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Infiltrometers and deriving Horton's constants

Short answer

Flooding-type infiltrometers (single/double ring) pond water and measure intake rate; rainfall-simulator types apply artificial rain and collect runoff. Horton's constants are found by plotting ln(f – f_c) vs t: f_c from final steady rate, f_0 from intercept, k from slope, e.g., f = 0.5 + 4.0 e^{-1.0t} cm/h.

Describe types of infiltrometers with sketch. How are the data of infiltrometer used to derive the Horton's constant? Explain with assumed data.

Infiltrometers are devices used to measure the infiltration rate of soil in the field. There are two types.

1. Flooding-type infiltrometers

Water is ponded on the soil, and the rate of water addition required to keep a constant depth is measured.

  • Simple (single) ring infiltrometer: a metal cylinder, 30 cm diameter and 60 cm long, driven about 50 cm into the ground. Water is kept at a constant depth (about 5 cm) and the volume added per unit time is the infiltration rate. Drawback: water spreads sideways below the ring, so the rate is over-estimated.
  • Double-ring infiltrometer: two concentric rings, inner 30 cm and outer 60 cm in diameter. Both are kept filled to the same depth. The outer ring forces the water in the inner ring to move vertically; only the inner ring is measured.
  |~~~~~|~~~~~~~~~~~~~~~~~~~~~|~~~~~|   <- water kept at the same level
  |~~~~~|~~~~~~~~~~~~~~~~~~~~~|~~~~~|      in both rings (about 5 cm)
==|=====|=====================|=====|== ground level
  |     |                     |     |
  v     v    v    v    v      v     v   water enters the soil
 outer  |<--- inner ring ---->|  outer
 ring        (measured)         ring

2. Rainfall-simulator type

Artificial rain is applied by sprinklers on a small plot (about 2 m by 4 m). Runoff is collected and measured; rainfall minus runoff gives infiltration. It represents the impact of real rain on the soil better than the flooding types.

Deriving Horton's constants

Horton's equation: f=fc+(f0−fc)e−ktf = f_c + (f_0 - f_c)e^{-kt}

Procedure:

  1. Plot ff against tt; the curve flattens to the constant fcf_c (read it from the final stable readings).
  2. Compute (f−fc)(f - f_c) for each reading and plot ln⁡(f−fc)\ln(f-f_c) against tt (or f−fcf - f_c on semi-log paper). This should be a straight line:
ln⁡(f−fc)=ln⁡(f0−fc)−kt\ln(f - f_c) = \ln(f_0 - f_c) - kt
  1. The intercept at t=0t = 0 gives f0−fcf_0 - f_c, so f0f_0. The slope of the line is −k-k.

Assumed data

Let fc=0.5f_c = 0.5 cm/h and the readings be:

t (h)0123
f (cm/h)4.52.01.00.68
f−fcf - f_c4.01.50.50.18
ln⁡(f−fc)\ln(f-f_c)1.3860.405-0.693-1.715

The points lie nearly on a straight line. Taking the two end points: slope =(−1.715−1.386)/3=−1.03= (-1.715 - 1.386)/3 = -1.03, so k≈1.0 h−1k \approx 1.0\ \text{h}^{-1}. The intercept is ln⁡(4.0)\ln(4.0), so f0=4.0+0.5=4.5f_0 = 4.0 + 0.5 = 4.5 cm/h.

Thus the fitted equation is f=0.5+4.0e−1.0tf = 0.5 + 4.0e^{-1.0t} cm/h.

✓ Answer checked by Claude Sonnet 5.5

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