During the past week I have run some initial 'unconstrained' simulations of the entire 59-mile MNRR segment, using the circumferential speed method (which is the unmodified 'sigma' in JP), Johannesson-Parker implementation 3, and two prototype variable-width methods. The second variable-width method, based on sediment uptake and loss from water flowing above or below a critical speed, did not perform well in the short time I devoted to it, and is not shown here. Nor did I try a braided-river meandering method, also due to time constraints. I would like to save the variable-width and braided meandering methods for next month, if time permits, or for the followup project, if it occurs. Although these are both interesting and worthwhile lines of pursuit, they are not strictly germane to the current project. For the remainder of this project, I suggest that we restrict ourselves to fixed-width meandering methods, using either an average-width river as input (in the case of JP), or the actual-width river, in the case of circumferential speed. The examples shown below should make this recommendation clearer.
Here is the initial average-width (747.84 m) river:
Here is the initial actual-width (186.79 to 1647.97 m) river:
Here are the end results of 100 yr simulations (dt = 0.1) using several methods and input parameters. Migration rates were adjusted so that the initial erosion was on the order of 1 ha/yr/km (as quoted in EJ2006). All plots are shown at the same scale:
method = circumferential speed (sigma) width = 747.84 flow = 899.33 depth = 3.429 ldist = 0.5 widths sdist = 1.0 width mrate = 200.0 mexp = 1.0
method = circumferential speed (sigma) width = actual flow = 899.33 depth = 3.429 ldist = 0.5 widths sdist = 1.0 width mrate = 200.0 mexp = 1.0
method = JP3 width = 747.84 flow = 899.33 depth = 3.429 slope = 1.918e-04 diam = 0.001 mrate = 2.0 mexp = 1.0
method = JP3 width = 400.0 flow = 899.33 depth = 3.429 slope = 1.918e-04 diam = 0.001 mrate = 20.0 mexp = 1.0
method = JP3 width = 200.0 flow = 899.33 depth = 3.429 slope = 1.918e-04 diam = 0.001 mrate = 40.0 mexp = 1.0
method = variable width speed (sigma) width = 747.84 flow = 899.33 depth = 3.429 ldist = 0.5 sdist = 1.0 mrate = 140.0 mexp = 1.5
method = variable width speed (sigma) width = actual flow = 899.33 depth = 3.429 ldist = 0.5 sdist = 1.0 mrate = 100.0 mexp = 1.5
As you can see, there is quite a bit of variation in the results, although it is variation 'on a theme'. Even in 100 years, the simulation does not become 'unbounded'. The planform is clearly finite, and the river stays fairly close to its original position. And yet none of these simulations captured the essence of what I had hoped to achieve: the dynamic 'wildness' of the unmanaged river of over 100 years ago. I was hoping, in the unconstrained simulations, to get something that looked like the 1895 maps:
including the long, open loops near Vermillion and Sioux City. So far, the 'wildest' simulation I have done is the following:
method = circumferential speed (sigma) width = actual flow = 899.33 depth = 3.429 ldist = 1.0 widths sdist = 2.0 widths mrate = 1000.0 mexp = 1.5
My schedule for the next several months is:
July
August
September-October
November-December