Title: Modelling Environmental Processes An illustration
1Modelling Environmental ProcessesAn illustration
- Dr Ian Renfrew
- Environmental Sciences
2Overview
- The aim of this course is to show how
environmental problems may be solved from the
initial problem, to mathematical formulation and
numerical solution. - The course consists of lectures on numerical
methods and computing practicals. Both are
extremely important, i.e. compulsory! - The computing practicals will be run in Matlab.
- The unit will guide students through the solution
of a geophysical problem of their own choosing. - The problem will be discussed and placed into
context through an essay, and then solved and
written up in a project report. A taught
practical is also assessed.
3Background
- For UG ENV 2A21 and 2A22
- For MSc
- Some computer programming (any language)
- Some understanding of calculus, in particular
differential equations
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5Learning outcomes
- Start with a geophysical phenomenon
- Determine the key physical/chemical processes
- Literature review, text books, observations,
laboratory experiments, etc - Express the key processes in terms of
mathematical equations - Formulate a numerical solution to these equations
- Write a computer program to solve the numerical
equations - Test, view and analyse the results discuss their
significance
6An illustration
- A research-led geophysical problem
- Modelling the flow of cold-air off an ice shelf
and over a polynya (a persistent area of open
water within the sea ice) - The model is documented in detail in
- Renfrew, I. A. and J. C. King, 2000 A simple
model of the convective internal boundary layer
and its application to surface heat flux
estimates within polynyas, Boundary-Layer
Meteorology, 94, 335-356. - Model then applied to an area in the Southern
Weddell Sea, where coastal polynyas are common - Renfrew, I. A., J. C. King, and T. Markus, 2002
Coastal polynyas in the southern Weddell Sea
variability of the surface energy budget, J.
Geophys. Res. (Oceans), 107 (C6), 3063, doi
10.1029/2000JC000720.
7Coastal air-sea-ice interaction
8Polynyas and Leads
9Why is this important?
- Atmosphere-Ocean heat exchange around Antarctica
are key part of the oceans thermohaline
circulation. - In winter, most heat exchange is thought to take
place through polynyas and leads (sea ice acts to
insulate the ocean) - Need to quantify this heat exchange
10How to quantify the heat exchange?
- Estimate the surface sensible heat flux, surface
latent heat flux and the radiative fluxes. - To use standard bulk formulae for the fluxes we
need to know near-surface air temperature, wind,
relative humidity, and the sea surface
temperature.
11The surface energy budget
- QsQl Qr QpQo Qtot pi Lf F
- where
- Qs sensible heat flux
- Ql latent heat flux
- Qr net radiative flux
- Qp heat flux from precipation
- Qo upward heat flux from the ocean
- and
- pi is the density of ice, Lf the latent heat of
fusion, and - F an ice production rate.
12The surface energy budget
- Surface sensible and latent heat fluxes can be
calculated - Qs CH ?cp U10 (?SST ?m)
- Ql CE ? cp U10 (qsat qa)
- where
- U10 is the wind speed at 10 m
- ?SST and ?m are the potential temperatures at
the sea surface and in the atmosphere - qa is the specific humidity
- qsat is the saturated specific humidity at ?SST
- and CH CE are exchange coefficients.
13What are the key physical processes?
14What are the key physical processes?
- Cold air flowing off a cold ice surface over a
warm ocean surface - upstream air is stable
- flux of heat from ocean into boundary-layer
atmosphere - this will cause an unstable surface-layer which
will convectively mix upwards through the
boundary layer - after convective mixing the boundary-layer ?
will be constant with height - a mixed-layer boundary-layer model seems
appropriate
15What are the key physical processes?
what about upstream temperature profile? 1st
order importance use climatological
information mixing of heat from above? 2nd order
importance but easily encorporated changes in
surface roughness ice to water? 2nd order
importance changes in wind speed? 2nd order
importance literature was ambiguous development
of clouds? 2nd order importance not simple to
model changes in relative humidity? 3nd order
importance qa mainly determined by temp.
16A Convective Internal Boundary-Layer model
Parameters set from climatology ?? stability
- piecewise linear profile hsl initial CIBL
height ß entrainment ratio
- Variables
- U10 constant with x (c.f. literature review)
- ?SST constant with x (ok over 10s km)
- h(x) CIBL height will increase with distance
- ?m(x) will warm with distance
- qa(x) will increase as ?m increases
- Thus Qs and Ql will change with x
17Literature review
- Garratt, JR, 1992 The atmospheric boundary
layer, Cambridge University Press, page 154 - Outlines simple mixed-layer models,
- When temperature is constant with x then an
analytic solution is possible (given certain
assumptions) - h Cx1/2, where C is a constant and typically
C(stability,Um,Qs, entrainment) - In our situation, with ?m(x) and Qs(x) an
analytic solution is not possible - Devised an iterative solution to the numerical
equations.
18Model equations
19Model equations
20Model equations
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22Numerical Solution
The model equation set (9), (10) and (11) are
solved by numerical integration, and an iteration
scheme where 1. Hs(xi) is calculated via (11),
using ?m(xi-1) as a first guess. 2. Equations (9)
and (10) are solved for ?m(xi) and h(xi). 3.
?m(xi) is then used to give a revised estimate of
Hs(xi). Steps 2 and 3 are repeated until h
converges to within a defined criteria (set as
one metre), which usually required only two
iterations. The accuracy of the numerical
integration can be checked by comparing Hs from
the bulk formula and as calculated from Equations
(7) and (8) they typically agreed to within 2 W
m-2. The numerical solution outlined here is
rapid enough for climatological use.
23Matlab code
- I have put a simplified version of the CIBL model
code on my website http//lgmacweb.env.uea.ac.uk/e
046/teaching/teaching.htm - cbl_growth_gm.m main code
- Sets up parameters and input variables
- Grows CIBL for successive values of x
- Simple numerical integration to solve equations
(9) (10) - Iteration routine to assure convergence
- Simplified model uses a constant heat flux
coefficient - cbl_plot_gm.m plotting code
- Simplified for just model solution, no validation
data - thermo_rh.m thermodynamics variable function
24Results for a typical cold air outbreak
25Results for 4 February 1997 off the Ronne Ice
Shelf, Antarctica Input data are from an
automatic weather station on the ice
shelf. Validation data are from radiosondes ()
and ship-borne observations (o).
Visible satellite image of Ronne Ice Shelf and
southern Weddell Sea 4 February 1997
26Results for 4 February 1997 off the Ronne Ice
Shelf, Antarctica Input data are from an
automatic weather station on the ice
shelf. Validation data are from radiosondes ()
and ship-borne observations (o).
27Input data from upstream weather
station. Validation data from instrumented
aircraft. Systematic differences are due to CIBL
model limitations. For example, a previous CIBL
development and the development of clouds with
fetch. Note (o) plot total heating fluxes,
while () plot turbulent heat flux convergence
only (i.e. the heating that we model).
28Relevance to Modelling Env Processes
- My illustration was original research that led
to a publication, your course projects should not
be as complicated or as lengthy!
29Relevance to Modelling Env Proceses
- The basic principles should be the same
- Determine your geophysical problem
- Simplify to something tractable
- Devise a mathematical model
- Develop a numerical model
- Examine solutions within parameter space
- Discuss their significance
- The first three should be covered in essay
- The whole project covered by the final report