This shows you the differences between two versions of the page.
| Both sides previous revision Previous revision | |||
|
students_summer2026 [2026/06/01 12:31] trinh |
students_summer2026 [2026/06/01 12:47] (current) trinh |
||
|---|---|---|---|
| Line 21: | Line 21: | ||
| Chapter 20 covers an introduction to the basic model (though focussing on a special model known as the Probability Distributed Model). It is pitched at the audience of an undergraduate Engineering course (actually this is delivered as a fourth-year or MSc-level year), but it is generally not too sophisticated and can be understood with some help. I like how there is a little Matlab script to try. | Chapter 20 covers an introduction to the basic model (though focussing on a special model known as the Probability Distributed Model). It is pitched at the audience of an undergraduate Engineering course (actually this is delivered as a fourth-year or MSc-level year), but it is generally not too sophisticated and can be understood with some help. I like how there is a little Matlab script to try. | ||
| + | |||
| + | The initial model that is used in that chapter is as simple as this [from (20.7)]: | ||
| + | $$ | ||
| + | \frac{dS}{dt} = q_p - E_a - q_s, | ||
| + | $$ | ||
| + | where the goal is to solve for the storage $S = S(t)$. | ||
| + | |||
| + | To do this, you take in precipitation rate, $q_p$ (provided by data), the actual evapotranspiration rate $E_a$, given by [eqn (20.11)]: | ||
| + | $$ | ||
| + | E_a = H(S) E_p, | ||
| + | $$ | ||
| + | where $E_p$ is a potential evapotranspiration rate (provided by data), and $H$ is a Heaviside function, which is $1$ if $S > 0$ and zero otherwise. Finally, the runoff, $q_s$, is the key quantity to be obtained, which is modelled by: | ||
| + | $$ | ||
| + | q_s = H(S - c) q_p. | ||
| + | $$ | ||
| + | In other words, if the storage $S$ inceeds some capacity, $c$, all of the rain $q_p$ goes into runoff. In theory, $c$ is chosen by calibration, | ||
| + | |||
| + | {{ : | ||
| + | |||
| + | You can read in that chapter why this is a poor model and how it is then improved. | ||
| + | |||
| + | ==== Getting the right answers for the right reasons ==== | ||
| + | |||
| + | The next reference I want to provide is just a general review of the state of hydrology given by James Kirchner in 2006: | ||
| + | |||
| + | //Kirchner, J. W. (2006). Getting the right answers for the right reasons: Linking measurements, | ||
| + | // | ||
| + | |||
| + | There is not much to add to this. I think it is a nice article to begin to understand why model differentiation and complexity are difficult topics in the area of hydrology. | ||
| + | |||
| + | ==== A workshop on hydrological modelling ==== | ||
| + | |||
| + | The last reference I want to share is this one: | ||
| + | |||
| + | //Knoben, W. J. M., & Spieler, D. (2022). Teaching hydrological modelling: Illustrating model structure uncertainty with a ready-to-use computational exercise. Hydrology and Earth System Sciences, 26(12), 3299–3314. https:// | ||
| + | // | ||
| + | |||
| + | In this article, they discuss how a teaching exercise was designed to investigate some issues of hydrological modelling and uncertainty. The toolbox here is the excellent [[https:// | ||
| + | |||
| + | As part of your investigations, | ||