Title: Why do moisture convergence deep convection schemes work for more scales than those they were in principle designed for?
1Why do moisture convergence deep convection
schemes work for more scales than those they were
in principle designed for?
- Jean-François Geleyn
- ONPP/CHMÚ CNRM/Météo-France
- (on an incentive from Philippe Bougeault and
using ideas - of Brian Mapes() and Jean-Marcel Piriou)
- CCWS, Tartu, Estonia, 24-1-2005
- () in The physics and parameterisation of moist
atmospheric convection, pp.321-358, NATO ASI
Series, 1997, Kluwer Academic Publishers,
Dordrecht
2P. Bougeault (pers. com. - 12/1/04)
- I was well conscious about this limitation (of
the moisture convergence closure) in 85, but the
problem is that I mostly wanted to fit GATE data,
where there is no correlation between CAPE and
rainfall, while there is a strong correlation
between MOCON and rainfall. But, as Mapes
rightly says, the latter does not guarantee a
causal link because one might mix cause and
consequence. - But, since it works on this basis at Meteo-France
as well as at ECMWF for 20 years, this cannot be
that wrong either!
3Why is deep-convection so special in the
parameterisation trade?
- Because such a parameterisation automatically
requires some knowledge of the models resolved
tendencies (closure problem). - Because it is a non-hydrostatic phenomenon that
we try to parameterise in a hydrostatic-type
framework (for the scales -above 10km- where we
need such a parameterisation). - Because the basic atmospheric state always looks
at the edge of a yes/no behaviour. - Because visible convection appears like a local
auto-organised process while its invisible
influence and conditions of existence are very
much of a large-scale type.
4Why do we need a parameterisation of
deep-convection?
- Because for models that do not resolve the 10km
scale, associated clouds are clearly sub-grid and
look like the result of an auto-organisation
process. - Because without it, resolved microphysics of
clouds and precipitation takes over the vertical
stabilising role, but at the wrong scale with
sometimes catastrophic consequences on the
modelled atmosphere. - Not because it helps maintaining the correct
local vertical gradients of temperature and
humidity but because it controls the intensity of
larger-scale dynamical adjustment motions (Hadley
cell, ).
5Convective instability is a local property
Conditional instability of the first kind
6The mass-flux approach
- Hypotheses
- steady cloud
- negligible updraft area
7The mass-flux approach (Bougeaults 1985 variant)
8The CISK vs. WISHE controversy
Static view (there is also a wave-propagation
equivalent)
Conditional Instability of the Second Kind
Wind Induced Surface Heat Exchange
9The CISK vs. WISHE main difference
But the truth seems to be situation- and scale
dependent !
10The Quasi-Equilibrium (QE) concept history
- Whatever causality is at work, QE is verified at
very large scale, but not necessarily below. - Study of the phenomenology of convection pushed
to the concept of mass-flux formulation for
convective parameterisation schemes. - This shifted the old problem of convective
closure from budgets to complex questions about
the dynamics of convective circulations. - But the (misleading?) answer was to replace the
search of an additional convective impact under
given local circumstances by that of a full
convective answer to a non-convective forcing.
11The Quasi-Equilibrium (QE) concept controversy
- CISK idea of QE convective circulations are
determining the larger scale vertical
velocities that in turn force convection. - WISHE idea of QE being in a lift, you are not
going up because the counter-weight goes down. - Anti-QE thinking (20 years lost, they say)
- Scales are not separable (the invisible part
of convection is at the scale of the Rossby
radius of deformation) - Forcing and answer are not really separable
either (at least scale-dependent in a model where
the return flow must be accounted for in the same
grid-box)! - There is no under-law of convective regions
dynamics that aggregates local behaviours to a
simple balance.
12QE and causality. Le Châteliers principle as an
answer? (1/2)
- Chemical reactions QE if the modification of
some parameters does displace the equilibrium,
other forces counteract the primary evolution,
but only partly. - Mapes (1997)
- If convective heating follows cooling by
adiabatic ascent (WISHE in full QE meaning) the
resulting effect will be cooling - If convective heating precedes cooling by
adiabatic ascent (CISK in full QE meaning) the
resulting effect will be heating. - Test to be done by statistical differences
between observations of active and non-active
periods.
13QE and causality. Le Châteliers principle as an
answer? (2/2)
14QE gt scale separation. Which concept to replace
that? (Mapes, 97)
15Vertical velocity. Which representativeness?
Which use?
For any conservative quantity ? one may
symbolically write
In other words, the computed large-scale vertical
velocity is just the average of the (rare) cloud
ascents and of a slightly sinking environment
everywhere. Hence the large scale vertical
advection term is dynamically meaningless (but
model-wise unavoidable) and has to be compensated
by a good estimate of the mass flux, slightly
bigger thanks to surface evaporation.
Thus, if QE is doubtful, the mass-flux
parameterisation should never use the diagnosed
large-scale vertical velocity as input.
16What else do we have as input for the closure
assumption?
- CAPE (Convective Available Potential Energy)
- CIN (Convective INhibition energy)
- Moisture convergence a good old concept first
introduced by Kuo (1965, 1974) in order to get
rid of convective adjustment - Moisture availability an extension of the
previous concept that tries to get rid of the QE
constraint through adding local auto-organised
moisture sources for a bulk convective
condensation (a synthesis of the 3 above ones?)
17Standard ingredients of a convective
parameterisation (and new ideas?)
18Summary
- The MOCON ? Rainfall link is sufficiently
stronger than any equivalent (at large scale and
in a steady environment) for schemes
intelligently based on such a closure to be very
robust and applicable even if the balance is less
accurate. - Going further implies to stop thinking
large-scale forcing vs. cloud balancing - Introducing a local organisation source of
moisture leads to the overall concept of (CAPE-
CIN-dependent) moisture availability - The cloud-stationarity hypothesis might be
relaxed - What then really counts is the Bulk Convective
Condensation rate (BCC). - Bougeaults 85 scheme anticipates such steps, but
not enough for meso-scale-organised and/or dry
environmental cases.