Homework #8            2013, Earth Surface Processes, Humphrey

1 a) Use Manning’s equation to discuss how basal shear stress would change in a river that enters a reach that is twice as steep?  At first glance it might appear that the slope goes up, but the depth goes down, so the shear stress might not change.  Not true.  This is a hard question… a couple of hints, use depth instead of hydraulic radius in Manning’s equation, and assume the width does not change, so that the discharge (Q=v*d*w) stays constant.  Typically the width actually decreases, which increases the shear stress.

    b) Show that the Shields parameter and equation implies that otherwise similar alluvial rivers (alluvial rivers are rivers that are reworking sediment that the river itself is moving) must be steeper for coarser sediment. (Hint, write out the terms for tb and appeal to the previous question)

   c) If discharge in a river increases downriver, as is usually the case, but the sediment size in transport stays the same: what will probably happen to the river slope?

    d) Again looking at the previous parts to this question, if the river gets steeper, and the bed sediment gets coarser (as we would expect), what would be the effect of the coarse sediment on the basal shear stress (as opposed to the sediment staying the same size)?

2.     In class we used the energy in river flow, and showed that the Froude number can be interpreted as the ratio of kinetic energy to potential energy in the flow.  Many questions in river flow can be addressed by examining the total energy of the flow.  Energy, per unit width and unit length, (in other words a square meter column of water the depth of the river) of the flow can be expressed as a height of water (similar to the concept of hydraulic head in Darcy’s groundwater flow).  To be precise the energy in a column is equal to the potential energy above the bed (rgh) plus the kinetic energy (rv2/2), ‘h’ is the depth, and ‘v’ is the velocity of the water. Dividing this by density*gravity turns this into the energy head of the flow: E = h + v2/(2g)

In most river flows, by far the largest part of this energy head is just the depth of flow, with the kinetic energy only a few extra centimeters of head.  Because of this we often ignore the kinetic energy.

To get a sense for the amount of energy in river flow, we calculate several energies (expressed as water head).  Use the Laramie river in flood, with a depth of 1m, flow velocity of 1m/s, slope of 2x10-4.  Calculate:

a.    the potential energy per width, per meter length of the Laramie river (as a head).

b.    the kinetic energy of the flow (as a head)

c.    the potential energy lost by a column of water per meter of flow down river (as a head)

d.    the Froude number for the Laramie river

e.    the super elevation expected on a bend in the Laramie river (assume the bend has a radius of 20m and the width is about 4 meters).  Does this elevation of the water come from the potential energy of the flow, or the kinetic energy?

f.     Extensive high Froude number flow (shooting flow) is relatively rare and usually only found in steep bedrock rivers.  Calculate the velocity that would be needed in the Laramie river to achieve super critical flow.

g.    (hard, mini puzzle) Assuming the discharge, width and the roughness stay the same, how steep would the Laramie river have to be to reach a Fr of 1?

3.    While we are talking about energy: energy is expended by a column of river water to move the load of sediment.  Analyzing this is very difficult to do correctly, but we can approximate the energy by saying that the water flow has to counteract the settling velocity.  We will make several assumptions: the only sediment in transport is sand (0.2mm), and the amount in transport (mass qsed) is 0.1kilograms/(m*s).  Remember, energy is Force * distance.  Force is easy; it is the weight of the sediment, distance is less obvious, but think of the settling velocity of the sand.

Compare the energy to move the sediment with the energy of the flow from ‘c’ above.

4.   If a minor flood occurs in the Upper Yellowstone and Missouri drainage, how long will it take for that kinematic flood wave take to reach New Orleans? You should use several locations down the river system to get the relevant data.  Dams, of course will totally change this, however, try to get an estimate as if the dams weren’t there.  This would give an idea of how quickly floods used to drain from the continent, while current floods take much longer.

 5  We talked about the logarithmic velocity profile that develops above a rough bed.  An equation that works for rivers such as the Laramie river is:  v(z)  = 2.5 v* ln(z/D84) + 8.5,  where the D84  can be considered the size of the roughness particles on the bed (pea gravel), but is technically the 2 sigma size of the coarse tail of sediment distribution on the bed.  Note, particle roughness and depth have to measured in the same units,  and that the velocity is in cm/sec.  Apply this to the Laramie river, and compare with your estimate from your homework, and with the velocity obtained from Mannings equation.

6  Rivers are mainly transporting mechanisms for moving sediment from the hillslope sources to the lake and ocean sinks.  To illustrate this, try to get an estimate of the percentage of the land in the US that is actually overlain by flowing water (creeks rivers etc.).  I have never tried this question before, see what you can find out.