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Delft Universit y of Technolog y 1 CESAR Science Day, 19 June 2013 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

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Page 1: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 1

CESAR Science Day, 19 June 2013

CESAR Science Day, 19 June 2013

Albert Oude Nijhuis

Dynamics of turbulence in precipitation: Unravelling the eddies

Page 2: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 2

CESAR Science Day, 19 June 2013

• UFO project• Retrieval of wind field with IDRA• Retrieval of the Eddy Dissipation Rate• The Inertia Effect• Outlook

Contents

Page 3: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 3

CESAR Science Day, 19 June 2013

Page 4: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 4

CESAR Science Day, 19 June 2013

UFO Project

Page 5: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 5

CESAR Science Day, 19 June 2013

UFO Project

Page 6: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 6

CESAR Science Day, 19 June 2013

UFO Project

Page 7: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 7

CESAR Science Day, 19 June 2013

UFO Project

• The combination of LIDAR and RADAR can be used to detect wake vortices in all weather conditions.

• Quantitative information on turbulence, e.g. the eddy dissipation rate, can be retrieved from the Doppler moments, velocity and spectral width, from LIDAR and RADAR instrument.

Page 8: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 8

CESAR Science Day, 19 June 2013

Retrieval of wind field with IDRA

In contours: Doppler velocitiesHorizontal wind vectors areobtained via a least sqaures fit.

Page 9: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 9

CESAR Science Day, 19 June 2013

Retrieval of wind field with IDRA

Model from Doviak and Zrnic (1992)

Page 10: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 10

CESAR Science Day, 19 June 2013

Retrieval of wind field with IDRA

Page 11: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 11

CESAR Science Day, 19 June 2013

Retrieval of the eddy dissipation rate

The eddy dissipation rate (EDR) is based on the assumption of homogenous isotropic frozen turbulence. In the inertial sub-range the dissipation goes with a -5/3 power.

Figure from O'Connor (2010).

Page 12: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 12

CESAR Science Day, 19 June 2013

Retrieval of the eddy dissipation rate

Several retrieval methods are possible:• 1. Use the Doppler spectral width. Subtract the fall speed

distribution and compute the turbulence spectral width. Then calculate the EDR.

• 2. Use a sequence of Doppler velocities and compute the variance. Use an analytic relation to compute the EDR.

• 3. Use a sequence of Doppler velocities, and compute the vertical velocity energy density spectrum (FFT). Fit the slope from the loglog plot, which can be used to compute the EDR.

The eddy dissipation rate (EDR) is based on the assumption of homogenous isotropic frozen turbulence. In the inertial sub-range the dissipation goes with a -5/3 power.

Page 13: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 13

CESAR Science Day, 19 June 2013

Retrieval of the eddy dissipation rate

EDR from Doppler spectral width

TARA (S-band RADAR) measures the vertical Doppler verlocity at Cabauw.

EDR from Doppler velocitiy sequence

O'Connors method(from the variance)

LSF method 1

LSF method 2

Different retrieval methods lead to different answers!

Page 14: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 14

CESAR Science Day, 19 June 2013

Retrieval of the eddy dissipation rate

EDR from Doppler spectral width

EDR from the spectral width is quite a challenge, as it is depending on the drop size distribution!

Page 15: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 15

CESAR Science Day, 19 June 2013

Retrieval of the eddy dissipation rate

EDR from Doppler velocitiy sequence

O'Connors method(from the variance)

The basics

Page 16: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 16

CESAR Science Day, 19 June 2013

Retrieval of the eddy dissipation rate

Figure from O'Connor (2010). Power spectrum for a LIDAR instrument.

Power spectrum from TARA (S-band RADAR). +/- 60 min. of data.

For the RADAR the -5/3 power law seems not to be satisfied for the shorter spatial scales.

Page 17: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

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CESAR Science Day, 19 June 2013

The inertia effect

• Large droplets have inertia. They need some time to participate in the turbulent motion.

A very simple model can be used (Gorelik, 1964):- For each drop size there is a minimum length scale Lmin.- For turbulent motions larger than Lmin the drop is a perfect tracer.- For turbulent motions smaller than Lmin the drop will not participate in the motion.- For Lmin we use the approximation:

Page 18: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

DelftUniversity ofTechnology 18

CESAR Science Day, 19 June 2013

The inertia effect

• Large droplets have inertia. They need some time to participate in the turbulent motion.

Power spectrum from TARA (S-band RADAR). +/- 60 min. of data.

Theoretical power spectrum,with and without the inertia effect. Inertia effect??

Page 19: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

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CESAR Science Day, 19 June 2013

Benchmark: plot vs. height

Spectral widthFrom variance, method from (O'Connor, 2010)

Spectrum lsf method 1 Spectrum lsf method 2

Page 20: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

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CESAR Science Day, 19 June 2013

Comparing retrieval methods

LSF 2 (y-axis) vs. O'Connor

LSF 1 (y-axis) vs. O'Connor

Page 21: Delft University of Technology 1 CESAR Science Day, 19 June 2013 Albert Oude Nijhuis Dynamics of turbulence in precipitation: Unravelling the eddies

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CESAR Science Day, 19 June 2013

Outlook

• Benchmark / validate EDR retrieval methods• Investigation of the inertia effect. Potentially it may be

possible to retrieve the drop-size distribution.• The addition of a Doppler LIDAR on CESAR would be helpfull.

Then the LIDAR+RADAR combination performance for all weather conditions can be assessed.