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REPRESENTATION of TSUNAMIS in GENERALIZED HYPERSPACE Email:  * [email_address]   **kingkarn@ice.ci.ritsumei.ac.jp  Frank C. Lin* University of Maryland Eastern Shore, Princess Anne, MD. 21801, U.S.A . and Kingkarn Sookhanaphibarn** Ritsumeikan University,Kusatsu, Shiga,525-8577, Japan
PLAN of this TALK   I. First, we recapitulate a previous study* in which a  new, reliable, unequivocal, economical  and  instantaneous  response method for  DETECTING  tsunamis  at birth  using TIR images from geostationary satellites; II. We show then the representations for tsunamis can be mapped into each other by a linear transformation.  *Lin,F.C., na Nakornphanom, K.Sookhanaphibarn and Lursinsap, C: “A New Paradigm for Detecting Tsunamis by Remote Sensing”,  International   Journal of Geoinformatics , Vol.6, No.1, March, 2010, p.19-30
Fig.1: The DART Method
Shortcomings of the DART System ,[object Object],[object Object],[object Object],[object Object],[object Object]
Fig.2:  FY-2C  041226  0800  IR1
MAIN EVENT F ig.3:  Signal along latitude 1067 (Banda Aceh) at 7 am F ig.4:  Signal along latitude 1067 (Banda Aceh) at 8 am
Fig. 5: Wavelet Decomposition at Latitude 1067, 7 am   Fig. 6: Wavelet Decomposition at Latitude 1067, 8 am
TABLE I .
Fig.7: Earthquake Locations
Fig.8 : Signal from the Sumatra Aftershock at 09:00 a.m Fig.9 : Signal from the Aftershock at 10:00 a.m
Fig. 10: Detail Decomposition of Aftershock Signal at 0900 and Latitude 1067 Fig 11  Detail : Decomposition of Aftershock Signal at 1000 and   Latitude 1067
NOAA Pathfinder V - TIR Images
Declouded IR images from the NOAA V5 Pathfinder satellite   Fig 12 : Detail Wavelet Decomposition of NOAA Night Image   Fig.13 : Detail Wavelet Decomposition of NOAA Day Image
4.The Nicobar Island:  (Location 3): Fig.14 : Signal from the Nicobar Aftershock at 0900  LAT 1042 Fig.15 : Signal from the Nicobar Aftershock at 1000 LAT 1042
Wavelet Decomposition,Nicobar Fig.16 : Wavelet Decomposition at Nicobar at 0900 LAT 1042   Fig.17 : Wavelet Decomposition at Nicobar at 1000 LAT 1042
CASE 1:ANDAMAN-1 and ANDAMAN-4   LAT 1012 :  (Location 4 &7): FIG.18 : ANDAMAN-1 & 4 Signal 0600 LAT 1012   Fig.19 : Wavelet Decomposition of ANDAMAN-1 & 4 at 0600, LAT 1012
ANDAMAN-4   0700 LAT 1012   Fig.:20 : Signal for ANDAMAN-4  0700 LAT 1012 Fig.21 : Wavelet Decomposition for ANDAMAN-4  0700 LAT 1012
At 0800, another tsunami signal is detected at the Andaman-1 epicenter   Fig.22 : Signal for ANDAMAN-1 0800 LAT 1012   Fig.23 : Wavelet Decomposition for ANDAMAN-1 0800 LAT 1012 LON 978
CASE 2:  ANDAMAN-2 , LAT  978 : (Location  5 ): Fig.24 : Satellite Photo of Epicenter for ANDAMAN-2 0800 LON 958
No Tsunami Cases : Fig.25 : Signal for ANDAMAN-2 0700 LAT 978   Fig.26 : Wavelet Decomposition of ANDAMAN-2 0700 LAT 978
No Tsunami Cases: Fig. 27 : Signal of ANDAMAN-2 0800 LAT 978 LON 958   Fig.28 :  Wavelet Decomposition for ANDAMAN-2 0800  LAT 978
CASE 3: ANDAMAN-3,LAT 965 (Location 6): Fig.29 : Signal for ANDAMAN-3 10:56 LAT 965   Fig:30 : Wavelet Decomposition for ANDAMAN-3 10:56 LAT 965
ANDAMAN-3 Lat.965 11:29  (No Tsunami Signal) Fig.31 : Signal for ANDAMAN-3 11:29 LAT 965 LON 955   Fig.32 : Wavelet Decomposition for ANDAMAN-3 11:29 LAT 965 LON 955
Tsunami Magnitude & Intensity ,[object Object],[object Object],[object Object],[object Object],Intensity:  I t  = log 2 (√2 * S)   (2)
Infrared Tsunami vs Earthquake Magnitude ,[object Object]
Tsunami Index  I ,[object Object]
Earthquake vs Infrared Tsunami Index at Epicenter
System Modules ,[object Object],[object Object],[object Object],[object Object]
Representations of Tsunamis : ,[object Object],[object Object],[object Object],[object Object],[object Object]
The  Vector  Representation   We can represent a tsunami by a vector , with the components x, y, z, t, M e , M t  and P x  (pixel brightness).
Phase space (Iida) & Infrared Space (Lin) Representations ,[object Object],[object Object],Lin  et al  : M t  = 9.2299–0.0592*Me
Linear Transformation ,[object Object],[object Object],[object Object]
CONCLUSION ,[object Object],[object Object]
Questions, Comments??

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RepresentationOfTsunamisInGeneralizedHyperspace.ppt

  • 1. REPRESENTATION of TSUNAMIS in GENERALIZED HYPERSPACE Email: * [email_address] **kingkarn@ice.ci.ritsumei.ac.jp Frank C. Lin* University of Maryland Eastern Shore, Princess Anne, MD. 21801, U.S.A . and Kingkarn Sookhanaphibarn** Ritsumeikan University,Kusatsu, Shiga,525-8577, Japan
  • 2. PLAN of this TALK I. First, we recapitulate a previous study* in which a new, reliable, unequivocal, economical and instantaneous response method for DETECTING tsunamis at birth using TIR images from geostationary satellites; II. We show then the representations for tsunamis can be mapped into each other by a linear transformation. *Lin,F.C., na Nakornphanom, K.Sookhanaphibarn and Lursinsap, C: “A New Paradigm for Detecting Tsunamis by Remote Sensing”, International Journal of Geoinformatics , Vol.6, No.1, March, 2010, p.19-30
  • 4.
  • 5. Fig.2: FY-2C 041226 0800 IR1
  • 6. MAIN EVENT F ig.3: Signal along latitude 1067 (Banda Aceh) at 7 am F ig.4: Signal along latitude 1067 (Banda Aceh) at 8 am
  • 7. Fig. 5: Wavelet Decomposition at Latitude 1067, 7 am Fig. 6: Wavelet Decomposition at Latitude 1067, 8 am
  • 10. Fig.8 : Signal from the Sumatra Aftershock at 09:00 a.m Fig.9 : Signal from the Aftershock at 10:00 a.m
  • 11. Fig. 10: Detail Decomposition of Aftershock Signal at 0900 and Latitude 1067 Fig 11 Detail : Decomposition of Aftershock Signal at 1000 and Latitude 1067
  • 12. NOAA Pathfinder V - TIR Images
  • 13. Declouded IR images from the NOAA V5 Pathfinder satellite Fig 12 : Detail Wavelet Decomposition of NOAA Night Image Fig.13 : Detail Wavelet Decomposition of NOAA Day Image
  • 14. 4.The Nicobar Island: (Location 3): Fig.14 : Signal from the Nicobar Aftershock at 0900 LAT 1042 Fig.15 : Signal from the Nicobar Aftershock at 1000 LAT 1042
  • 15. Wavelet Decomposition,Nicobar Fig.16 : Wavelet Decomposition at Nicobar at 0900 LAT 1042 Fig.17 : Wavelet Decomposition at Nicobar at 1000 LAT 1042
  • 16. CASE 1:ANDAMAN-1 and ANDAMAN-4 LAT 1012 : (Location 4 &7): FIG.18 : ANDAMAN-1 & 4 Signal 0600 LAT 1012 Fig.19 : Wavelet Decomposition of ANDAMAN-1 & 4 at 0600, LAT 1012
  • 17. ANDAMAN-4 0700 LAT 1012 Fig.:20 : Signal for ANDAMAN-4 0700 LAT 1012 Fig.21 : Wavelet Decomposition for ANDAMAN-4 0700 LAT 1012
  • 18. At 0800, another tsunami signal is detected at the Andaman-1 epicenter Fig.22 : Signal for ANDAMAN-1 0800 LAT 1012 Fig.23 : Wavelet Decomposition for ANDAMAN-1 0800 LAT 1012 LON 978
  • 19. CASE 2: ANDAMAN-2 , LAT 978 : (Location 5 ): Fig.24 : Satellite Photo of Epicenter for ANDAMAN-2 0800 LON 958
  • 20. No Tsunami Cases : Fig.25 : Signal for ANDAMAN-2 0700 LAT 978 Fig.26 : Wavelet Decomposition of ANDAMAN-2 0700 LAT 978
  • 21. No Tsunami Cases: Fig. 27 : Signal of ANDAMAN-2 0800 LAT 978 LON 958 Fig.28 : Wavelet Decomposition for ANDAMAN-2 0800 LAT 978
  • 22. CASE 3: ANDAMAN-3,LAT 965 (Location 6): Fig.29 : Signal for ANDAMAN-3 10:56 LAT 965 Fig:30 : Wavelet Decomposition for ANDAMAN-3 10:56 LAT 965
  • 23. ANDAMAN-3 Lat.965 11:29 (No Tsunami Signal) Fig.31 : Signal for ANDAMAN-3 11:29 LAT 965 LON 955 Fig.32 : Wavelet Decomposition for ANDAMAN-3 11:29 LAT 965 LON 955
  • 24.
  • 25.
  • 26.
  • 27. Earthquake vs Infrared Tsunami Index at Epicenter
  • 28.
  • 29.
  • 30. The Vector Representation We can represent a tsunami by a vector , with the components x, y, z, t, M e , M t and P x (pixel brightness).
  • 31.
  • 32.
  • 33.

Notas do Editor

  1. 1.Instantaneous – Mentawai 2010 2 False Positive 3.Expensive 4.Not Available..