx_actual 1 / 2 * var / time set-current-plot "Growth of Tracer Variance" set-current-plot-pen "theory" plotxy time 2 * 8 / 945 * U_o ^ 2 * L ^ 2 / D_y * (step * dt) set-current-plot-pen "actual" plotxy time var if (step mod 30 = 1) [ set-current-plot "Histogram" clear-plot set histscale (max values-from turtles [xc] - min values-from turtles [xc]) / (max values-from turtles [xcor] - min values-from turtles [xcor]) set axmin min values-from turtles [xc] - (min values-from turtles [xcor] + screen-edge-x) * histscale set axmin round axmin set axmax max values-from turtles [xc] + (screen-edge-x - max values-from turtles [xcor]) * histscale set axmax round axmax set-plot-x-range axmin axmax set-histogram-num-bars 50 histogram turtles [xc] set-current-plot "Tracer Concentration Profile vs. Gaussian" clear-plot set-plot-x-range axmin axmax set-current-plot-pen "C(x)" set histbars 70 set-histogram-num-bars histbars histogram turtles [xc] set-current-plot-pen "Gauss" ask turtles [ set Gx axmin + who * (axmax - axmin) / 999 set Gauss 1000 * (axmax - axmin) / histbars / sqrt (2 * pi * var) * exp ( -1 * (Gx - xbar) ^ 2 / (2 * var) ) plotxy Gx Gauss ] ] end to move-turtles ask turtles [set localvel vel-of patch-here set delx localvel * dt set dely sqrt( 2 * D_y * dt) * (random-normal 0 1) bound-reflect set xc xc + delx set yc yc + dely set ycor yc set xnew xnew + delx * truescale ] set xnewmax max values-from turtles [xnew] set xnewmin min values-from turtles [xnew] set xnewbar mean values-from turtles [xnew] if (xnewmax > screen-edge-x) [ set scale min list 1 (0.67 * screen-edge-x / ( xnewmax - xnewmin )) ask turtles [ set xnew scale * xnew - screen-edge-x - scale * xnewmin ] set truescale truescale * scale ] ask turtles [set xcor xnew] end to bound-reflect if ( pcolor-of (patch-at delx dely) = red) [ set dely dely - 2 * ( yc + dely - ( L * abs pycor-of patch-at delx dely / pycor-of patch-at delx dely ) ) ] end ; add model procedures here @#$#@#$#@ GRAPHICS-WINDOW 32 17 965 239 50 10 9.14 1 10 0 0 CC-WINDOW 3 628 265 820 Command Center BUTTON 6 366 73 399 NIL setup NIL 1 T OBSERVER BUTTON 74 366 137 399 NIL go T 1 T OBSERVER SLIDER 5 420 179 453 D_y D_y 0.01 1 0.01 0.01 1 NIL PLOT 707 413 1000 628 Growth of Tracer Variance time Tracer Variance 0.0 100.0 0.0 100.0 true true PENS "actual" 1.0 2 -65536 true "theory" 1.0 0 -16777216 true PLOT 4 241 1004 361 Histogram x N -1000.0 1000.0 0.0 100.0 true false PENS "N" 1.0 1 -16777216 true MONITOR 707 363 791 412 NIL time 2 1 SWITCH 211 417 314 450 line line 0 1 -1000 MONITOR 469 362 536 411 NIL xbar 2 1 PLOT 352 413 690 628 Tracer Concentration Profile vs. Gaussian x C(x) 0.0 100.0 0.0 100.0 true true PENS "C(x)" 1.0 0 -65536 true "Gauss" 1.0 0 -16777216 true SLIDER 5 457 177 490 U_o U_o 1 100 1 1 1 NIL MONITOR 795 363 869 412 NIL Kx_theory 2 1 MONITOR 873 363 947 412 NIL Kx_actual 2 1 @#$#@#$#@ WHAT IS IT? ----------- This is a model of shear dispersion. It simulates the release of a passive tracer into a channel of width B with a longitudinal velocity profile U(y). The individual tracer particles (think of them as molecules) advect with the current at the same time as they undergo a random diffusion process in the y-direction. The combination of transverse diffusion and "differential advection" gives rise to a longitudinal dispersion process that follows Fick's Law. This means that the tracer concentration profile in the longitudinal direction is Gaussian and longitudinal variance grows linearly with time, after an initial transient period. HOW IT WORKS ------------ The user first initiates the trace molecules by pressing the "setup" button. This action releases the molecules in a transverse line at x = 0. Pressing the "Go" button then starts the simulation. Prior to starting the simulation, the user may use the slider buttons to vary the values of U, the longitudinal velocity along the channel centerline, and Dy, the trasverse diffusion constant. The transverse-dependence of the velocity, U(y) is visually represented by the color variation of the channel (dark blue is the maximum velocity, near the channel centerline, while white corresponds to zero velocity at the edges). The red lines are the solid channel boundaries, which tracer molecules are prohibited from crossing. The triangles represent the tracer particles. Once the simulation has begun, the motion of the tracer can be monitored by watching the particles move within the colored channel. In addition, the behavior of the tracer is shown by the three plots entitles "Histogram", "Tracer Concentration Profile vs. Gaussian", and "Growth of Tracer Variance". The histogram plot shows a histogram of the locations of all tracer particles with time. Note that the x axis changes with time, as the tracer becomes more and more spread out. The next plot compares the tracer concentration profile to an ideal Gaussian curve. When the Fickian dispersion regime has been reached, the tracer curve should closely resemble a Gaussian. The last curve shows the growth of the tracer variance with time, and compares it with the prediction based on Fickian dispersion theory. Note that when the slope of the line from the simulation matches the slope of the ideal linear curve, the Fickian regime has been reached. THINGS TO NOTICE ---------------- Notice that the higher the value of Dy, the faster the particles move in the transverse direction. Note that the time necessary to reach the Fickian dispersion regime depends on the values of U and Dy. See if you can determine this dependence through some combination of scaling and simulation. Try varying the values of Dy and for each run, note the time at which you think Fickian dispersion has begun (Gaussian concentration profile and/or linear growth of tracer variance). THINGS TO TRY ------------- This section could give some ideas of things for the user to try to do (move sliders, switches, etc.) with the model. EXTENDING THE MODEL ------------------- This section could give some ideas of things to add or change in the procedures tab to make the model more complicated, detailed, accurate, etc. NETLOGO FEATURES ---------------- This section could point out any especially interesting or unusual features of NetLogo that the model makes use of, particularly in the Procedures tab. It might also point out places where workarounds were needed because of missing features. RELATED MODELS -------------- This section could give the names of models in the NetLogo Models Library or elsewhere which are of related interest. 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