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Chapter 14 - Limitations on Predictive Modeling in Geomorphology ...

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LIMITATIONS ON PREDICTIVE MODELING 339<br />

Bedload transport is an example of a specific process that has been studied extensively<br />

<strong>in</strong> the laboratory and that also plays an important role <strong>in</strong> the evoluti<strong>on</strong> of many<br />

geomorphic systems. Over a period of many decades, small-scale experiments <strong>in</strong> flumes<br />

have been carried out and semiempirical and empirical models developed and ref<strong>in</strong>ed <strong>on</strong><br />

the basis of those experiments (ASCE 1975). These models reflect properties such as gra<strong>in</strong><br />

size and surface slope that are underly<strong>in</strong>g determ<strong>in</strong>ants of the physical behavior of the<br />

system. For example, the Meyer-Peter formula can be written (Meyer-Peter and Muller<br />

1948) (<strong>in</strong> SI units) as<br />

2/ 3<br />

q<br />

d<br />

50<br />

S qs<br />

= 17 + 0.4<br />

d<br />

where q s and q are, respectively, sediment and water discharge <strong>in</strong> kg m -1 s -1 , S is the local<br />

slope, and d 50 is the median gra<strong>in</strong> size of the bed material <strong>in</strong> meters. Other models or<br />

'formulas' are expressed directly <strong>in</strong> terms of bed shear stress. Although empirical, these<br />

expressi<strong>on</strong>s are derived from experiments where the <strong>in</strong>dependent variables are<br />

well-c<strong>on</strong>trolled. The form of these equati<strong>on</strong>s is therefore directly c<strong>on</strong>nected to measured<br />

physical behavior under specific experimental c<strong>on</strong>diti<strong>on</strong>s. Figure <str<strong>on</strong>g>14</str<strong>on</strong>g>.1 shows the tightly<br />

clustered experimental results up<strong>on</strong> which the Meyer-Peter formula is based.<br />

When the predicti<strong>on</strong>s of formulae due to different authors are compared, however,<br />

agreement between them is typically poor. Figure <str<strong>on</strong>g>14</str<strong>on</strong>g>.2 shows predicti<strong>on</strong>s of bedload<br />

transport rates based up<strong>on</strong> a number of well-known transport equati<strong>on</strong>s. These curves<br />

were derived under diverse experimental c<strong>on</strong>diti<strong>on</strong>s, and experimental variability may<br />

account for some of the differences <strong>in</strong> predicti<strong>on</strong> shown <strong>in</strong> the figure. However, the<br />

transport equati<strong>on</strong>s illustrated are <strong>in</strong>tended to be applicable for a range of gra<strong>in</strong> sizes from<br />

medium sand to granules. It thus seems fair to make a general comparis<strong>on</strong>, as shown <strong>in</strong><br />

Figure <str<strong>on</strong>g>14</str<strong>on</strong>g>.2, of the transport rates predicted by these equati<strong>on</strong>s. This comparis<strong>on</strong> is based<br />

up<strong>on</strong> results of a comprehensive review of sedimentati<strong>on</strong> sp<strong>on</strong>sored by the American<br />

Society of Civil eng<strong>in</strong>eers (ASCE 1975). Variati<strong>on</strong> over several orders of magnitude<br />

between predicti<strong>on</strong>s for different models suggests that applicati<strong>on</strong> of such formulas to<br />

large-scale geomorphic systems, where local c<strong>on</strong>diti<strong>on</strong>s are often poorly known, will<br />

result <strong>in</strong> significant uncerta<strong>in</strong>ty.<br />

In fluvial problems, empirical rat<strong>in</strong>g curves that bypass any reference to important<br />

underly<strong>in</strong>g physical variables (gra<strong>in</strong> size, shear stress, etc.) have often been used <strong>in</strong><br />

practice. River transport of suspended and c<strong>on</strong>tact load can be described by power-law<br />

rat<strong>in</strong>g curves that relate transport rate to total discharge (ASCE 1975; Richards 1982).<br />

Rat<strong>in</strong>g curves are also comm<strong>on</strong>ly used to estimate reservoir sedimentati<strong>on</strong> (S<strong>in</strong>gh and<br />

Durgunoglu 1992) and soil erosi<strong>on</strong> (Wischmeier 1976). Such rat<strong>in</strong>g curves do not reflect<br />

underly<strong>in</strong>g small-scale properties of sediment transport, but are keyed to measurable<br />

large-scale properties such as total discharge and average slope.<br />

These examples reflect eng<strong>in</strong>eer<strong>in</strong>g attempts to make predicti<strong>on</strong>s of geomorphic<br />

processes. Such attempts may seem crude by the standards of scientific geomorphology,<br />

but geomorphic predicti<strong>on</strong> is <strong>in</strong> practice nearly always based <strong>on</strong> empiricism. This is partly<br />

due to immaturity of the scientific basis of geomorphology, but it also reflects the fact that<br />

complex systems such as those characteristic of geomorphology tend to be resistant to<br />

reducti<strong>on</strong>ism. Because of its overwhelm<strong>in</strong>g success <strong>in</strong> physics, <strong>on</strong>e is accustomed to<br />

2 / 3<br />

50<br />

,

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