1 / 145

Doppler Radar

Doppler Radar. The Doppler Effect The Doppler Dilemma Etc – other topics Doppler Analysis and Diagnosis (Important New and Original Material linked to slide 80). The Doppler effect. Classically, the Doppler effect is a frequency shift

mason-weber
Download Presentation

Doppler Radar

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Doppler Radar • The Doppler Effect • The Doppler Dilemma • Etc – other topics • Doppler Analysis and Diagnosis (Important New and Original Material linked to slide 80)

  2. The Doppler effect • Classically, the Doppler effect is a frequency shift • The change in frequency of a signal returned from a target owing to its radial motion relative to an observer • With radar, this is measured as a shift in phase between the transmitted pulse and the backscattered microwave radiation • Average radial velocity of the target is calculated from this phase shift

  3. The Radar Waveform

  4. Velocity Spectrum Stationary GC WX WX Moves -VN 0 +VN

  5. Phase Shift Ambiguity A shift of ¼ wavelength is ambiguous. You don’t know if your are coming or going?

  6. Velocity folding – Phase Shift Ambiguity • Target radial velocities producing phase shifts greater than one-half wavelength (or p radians) results in velocity folding • Maximum unambiguous radial velocity Vmax (Nyquist velocity) = • (PRF X Wavelength)/ 4 • This range is not adequate to describe all horizontal velocities Nyquist velocity=1200 X 5cm/4 = 1500cm/sec=15m/s=30knots Is a Nyquist velocity of 30knots enough?

  7. The velocities with this storm are HUGE !!!! Quick, increase the PRF and give me a sector scan on the storm cell ! Vmax (Nyquist velocity) = (PRF X Wavelength) / 4 By increasing the PRF, velocity foldng starts at a higher radial velocity

  8. Folded Doppler quickly reaches the maximum colour range and cycles to opposite colours = noisy, complicated fields Interpretation is challenging! Helen was right! ? ? After PRF increased Before Helen’s Demand

  9. Doppler Dilemma • Maximum unambiguous range: • Rmax = c / 2PRF • What is this for PRF = 1200 ? • VmaxRmax = cl/8 • Vmax and Rmax are inversely proportional to each other, but we want to maximize both • That’s the Doppler dilemma 125 km

  10. How can we increase Vmax ?

  11. Velocity Unfolding • Use two PRF’s and take the difference in the Doppler velocities ! • The difference turns out to be a unique function of the actual velocity out to much higher velocities!! • So DV and one of the velocity measurements can be used to unambiguously calculate the actual radial velocity, perhaps up to 48 m/s (almost 100 knots).

  12. Whoa. Now that’s fast!!

  13. Dual PRF Unfolding

  14. Now we can see the whole storm, Bill ! That’s great, Jo. Now if only Dorothy and pigs would fly !

  15. Example: Radial Velocity Product with Vr to 48 m/s N-S Warm Front? Katabatic Cold Front? WLY upper level winds SELY low level winds

  16. Doppler Patterns

  17. Doppler wind interpretation • You can determine wind direction vs. height away from radar in two different directions • Go out along zero line • Draw line back to radar • Wind is perpendicular to this line, towards the red echoes

  18. Doppler wind interpretation • For any height you can attempt to determine the wind in 4 locations • Determine the two zero line winds • Look roughly 90° away for the max wind, which should be all directed along a radial • In this way you can see areas of non-uniform flow • confluence, diffluence

  19. Doppler Uniform 30 m/s wind everywhere

  20. Doppler Display - Uniform Wind Shear Vertical Wind Shear of 13 knots per kilometre = Speed Shear only

  21. 20 20 Doppler with Directional Shear and Jet Directional Shear and Wind Maximum

  22. Doppler with Wind Shear - Speed and Directional Direction veering with height Speed increasing with height

  23. The Doppler Vortex

  24. Doppler Practice Westerly Winds with only Speed shear

  25. Doppler Practice Westerly Winds with Low Level Jet

  26. Doppler Practice Veering Winds with no Speed shear

  27. Doppler Practice Backing Winds with no Speed shear

  28. Doppler Practice Changes in Stability? Low Level Veering under High Level Backing Winds - no Speed shear

  29. Doppler Practice Wind shift line

  30. Doppler Practice Large Scale Convergence

  31. Doppler Practice Radar Site Divergence

  32. Doppler Practice Radar Site Cyclonic Vortex

  33. SWLY NNELY Doppler Practice LLJ QS Horizontal LLJ Marginal winds Backing with Height - Cold Air Advection Maybe a Cold Conveyor Belt ahead of a synoptic system…

  34. Doppler Displays

  35. Velocity Azimuth Display - VAD • Doppler radial velocity data used to construct a wind profile in the vertical • Direction, speed (m/s) and reflectivity (dBZ) displayed as a function of height (km) • Note: Velocity scale is fixed in range 0-20 m/s ( i.e. most of the unfolded velocities are not used )

  36. Velocity Azimuth Display - VAD • At a given height (h), then the radial velocity is: • For a uniform flow field and assume Vw (Vertical Velocity) approximately = 0 then • Best fit of a sine curve to the observations around the circle.

  37. Velocity Azimuth Display - VAD • Accuracy of VAD decreases with elevation angle and height. The desired horizontal wind component becomes a smaller part of the radial wind component actually measure. • Errors in the radial component has a bigger impact on the accuracy of the horizontal wind

  38. VAD Example

  39. A new Velocity Azimuth Display LOLAA sees winds far from radar 3.5° scan sees winds closer in to radar – behaves most like a “profiler”

  40. Doppler Spectra Width • Spread of the Doppler Power Spectrum • the spread, range of terminal fall speeds of the scatterers (more pronounced for rain than for snow) spectra for rain spectra for snow • turbulence of the air (upper levels in severe convection) • vertical wind shear (e.g., along a gust front) • antenna motion Rain Snow

  41. Doppler Image Characteristics Small Spectral Width Large Spectral Width

  42. Spectral Width and “Doppler Display Texture” Rain Texture Snow Texture

  43. The Doppler Precipitation Spectral Width Doppler Precipitation Texture Example

  44. The Doppler Twist Signature - Example • The white dashed line separates different wind regimes in the vertical. • It also separates regimes of differing Doppler texture. • Above the dashed line the Doppler texture is uniform and characteristic of snow. • Below the dashed line the texture is lumpy like oatmeal and characteristic of rain. • This is also an example of the Virga Hole Signature The dashed line is likely the warm front. The layer immediately below is where the snow is melting into rain.

  45. Filtering using Doppler and Processing

  46. Second Trip Echo – Extending the Range of the Doppler Scan Random Phase Processing extends the Doppler Range Dual PRF’s extends the Nyquist Velocity

  47. Second Trip Echoes

  48. Second Trip Echo The velocity signatures of second trip echoes are very noisy. These still contribute to the reflectivity signal where they should not.

  49. Second Trip Processing

  50. Second Trip Processing Doppler Reflectivity with Processed Second Trip Echoes Conventional CAPPI Doppler Reflectivity with Second Trip Echoes Doppler Reflectivity

More Related