Why do moisture convergence deep convection schemes work for more scales than those they were in principle designed for? - PowerPoint PPT Presentation

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Why do moisture convergence deep convection schemes work for more scales than those they were in principle designed for?

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ONPP/CHM & CNRM/M t o-France (on an incentive from Philippe ... More mitigated results on TOGA-COARE (and GATE) Is QE really usefull ? QE = scale separation. ... – PowerPoint PPT presentation

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Title: Why do moisture convergence deep convection schemes work for more scales than those they were in principle designed for?


1
Why 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

2
P. 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!

3
Why 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.

4
Why 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, ).

5
Convective instability is a local property
Conditional instability of the first kind
6
The mass-flux approach
  • Hypotheses
  • steady cloud
  • negligible updraft area

7
The mass-flux approach (Bougeaults 1985 variant)
8
The CISK vs. WISHE controversy
Static view (there is also a wave-propagation
equivalent)
Conditional Instability of the Second Kind
Wind Induced Surface Heat Exchange
9
The CISK vs. WISHE main difference
But the truth seems to be situation- and scale
dependent !
10
The 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.

11
The 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.

12
QE 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.

13
QE and causality. Le Châteliers principle as an
answer? (2/2)
14
QE gt scale separation. Which concept to replace
that? (Mapes, 97)
15
Vertical 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.
16
What 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?)

17
Standard ingredients of a convective
parameterisation (and new ideas?)
18
Summary
  • 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.
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