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Slope-Velocity-
Equilibrium and
evolution of surface
roughness on stony
hillslopes
MARK A. NEARING1, VIKTOR O. POLYAKOV1, MARY
H. NICHOLS1, MARIANO HERNANDEZ1, LI LI2, YING
ZHAO2, GERARDO ARMENDARIZ1
1USDA-AGRICULTURAL RESEARCH SERVICE, SOUTHWEST WATERSHED
RESEARCH CENTER, TUCSON, AZ, 85719, USA
2SCHOOL OF NATURAL RESOURCES AND THE ENVIRONMENT, UNIVERSITY OF
ARIZONA, TUCSON, AZ, 85705, USA
13 Years Rainfall Simulation
on western rangeland
What is the source
of velocity variability?
1. Runoff
272 experiments,
23 sites
Velocity vs. Runoff
coded by slope
Velocity vs. Runoff
coded by ground cover
R-
Square
Variables in
Model
R-
Square
Variables in
Model
0.4120 runoff 0.0864 foliar grass
0.2909 litter 0.0593 foliar shrub
0.2439 ground cover
total
0.0488 foliar total
0.1831 basal gap
fraction
0.0225 basal
0.1625 basal gap av.
length
0.0049 canopy gap av.
length
0.1484 rock 0.0025 slope
0.1079 canopy gap
fraction
0.0010 foliar forbs
𝑽 =
𝟏
𝒏
𝑹 𝟐/πŸ‘
𝑺 𝟏/𝟐
𝑽 = π‘ͺ(𝑹𝑺) 𝟏/𝟐
Slope-Velocity-Equilibrium
is a state of a soil surface that:
1. evolves naturally over time due to the
interaction between overland flow and surface
morphology,
2. wherein steeper areas develop a relative
increase in physical and hydraulic roughness
3. such that flow velocity is a function of
overland flow rate independent of slope
gradient.
Methods:
1. Artificial rainfall was applied to 2m by 6m plots
at 5%, 12%, and 20% slope gradients.
2. Measurements of runoff rate, velocity, rock
cover, and surface roughness.
Hypothesis:
Velocities measured at the end of each
experiment were a unique function of discharge
rates, independent of slope gradient or rainfall
intensity.
Velocity with Dye and Salt
Rock Cover by size
Plot-average rock cover (>0.5 cm) as a
function of cumulative runoff for the 6
experiments.
Flow velocities down the full
plot as a function of
cumulative runoff depth for:
a) I=59 mm hr-1, and b) I=178
mm hr-1.
Final flow velocities for all 6 experiments at each of the three velocity
transect measurement transects and two rainfall rates.
𝑽 =
𝟏
𝒏
𝑹 𝟐/πŸ‘
𝑺 𝟏/𝟐
𝑽 = π‘ͺ(𝑹𝑺) 𝟏/𝟐
V = 26.39 q0.696 (r2 = 0.95, n = 36)
β€’ This study supports the hypothesis of slope-velocity-
equilibrium
β€’ Physical surface roughness was greater at steeper slopes.
β€’ Hydraulic roughness was greater at steeper slopes.
β€’ Velocities measured at the end of each experiment were a
unique function of discharge rates, independent of slope
gradient or rainfall intensity.
β€’ Hydraulic equations, such as Chezy and Manning, in
hillslope scale runoff models are problematic because the
coefficients vary with slope and rainfall intensity.
The long drive home

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Slope velocity-equilibrium and evolution of surface roughness

  • 1. Slope-Velocity- Equilibrium and evolution of surface roughness on stony hillslopes MARK A. NEARING1, VIKTOR O. POLYAKOV1, MARY H. NICHOLS1, MARIANO HERNANDEZ1, LI LI2, YING ZHAO2, GERARDO ARMENDARIZ1 1USDA-AGRICULTURAL RESEARCH SERVICE, SOUTHWEST WATERSHED RESEARCH CENTER, TUCSON, AZ, 85719, USA 2SCHOOL OF NATURAL RESOURCES AND THE ENVIRONMENT, UNIVERSITY OF ARIZONA, TUCSON, AZ, 85705, USA
  • 2. 13 Years Rainfall Simulation on western rangeland What is the source of velocity variability? 1. Runoff 272 experiments, 23 sites
  • 4. Velocity vs. Runoff coded by ground cover
  • 5. R- Square Variables in Model R- Square Variables in Model 0.4120 runoff 0.0864 foliar grass 0.2909 litter 0.0593 foliar shrub 0.2439 ground cover total 0.0488 foliar total 0.1831 basal gap fraction 0.0225 basal 0.1625 basal gap av. length 0.0049 canopy gap av. length 0.1484 rock 0.0025 slope 0.1079 canopy gap fraction 0.0010 foliar forbs
  • 6. 𝑽 = 𝟏 𝒏 𝑹 𝟐/πŸ‘ 𝑺 𝟏/𝟐 𝑽 = π‘ͺ(𝑹𝑺) 𝟏/𝟐
  • 7. Slope-Velocity-Equilibrium is a state of a soil surface that: 1. evolves naturally over time due to the interaction between overland flow and surface morphology, 2. wherein steeper areas develop a relative increase in physical and hydraulic roughness 3. such that flow velocity is a function of overland flow rate independent of slope gradient.
  • 8. Methods: 1. Artificial rainfall was applied to 2m by 6m plots at 5%, 12%, and 20% slope gradients. 2. Measurements of runoff rate, velocity, rock cover, and surface roughness. Hypothesis: Velocities measured at the end of each experiment were a unique function of discharge rates, independent of slope gradient or rainfall intensity.
  • 9.
  • 10.
  • 11. Velocity with Dye and Salt Rock Cover by size
  • 12. Plot-average rock cover (>0.5 cm) as a function of cumulative runoff for the 6 experiments.
  • 13. Flow velocities down the full plot as a function of cumulative runoff depth for: a) I=59 mm hr-1, and b) I=178 mm hr-1.
  • 14. Final flow velocities for all 6 experiments at each of the three velocity transect measurement transects and two rainfall rates.
  • 15. 𝑽 = 𝟏 𝒏 𝑹 𝟐/πŸ‘ 𝑺 𝟏/𝟐 𝑽 = π‘ͺ(𝑹𝑺) 𝟏/𝟐 V = 26.39 q0.696 (r2 = 0.95, n = 36)
  • 16. β€’ This study supports the hypothesis of slope-velocity- equilibrium β€’ Physical surface roughness was greater at steeper slopes. β€’ Hydraulic roughness was greater at steeper slopes. β€’ Velocities measured at the end of each experiment were a unique function of discharge rates, independent of slope gradient or rainfall intensity. β€’ Hydraulic equations, such as Chezy and Manning, in hillslope scale runoff models are problematic because the coefficients vary with slope and rainfall intensity.