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Chaos & Weather Control 
Ross N. Hoffman 
Atmospheric and Environmental Research 
5 Nov 2003 
Atlanta 
H.Iniki 1992 (NWS image)
5 Nov 2003, Atlanta 2 
Acknowledgments 
•Co-investigators: John Henderson, Mark Leidner, GeorgeModica 
•Supported by a NIAC phase 2 contract 
•DOD CHSSI project supported the development of the parallel version of the MM5 4d-VAR system at AER
5 Nov 2003, Atlanta 3 
Today’s talk 
•Experiments to control hurricanes 
•A different approach to weather control–not just hurricanes 
•Based on the sensitivity of the atmosphere 
•The same reason why it is so difficult to predict the weather!
5 Nov 2003, Atlanta 4 
Conventional WxMod•Rain enhancement•Fog dissipation–Cold fog –ice nuclei–Warm fog –jet engines provide heat•Frost prevention (Florida citrus) •Hail suppression –ice nuclei•Lightning suppression –chaffProject Cirrus 1948
5 Nov 2003, Atlanta 5 
Rain enhancement 
•Cold clouds –ice nuclei 
•Warm clouds –CCN; hygroscopic flares; brine spray 
•Anthropogenic aerosols and dust result in inadvertent WxMod 
•AddingCCNs or ice nuclei can increase or decrease rainfall 
–Too many and the drops are too small. Too few and there are not enough drops
5 Nov 2003, Atlanta 6 
Critical Issues in Weather Modification Research 
•New National Academies Report 
–Committee on the Status and Future Directions in U.S Weather Modification Research and Operations, National Research Council 
–The prepublication online version: 
–www.nap.edu/books/0309090539/html/
5 Nov 2003, Atlanta 7 
Future WxMod 
•Improved models, observations, and assimilation systems will advance to the point where forecasts are: 
–much improved, and 
–include an estimate of uncertainty 
•Thus allowing advance knowledge that a change should be detectable in particular cases
5 Nov 2003, Atlanta 8 
Theoretical basis•The earth’s atmosphere is chaotic•Chaos implies a finite predictability time limit no matter how well the atmosphere is observed and modeled•Chaos also implies sensitivity to small perturbations•A series of small but precise perturbations might control the evolution of the atmosphere
5 Nov 2003, Atlanta 9 
Current NWP operational practice 
•NWP centers have developed forecast techniques that capitalize on the sensitivity of the atmosphere 
1.4D variational data assimilation 
2.Generation of ensembles 
3.Adaptive observations
5 Nov 2003, Atlanta 10 
NCEP spaghetti plot
5 Nov 2003, Atlanta 11 
System components 
1.Numerical weather prediction 
2.Data assimilation systems 
3.Satellite remote sensing 
4.Perturbations 
5.Computer technology 
6.Systems integration
5 Nov 2003, Atlanta 12 
Why hurricanes? 
•Public interest: Threat to life and property 
•History: Project Stormfury (1963) 
•Sensitive to initial conditions 
•MM5/4d-VAR: Available tools
5 Nov 2003, Atlanta 13 
Iniki Simulation 
750-hPa Relative Humidity
5 Nov 2003, Atlanta 14 
HurricaneWxMod 
•Energetics 
–Biodegradable oil 
–Pump cold water up to the surface 
•Dynamic perturbations 
–Stormfury: cloud seeding 
–Space based heating
5 Nov 2003, Atlanta 15 
Space based heating 
•Solar reflectors: bright spots on the night side and shadows on the day side 
•Space solar power (SSP): microwave downlink could provide a tunable atmospheric heat source
5 Nov 2003, Atlanta 16 
Cosmos 1 solar sail
5 Nov 2003, Atlanta 17 Space solar powerNASA artwork by Pat Rawlings/SAIC
5 Nov 2003, Atlanta 18 
Microwave spectrum 
•Water and oxygen are the main gaseous absorbers 
–H2O lines at 22, 183 GHz 
–H2O continuum 
–O2 lines at 60, 118 GHz 
•Frequency and bandwidth control the heating profile
5 Nov 2003, Atlanta 19 
Heating rates (K/hr) Frequency (GHz) 0.00.51.01.52.02.53.03.5≥4 km
5 Nov 2003, Atlanta 20 
Power requirements 
•Heating rates calculated for 1500 W/m2 
•Equal to 6 GW/(2 km)2 
•Current experiments require similar heating rates over an area 100s times larger 
•Longer lead times, higher resolution will reduce these requirements significantly
5 Nov 2003, Atlanta 21 
Determination of perturbations 
•Optimal control theory 
•4d-Var methodology baseline 
•Modified control vector: temperature only 
•Refined cost function: property damage
5 Nov 2003, Atlanta 22 
Mesoscale model 
•The MM5 computation grid is 200 by 200, with a 20 km grid spacing, and ten layers in the vertical 
•Physics are either 
–Simplified parameterizations of the boundary layer, cumulus convection, stratiform cloud, andradiative transfer; or 
–Enhanced parameterizations of these physical processes and a multi-layer soil model
5 Nov 2003, Atlanta 23 
4Dvariationaldata assimilation 
•4D-Varadjusts initial conditions to fit all available observations during a 6 or 12 hour time window 
•The fit to the observations is balanced against the fit to the a priori or first guess from a previous forecast 
•We use a variant of 4D-Var in our experiments
5 Nov 2003, Atlanta 24 
Standard 4D-Varcost function•J is the cost function•P is the perturbed forecast•G is the goal–G is the target at t=T and the initial unperturbed state at t=0•S is a set of scales–S depends only on variable and level•x is temperature or a wind component•i, j, and k range over all the grid pointsJ = Σxijkt[(Pxijk(t)–Gxijk(t))/Sxk]2
5 Nov 2003, Atlanta 25 
Modified control vector 
•Control vector can be restricted by variable and by geographic region 
–Temperature only 
–Locations far from the eye wall
5 Nov 2003, Atlanta 26 
Refined cost function 
•JD= ΣijtDij(t)Cij 
•C is the replacement cost 
•D is the fractional wind damage 
–D = 0.5 [1 +cos(π(V1-V)/(V1-V0))] 
•D=0 for V<V0= 25 m/s 
•D=1 for V>V1= 90 m/s 
–Evaluated every 15 min. for hours 4–6
5 Nov 2003, Atlanta 27 
Relativepropertyvalues
5 Nov 2003, Atlanta 28 
Experiments 
•Hurricane Andrew simulations starting at 00 UTC 24 Aug 1992 
•Initial conditions from an earlier 6 h forecast; NCEP reanalysis; bogus vortex 
•4d-Var over 6 h (ending 06 UTC 24 Aug); 20 km grid; temperature increments only; simple physics 
•Simulations for unperturbed vs. controlled; 20 km simple physics vs. 7 km enhanced physics
5 Nov 2003, Atlanta 29 
Unperturbed surface winds
5 Nov 2003, Atlanta 30 
Unperturbed 
4 waywinds 
7 km 
20 kmControlled
5 Nov 2003, Atlanta 31 
Temperature increments
5 Nov 2003, Atlanta 32 
Temperature increments
5 Nov 2003, Atlanta 33 
Temperature increments
5 Nov 2003, Atlanta 34 
Temperature increments
5 Nov 2003, Atlanta 35 
Time evolution 00 UTC
5 Nov 2003, Atlanta 36 
Time evolution 06 UTC
5 Nov 2003, Atlanta 37 
Time evolution 12 UTC
5 Nov 2003, Atlanta 38 
Time evolution 18 UTC
5 Nov 2003, Atlanta 39 
Relative humidity 00 UTC
5 Nov 2003, Atlanta 40 
Relative humidity 06 UTC
5 Nov 2003, Atlanta 41 
Relative humidity 12 UTC
5 Nov 2003, Atlanta 42 
Relative humidity 18 UTC
5 Nov 2003, Atlanta 43 
Summary 
•Perturbations calculated by 4d-Var 
•Control path, intensity of simulated hurricane 
•Power requirements are huge 
–Higher resolution, longer lead times may help 
–Very large scale SSP could meet the requirements
5 Nov 2003, Atlanta 44 
The future 
•More realistic experiments: resolution, physics, perturbations 
•Future advances in several disciplines will lead to weather control capabilities 
–The first experiments will not be space based control oflandfalling hurricanes! 
•Can legal and ethical questions be answered
5 Nov 2003, Atlanta 45 
end 
•Contact: 
–ross@aer.com 
•Background: 
–R. N. Hoffman. Controlling the global weather. Bull. Am.Meteorol. Soc., 83(2):241--248, Feb. 2002.

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Chaos andweathercontrol

  • 1. Chaos & Weather Control Ross N. Hoffman Atmospheric and Environmental Research 5 Nov 2003 Atlanta H.Iniki 1992 (NWS image)
  • 2. 5 Nov 2003, Atlanta 2 Acknowledgments •Co-investigators: John Henderson, Mark Leidner, GeorgeModica •Supported by a NIAC phase 2 contract •DOD CHSSI project supported the development of the parallel version of the MM5 4d-VAR system at AER
  • 3. 5 Nov 2003, Atlanta 3 Today’s talk •Experiments to control hurricanes •A different approach to weather control–not just hurricanes •Based on the sensitivity of the atmosphere •The same reason why it is so difficult to predict the weather!
  • 4. 5 Nov 2003, Atlanta 4 Conventional WxMod•Rain enhancement•Fog dissipation–Cold fog –ice nuclei–Warm fog –jet engines provide heat•Frost prevention (Florida citrus) •Hail suppression –ice nuclei•Lightning suppression –chaffProject Cirrus 1948
  • 5. 5 Nov 2003, Atlanta 5 Rain enhancement •Cold clouds –ice nuclei •Warm clouds –CCN; hygroscopic flares; brine spray •Anthropogenic aerosols and dust result in inadvertent WxMod •AddingCCNs or ice nuclei can increase or decrease rainfall –Too many and the drops are too small. Too few and there are not enough drops
  • 6. 5 Nov 2003, Atlanta 6 Critical Issues in Weather Modification Research •New National Academies Report –Committee on the Status and Future Directions in U.S Weather Modification Research and Operations, National Research Council –The prepublication online version: –www.nap.edu/books/0309090539/html/
  • 7. 5 Nov 2003, Atlanta 7 Future WxMod •Improved models, observations, and assimilation systems will advance to the point where forecasts are: –much improved, and –include an estimate of uncertainty •Thus allowing advance knowledge that a change should be detectable in particular cases
  • 8. 5 Nov 2003, Atlanta 8 Theoretical basis•The earth’s atmosphere is chaotic•Chaos implies a finite predictability time limit no matter how well the atmosphere is observed and modeled•Chaos also implies sensitivity to small perturbations•A series of small but precise perturbations might control the evolution of the atmosphere
  • 9. 5 Nov 2003, Atlanta 9 Current NWP operational practice •NWP centers have developed forecast techniques that capitalize on the sensitivity of the atmosphere 1.4D variational data assimilation 2.Generation of ensembles 3.Adaptive observations
  • 10. 5 Nov 2003, Atlanta 10 NCEP spaghetti plot
  • 11. 5 Nov 2003, Atlanta 11 System components 1.Numerical weather prediction 2.Data assimilation systems 3.Satellite remote sensing 4.Perturbations 5.Computer technology 6.Systems integration
  • 12. 5 Nov 2003, Atlanta 12 Why hurricanes? •Public interest: Threat to life and property •History: Project Stormfury (1963) •Sensitive to initial conditions •MM5/4d-VAR: Available tools
  • 13. 5 Nov 2003, Atlanta 13 Iniki Simulation 750-hPa Relative Humidity
  • 14. 5 Nov 2003, Atlanta 14 HurricaneWxMod •Energetics –Biodegradable oil –Pump cold water up to the surface •Dynamic perturbations –Stormfury: cloud seeding –Space based heating
  • 15. 5 Nov 2003, Atlanta 15 Space based heating •Solar reflectors: bright spots on the night side and shadows on the day side •Space solar power (SSP): microwave downlink could provide a tunable atmospheric heat source
  • 16. 5 Nov 2003, Atlanta 16 Cosmos 1 solar sail
  • 17. 5 Nov 2003, Atlanta 17 Space solar powerNASA artwork by Pat Rawlings/SAIC
  • 18. 5 Nov 2003, Atlanta 18 Microwave spectrum •Water and oxygen are the main gaseous absorbers –H2O lines at 22, 183 GHz –H2O continuum –O2 lines at 60, 118 GHz •Frequency and bandwidth control the heating profile
  • 19. 5 Nov 2003, Atlanta 19 Heating rates (K/hr) Frequency (GHz) 0.00.51.01.52.02.53.03.5≥4 km
  • 20. 5 Nov 2003, Atlanta 20 Power requirements •Heating rates calculated for 1500 W/m2 •Equal to 6 GW/(2 km)2 •Current experiments require similar heating rates over an area 100s times larger •Longer lead times, higher resolution will reduce these requirements significantly
  • 21. 5 Nov 2003, Atlanta 21 Determination of perturbations •Optimal control theory •4d-Var methodology baseline •Modified control vector: temperature only •Refined cost function: property damage
  • 22. 5 Nov 2003, Atlanta 22 Mesoscale model •The MM5 computation grid is 200 by 200, with a 20 km grid spacing, and ten layers in the vertical •Physics are either –Simplified parameterizations of the boundary layer, cumulus convection, stratiform cloud, andradiative transfer; or –Enhanced parameterizations of these physical processes and a multi-layer soil model
  • 23. 5 Nov 2003, Atlanta 23 4Dvariationaldata assimilation •4D-Varadjusts initial conditions to fit all available observations during a 6 or 12 hour time window •The fit to the observations is balanced against the fit to the a priori or first guess from a previous forecast •We use a variant of 4D-Var in our experiments
  • 24. 5 Nov 2003, Atlanta 24 Standard 4D-Varcost function•J is the cost function•P is the perturbed forecast•G is the goal–G is the target at t=T and the initial unperturbed state at t=0•S is a set of scales–S depends only on variable and level•x is temperature or a wind component•i, j, and k range over all the grid pointsJ = Σxijkt[(Pxijk(t)–Gxijk(t))/Sxk]2
  • 25. 5 Nov 2003, Atlanta 25 Modified control vector •Control vector can be restricted by variable and by geographic region –Temperature only –Locations far from the eye wall
  • 26. 5 Nov 2003, Atlanta 26 Refined cost function •JD= ΣijtDij(t)Cij •C is the replacement cost •D is the fractional wind damage –D = 0.5 [1 +cos(π(V1-V)/(V1-V0))] •D=0 for V<V0= 25 m/s •D=1 for V>V1= 90 m/s –Evaluated every 15 min. for hours 4–6
  • 27. 5 Nov 2003, Atlanta 27 Relativepropertyvalues
  • 28. 5 Nov 2003, Atlanta 28 Experiments •Hurricane Andrew simulations starting at 00 UTC 24 Aug 1992 •Initial conditions from an earlier 6 h forecast; NCEP reanalysis; bogus vortex •4d-Var over 6 h (ending 06 UTC 24 Aug); 20 km grid; temperature increments only; simple physics •Simulations for unperturbed vs. controlled; 20 km simple physics vs. 7 km enhanced physics
  • 29. 5 Nov 2003, Atlanta 29 Unperturbed surface winds
  • 30. 5 Nov 2003, Atlanta 30 Unperturbed 4 waywinds 7 km 20 kmControlled
  • 31. 5 Nov 2003, Atlanta 31 Temperature increments
  • 32. 5 Nov 2003, Atlanta 32 Temperature increments
  • 33. 5 Nov 2003, Atlanta 33 Temperature increments
  • 34. 5 Nov 2003, Atlanta 34 Temperature increments
  • 35. 5 Nov 2003, Atlanta 35 Time evolution 00 UTC
  • 36. 5 Nov 2003, Atlanta 36 Time evolution 06 UTC
  • 37. 5 Nov 2003, Atlanta 37 Time evolution 12 UTC
  • 38. 5 Nov 2003, Atlanta 38 Time evolution 18 UTC
  • 39. 5 Nov 2003, Atlanta 39 Relative humidity 00 UTC
  • 40. 5 Nov 2003, Atlanta 40 Relative humidity 06 UTC
  • 41. 5 Nov 2003, Atlanta 41 Relative humidity 12 UTC
  • 42. 5 Nov 2003, Atlanta 42 Relative humidity 18 UTC
  • 43. 5 Nov 2003, Atlanta 43 Summary •Perturbations calculated by 4d-Var •Control path, intensity of simulated hurricane •Power requirements are huge –Higher resolution, longer lead times may help –Very large scale SSP could meet the requirements
  • 44. 5 Nov 2003, Atlanta 44 The future •More realistic experiments: resolution, physics, perturbations •Future advances in several disciplines will lead to weather control capabilities –The first experiments will not be space based control oflandfalling hurricanes! •Can legal and ethical questions be answered
  • 45. 5 Nov 2003, Atlanta 45 end •Contact: –ross@aer.com •Background: –R. N. Hoffman. Controlling the global weather. Bull. Am.Meteorol. Soc., 83(2):241--248, Feb. 2002.