Particle Filters for Numerical Weather Prediction Peter Jan van - - PowerPoint PPT Presentation

particle filters
SMART_READER_LITE
LIVE PREVIEW

Particle Filters for Numerical Weather Prediction Peter Jan van - - PowerPoint PPT Presentation

Particle Filters for Numerical Weather Prediction Peter Jan van Leeuwen + PF group (Mel Ades, Javier Amezcua, Phil Browne, David Livings, Alison Fowler, Matt Lang, Michael Goodliff) Data-Assimilation Research Centre DARC University of


slide-1
SLIDE 1

Particle Filters for Numerical Weather Prediction

Peter Jan van Leeuwen + PF group

(Mel Ades, Javier Amezcua, Phil Browne, David Livings, Alison Fowler, Matt Lang, Michael Goodliff)

Data-Assimilation Research Centre DARC University of Reading, UK

slide-2
SLIDE 2

What is a particle filter?

  • Write the prior pdf as
  • Then the posterior pdf is given as

with the weights wi related to the distance to the observations and the model equations

slide-3
SLIDE 3

Curse of dimensionality

The weights are degenerate with a large number of

  • bservations: one particle gets weight 1, rest weight 0.

This problem has largely been solved:

  • Particle filters have enormous freedom via proposal density:
  • Relaxation to observations between observation times
  • E.g. Equivalent-Weights Particle Filter is not degenerate by

construction

  • ONLY APPROXIMATION IS FINITE ENSEMBLE SIZE
  • Example: 65,000 dimensional highly nonlinear barotropic

vorticity model, observations every 50 timesteps, 32 particles

slide-4
SLIDE 4

Equivalent-Weights Particle Filter

  • Force model towards observations between
  • bservation times
  • Ensure that weights are equivalent at
  • bservation times:

t=0 t=50 t=100 y y

slide-5
SLIDE 5

Fully observed system

slide-6
SLIDE 6

Half-observed system

Observe 1/16 of the grid points within the red square

  • nly.
slide-7
SLIDE 7

The relaxation step

b=0.05 b=0.4

slide-8
SLIDE 8

The Equivalent-weights step

slide-9
SLIDE 9

Convergence of the pdf

32 particles 128 particles 512 particles

slide-10
SLIDE 10

Rank histograms

Full state observed

slide-11
SLIDE 11

Between observations

  • Relaxation (nudging)
  • 4DVar on each particle: Initial condition fixed

Model error essential

X X X X

slide-12
SLIDE 12

Why Particle Filters?

  • PF solve fully nonlinear data-assimilation problem
  • No state covariances !!!

4DVar: B matrix, EnKF’s localisation+inflation

  • Model errors essential, so we have to work on them:

natural way to model improvement

  • Particles are independent random draws from

posterior pdf

  • Perfect for forecasting!
slide-13
SLIDE 13

Conclusions + Outlook

  • Particle filters do not need state covariances.
  • Proposal density allows enormous freedom
  • We can solve the curse-of-dimensionality problem by

construction, e.g. Equivalent-weights scheme

  • Other efficient schemes are being derived.
  • We have to work on model error covariances
  • We are working on applications to ECMWF system and

HadCM3 climate model

slide-14
SLIDE 14

¼ observations over half of state