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© Crown copyright Met Office Cloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel

Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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Page 1: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

© Crown copyright Met Office

Cloud Simulation in VOCALSIan Boutle with thanks to Cyril Morcrette and Steven Abel

Page 2: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

© Crown copyright Met Office

Contents

• Representation of stratocumulus during VOCALS in the Met Office Unified Model (MetUM)

• Case study of simulations at various resolutions

• Analysis of prognostic cloud scheme increments for stratocumulus

• Improvements to the cloud forecast

• Implementation of a prognostic cloud scheme in a “cloud resolving” model

Page 3: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

© Crown copyright Met Office

Representation of stratocumulus during VOCALS in the MetUM

Page 4: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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Stratocumulus schematic

A test for many of the parametrization schemes in GCMs

Page 5: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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Wyant et al. (2010)Cloud Fraction, October average

Page 6: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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• Strong diurnal cycle in liquid water path and low cloud fraction

• Typically under-estimated in all models

• A mixture of good cloud cover, wrong water content and bad cloud cover, right water content

• Use the MetUM to investigate this…

Liquid water path

Cloud fraction

Wyant et al. (2010)

Page 7: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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VOCALS case-study

• Field experiment conducted during October and November 2008 to study the south-east Pacific stratocumulus.

• Additional observations available from Ronald H. Brown research vessel, FAAM BAE-146 and NSF C-130 flying out from Chile.

• Case study on 12th and 13th November 2008.

• Nested simulations driven from global NWP model (44km), with 12km, 4km and 1km horizontal resolution nested domains.

Page 8: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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Cloud fraction from 12km simulation

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Title

Cloud fraction from 1km simulation

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Snapshot of cloud fields at 15Z

GOES-10 Visible Image MetUM SW flux at TOA

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Nested Model Results

• All resolutions are surprisingly similar in their cloud evolution!

• Causes of LWP under-estimation are not resolution based.

• In-cloud water contents are always under-estimated

• Look at PC2 increments in global model to understand importance of different parametrization schemes on the cloud cover.

LWP

Cloud Cover

Obs from AMSR-E, SSMI and TMI

Obs from GOES-10

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PC2 Cloud Scheme in Global Model• Calculates sources and sinks of cloud liquid

condensate/fraction from:• Radiation (LW cooling, SW heating)• Microphysics (rain-out of condensate)• Advection (moves cloud around)• Convection (cloud detrained from convective plume)• Erosion (evaporation at cloud edges)• Boundary-layer (vertical mixing)• Pressure change (large-scale vertical motion)• Initiation (scheme closure at clear/overcast sky)

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Convection

LW Rad

Erosion

Precipitation

SW Rad

Boundary layer

Liquid Water Path Increments

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Important cloud liquid processes• Convection main source of cloud water –

detrainment from plume as it rises and terminal detrainment at capping inversion

• Long-wave cooling also important – mainly at stratocumulus cloud top

• Boundary-layer also creates some cloud by moistening the cloud layer

• Precipitation main sink of cloud water• Erosion also important – mixing of saturated

and sub-saturated air at cloud boundaries

• Short-wave heating removes some cloud during the day-time

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Convection

LW Rad

Erosion

SW Rad

Liquid Cloud Fraction Increments

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Important cloud fraction processes• Convection is main source again, for the same

reason• Long-wave cooling is negligible – cloud fraction

already near 1 at cloud top!• No precipitation effect on cloud fraction (by

scheme design)• Erosion is therefore the main sink• Again, short-wave heating removes cloud

during the day, almost in balance with the long-wave cooling

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What does all this tell us about LWP and cloud cover?

• Drizzle production is biggest sink of cloud liquid water• Autoconversion process converts cloud liquid (qcl) into rain water

(qrain) based on a process rate:

• A, B and C are parametrized values (Nd is cloud droplet number)

• Hypothesis to test: reducing the autoconversion rate should reduce drizzle and increase LWP

Bd

A NqclCt

qrain)()(

)( =∂

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Two possible autoconversion schemes

• Control MetUM uses Tripoli and Cotton (1980) parametrization

• Khairoutdinov and Kogan (2000) has much lower autoconversion rate, based on large-eddy simulations of stratocumulus

• Wood (2005) suggests that KK autoconversion rate is in better agreement to observations of stratocumulus

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• General increase in LWP and cloud cover from autoconversion scheme change

• Increase in LWP is higher at night than during the day – not uniform

• In-cloud amounts are now good all the time, there is just too much cloud cover during the day

LWP

Cloud Cover

Obs from AMSR-E, SSMI and TMI

Obs from GOES-10

Page 20: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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Implementation of a prognostic cloud scheme in a “cloud resolving” modelaka PC2 at 1km

Page 21: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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PC2 Cloud Scheme in 1km Model• Calculates sources and sinks of cloud liquid

condensate/fraction from:• Radiation (LW cooling, SW heating)• Microphysics (rain-out of condensate)• Advection (moves cloud around)• Convection (cloud detrained from convective plume)• Erosion (evaporation at cloud edges)• Boundary-layer (vertical mixing)• Pressure change (large-scale vertical motion)• Initiation (scheme closure at clear/overcast sky)

Convection resolved at the grid-scale

What happens if we lose the main source of cloud?!

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Snapshot at 12ZLiquid Water Path Cloud Fraction

Page 23: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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Pressure Change

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Precipitation / Erosion

Page 25: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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Long Wave Radiation

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Advection

Prevailing Wind

Page 27: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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LW Rad

Pressure Change

Precipitation

SW Rad

Advection

Liquid water increments

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LW Rad

Pressure Change

Erosion

SW Rad

Advection

Liquid cloud fraction increments

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Cloud sources and sinks at 1km• Pressure change is now a large source of cloud

(fraction and liquid), due to resolved scale ascent in convective clouds

• Vertical advection transports cloud upwards• Precipitation is still main sink of cloud liquid• Erosion, which was always a sink in the global

model, is now a large source of fraction near the cloud tops

• Can now see the advection moving individual clouds downstream with the flow

Page 30: Cloud Simulation in VOCALS - Royal Meteorological Society · PDF fileCloud Simulation in VOCALS Ian Boutle with thanks to Cyril Morcrette and Steven Abel ... • Can implement a prognostic

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Conclusions

• Stratocumulus is a fine balance between different parametrization schemes, and model resolution doesn’t really help too much with improving the simulation

• Most GCMs struggle to represent the diurnal cycle of cloud LWP

• Analysing the PC2 increments suggests the parametrization to focus on (microphysics) and changes to it lead to an improved simulation

• Can implement a prognostic cloud scheme in a high-resolution model, and it produces a reasonable simulation

• Large differences between global and 1km resolution PC2 process rates

• Need some careful thought about whether the assumptions behind the PC2 process rates are valid at this scale