Proposed new uses for the Ceilometer Network

Slides:



Advertisements
Similar presentations
You have been given a mission and a code. Use the code to complete the mission and you will save the world from obliteration…
Advertisements

Advanced Piloting Cruise Plot.
Chapter 1 The Study of Body Function Image PowerPoint
1 Copyright © 2010, Elsevier Inc. All rights Reserved Fig 2.1 Chapter 2.
By D. Fisher Geometric Transformations. Reflection, Rotation, or Translation 1.
Jeopardy Q 1 Q 6 Q 11 Q 16 Q 21 Q 2 Q 7 Q 12 Q 17 Q 22 Q 3 Q 8 Q 13
Jeopardy Q 1 Q 6 Q 11 Q 16 Q 21 Q 2 Q 7 Q 12 Q 17 Q 22 Q 3 Q 8 Q 13
Title Subtitle.
My Alphabet Book abcdefghijklm nopqrstuvwxyz.
FACTORING ax2 + bx + c Think “unfoil” Work down, Show all steps.
Addition Facts
Year 6 mental test 5 second questions
Robin Hogan, Chris Westbrook University of Reading Lin Tian NASA Goddard Space Flight Center Phil Brown Met Office Why it is important that ice particles.
Lidar observations of mixed-phase clouds Robin Hogan, Anthony Illingworth, Ewan OConnor & Mukunda Dev Behera University of Reading UK Overview Enhanced.
Ewan OConnor, Robin Hogan, Anthony Illingworth, Nicolas Gaussiat Liquid water path from microwave radiometers.
1 Do Polluted Clouds Have Sharper Cloud Edges? Christine Chiu, Julian Mann, Robin Hogan University of Reading Alexander Marshak, Warren Wiscombe NASA Goddard.
Ewan OConnor, Robin Hogan, Anthony Illingworth, Nicolas Gaussiat Radar/lidar observations of boundary layer clouds.
Anthony Illingworth, + Robin Hogan, Ewan OConnor, U of Reading, UK and the CloudNET team (F, D, NL, S, Su). Reading: 19 Feb 08 – Meeting with Met office.
© University of Reading Richard Allan Department of Meteorology, University of Reading Thanks to: Jim Haywood and Malcolm.
Radar/lidar observations of boundary layer clouds
Robin Hogan, Julien Delanoë, Nicky Chalmers, Thorwald Stein, Anthony Illingworth University of Reading Evaluating and improving the representation of clouds.
Joint ECMWF-University meeting on interpreting data from spaceborne radar and lidar: AGENDA 09:30 Introduction University of Reading activities 09:35 Robin.
Robin Hogan Julien Delanoë Nicola Pounder Chris Westbrook
Robin Hogan Anthony Illingworth Ewan OConnor Nicolas Gaussiat Malcolm Brooks University of Reading Cloudnet products available from Chilbolton.
Robin Hogan Department of Meteorology University of Reading Cloud and Climate Studies using the Chilbolton Observatory.
Robin Hogan, Richard Allan, Nicky Chalmers, Thorwald Stein, Julien Delanoë University of Reading How accurate are the radiative properties of ice clouds.
Evaluating the Met Office global forecast model using GERB data Richard Allan, Tony Slingo Environmental Systems Science Centre, University of Reading.
Integrated lidar backscatter: Quantifying the occurrence of supercooled water and specular reflection Robin Hogan and Anthony Illingworth Enhanced algorithm.
Integrated Profiling at the AMF
ABC Technology Project
Plane wave reflection and transmission
VOORBLAD.
1 Breadth First Search s s Undiscovered Discovered Finished Queue: s Top of queue 2 1 Shortest path from s.
Factor P 16 8(8-5ab) 4(d² + 4) 3rs(2r – s) 15cd(1 + 2cd) 8(4a² + 3b²)
© 2012 National Heart Foundation of Australia. Slide 2.
Lets play bingo!!. Calculate: MEAN Calculate: MEDIAN
Chapter 5 Test Review Sections 5-1 through 5-4.
DoD Center for Geosciences/Atmospheric Research at Colorado State University Annual Review Nov 15-17, Meteosat Second Generation Algorithms for.
Addition 1’s to 20.
25 seconds left…...
Januar MDMDFSSMDMDFSSS
Week 1.
We will resume in: 25 Minutes.
©Brooks/Cole, 2001 Chapter 12 Derived Types-- Enumerated, Structure and Union.
PSSA Preparation.
Cloud Radar in Space: CloudSat While TRMM has been a successful precipitation radar, its dBZ minimum detectable signal does not allow views of light.
Application of Cloudnet data in the validation of SCIAMACHY cloud height products Ping Wang Piet Stammes KNMI, De Bilt, The Netherlands CESAR Science day,
 nm)  nm) PurposeSpatial Resolution (km) Ozone, SO 2, UV8 3251Ozone8 3403Aerosols, UV, and Volcanic Ash8 3883Aerosols, Clouds, UV and Volcanic.
Using a Radiative Transfer Model in Conjunction with UV-MFRSR Irradiance Data for Studying Aerosols in El Paso-Juarez Airshed by Richard Medina Calderón.
May 10, 2004Aeronet workshop Can AERONET help with monitoring clouds? Alexander Marshak NASA/GSFC Thanks to: Y. Knyazikhin, K. Evans, W. Wiscombe, I. Slutsker.
1 Cloud Droplet Size Retrievals from AERONET Cloud Mode Observations Christine Chiu Stefani Huang, Alexander Marshak, Tamas Várnai, Brent Holben, Warren.
METO 621 Lesson 27. Albedo 200 – 400 nm Solar Backscatter Ultraviolet (SBUV) The previous slide shows the albedo of the earth viewed from the nadir.
Direct Radiative Effect of aerosols over clouds and clear skies determined using CALIPSO and the A-Train Robert Wood with Duli Chand, Tad Anderson, Bob.
1. The MPI MAX-DOAS inversion scheme 2. Cloud classification 3. Results: Aerosol OD: Correlation with AERONET Surface extinction: Correlation with Nephelometer.
Introduction Invisible clouds in this study mean super-thin clouds which cannot be detected by MODIS but are classified as clouds by CALIPSO. These sub-visual.
ARM Data Overview Chuck Long Jim Mather Tom Ackerman.
The Centre for Australian Weather and Climate Research A partnership between CSIRO and the Bureau of Meteorology Southern Ocean cloud biases in ACCESS.
Cloud property retrieval from hyperspectral IR measurements Jun Li, Peng Zhang, Chian-Yi Liu, Xuebao Wu and CIMSS colleagues Cooperative Institute for.
UCLA Vector Radiative Transfer Models for Application to Satellite Data Assimilation K. N. Liou, S. C. Ou, Y. Takano and Q. Yue Department of Atmospheric.
Cloudnet meeting Oct Martial Haeffelin SIRTA Cloud and Radiation Observatory M. Haeffelin, A. Armstrong, L. Barthès, O. Bock, C. Boitel, D.
UNIVERSITY OF BASILICATA CNR-IMAA (Consiglio Nazionale delle Ricerche Istituto di Metodologie per l’Analisi Ambientale) Tito Scalo (PZ) Analysis and interpretation.
Cloud Detection: Optical Depth Thresholds and FOV Considerations Steven A. Ackerman, Richard A. Frey, Edwin Eloranta, and Robert Holz Cloud Detection Issues.
The study of cloud and aerosol properties during CalNex using newly developed spectral methods Patrick J. McBride, Samuel LeBlanc, K. Sebastian Schmidt,
LIDAR Ben Kravitz November 5, 2009.
Absolute calibration of sky radiances, colour indices and O4 DSCDs obtained from MAX-DOAS measurements T. Wagner1, S. Beirle1, S. Dörner1, M. Penning de.
DETERMINATION OF PHOTOSYNTHETICALLY ACTIVE RADIATION
Emma Hopkin University of Reading
Presentation transcript:

Proposed new uses for the Ceilometer Network Christine Chiu Ewan O’Conner, Robin Hogan, James Holmes University of Reading

Outline What we propose to observe and why this is new How we retrieve cloud optical depth from ceilometer data How well the method performs and how we can work together

Ceilometers have been used to observe aerosols and clouds Cloud base height for all cloud cases Cloud optical depth for thin clouds How about thick clouds?

Cloud optical depth is the great unknown Differences between climate models: factor 2-4 (Zhang et al., JGR, 2005) Differences between ground-based methods: factor 2-4 (Turner et al., BAMS, 2007)

Multi-filter rotating shadowband radiometer (MFRSR) works only for overcast cases

AERONET cloud mode provides routine cloud optical depth measurements Normal aerosol mode (sun-seeking) Cloud mode (zenith-pointing) Chiu et al. (JGR, 2010)

Ceilometers measure zenith radiance too! “solar background light” (a lidar noise source) Signal no lidar Sun shoots Fractional day Zenith Radiance (arbitrary unit) cloudy clear lidar shoots 200508071800

1-channel zenith radiance measurements are ambiguous for cloud retrievals in a 1D radiative transfer world Cloud optical depth Zenith Radiance 3D simulations Cloud’s optical influence extends far beyond the borders of the cloud plane-parallel

Thick clouds – ceilometer’s active beam is completely attenuated

Use known overcast and clear-sky cases to develop our classification scheme Overcast thick clouds Cloud optical depth > 10 continuously at least for 1 hour Clear-sky Cloud optical depth < 3 continuously at least for 1hour Cloud’s optical influence extends far beyond the borders of the cloud

Determine if ceilometer’s active beam is completely attenuated Find the cloud top layer using cloud flags in Cloudnet products Backscatter signal (sr-1 m-1) Range (km) Calculate the mean backscatter signal from the cloud top to 1 km above cloud top

Histogram of mean backscatter for clear-sky cases 100 counts clear-sky cases Altitude (km) cloudy clear This threshold properly indentifies 97% of clear-sky cases mean backscatter (log scale) between cloud top and 1km above

Histogram of mean backscatter for overcast clouds clear cloudy 100 counts Altitude (km) This threshold properly indentifies 86% of cloudy cases mean backscatter (log scale) between cloud top and 1km above

Evaluate our classification scheme using cloud mode retrievals Cloud optical depth from ceilometer drizzling thin clouds time/spatial resolution examples are May 3, 19 UTC Cloud optical depth from AERONET cloud mode

Intercomparison at Chilbolton and Oklahoma sites

Comparison to other instruments AERONET cloud mode observations Microwave radiometer Cloud radar reff in μm, Liquid Water Path in g/m2

Example from Chilbolton 2010/08/17 Reflectivity Attenuated backscatter coefficient

Retrievals from ceilometer, cloud mode and MWR agree well Cloud optical depth MWR ct75K Aeronet ct75K Time (UTC)

Example – cirrus cloud (Oklahoma) Reflectivity Attenuated backscatter coefficient 20071122 SGP from ct25K Time (UTC)

Retrievals difference could be up to 30% if using a wrong cloud phase Cloud optical depth ice phase (D60) ice phase (D180) 20071122 SGP from ct25K water phase Time (UTC)

Ice water paths derived from various empirical relationships Ice water path (g/m2) ? 20071122 SGP from ct25K Time (UTC)

A more complex case – water cloud and thick ice cloud (Oklahoma) Reflectivity Attenuated backscatter coefficient

Agreement is shown again for water clouds Retrieved cloud optical depth AERONET ceilometer MWR Time (UTC)

Cloud optical depth could differ 30 –40% due to cloud phase Retrieved cloud optical depth Time (UTC)

Water clouds at the Oklahoma site in 2007 May-November Occurrence counts cloud optical depth

Difference between ceilometer and lidar applications Pros Seem easier to cross-calibrate ceilometer solar background light data Smaller impact from aerosol and Rayleigh scattering at ceilometer wavelengths Cons Surface albedo could fluctuate quite significantly at 905 nm A few weak water vapor absorption lines around 905 nm

Summary The use of solar background light can greatly enhance current cloud products of ceilometer networks Confident about cloud optical depth retrievals for water clouds Continue testing our classification algorithm that distinguishes optically thin and thick clouds A lot of work needs to be done for retrieving ice- and mixed-phase clouds