1 / 53

Transit Times in the North Atlantic DWBC Measured Using the Tracer Pair 129 I/ CFC-11

Transit Times in the North Atlantic DWBC Measured Using the Tracer Pair 129 I/ CFC-11. J. N. Smith 1 , W.M. Smethie Jr. 2 , 1 Bedford Institute of Oceanography, Canada 2 Lamont Doherty Earth Observatory, USA. Labrador Sea Workshop, BIO Nov. 10-11, 2008. 129 I Tracer Characteristics.

roza
Download Presentation

Transit Times in the North Atlantic DWBC Measured Using the Tracer Pair 129 I/ CFC-11

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. Transit Times in the North Atlantic DWBC Measured Using the Tracer Pair129I/CFC-11 J. N. Smith1, W.M. Smethie Jr.2, 1 Bedford Institute of Oceanography, Canada 2 Lamont Doherty Earth Observatory, USA Labrador Sea Workshop, BIO Nov. 10-11, 2008

  2. 129I Tracer Characteristics • t1/2= 1.6 x 107 y • Measured by AMS (IsoTrace: Univ. Toronto) • 250 ml samples • $200/sample for AMS • Sample collection; cheap • Nuclear fuel reprocessing plant source – Sellafield (UK) & La Hague (France)

  3. BNFL Sellafield

  4. DSOW

  5. DSOW

  6. Smith et al., JGR, 2005

  7. Boundary Current Model Waugh and Hall, JPO, 2005 X=0 tmix Labrador Sea u X=L Line W db di Core has uniform flow, u; interior has zero flow; mixing between regions is parameterized as relaxation with time scale, tmix; a = db/di .

  8. Tracer continuity equations: Cb and Ci are tracer concentrations in boundary current and interior, respectively; S is tracer source or sink. Similar to Pickart et al. (1989); Rhein (1994); Doney and Jenkins, 1994.

  9. Transit Time Distributions: co(t) = time varying, tracer concentration at x = 0 c(x, t) = interior tracer concentration G(x, t) = TTD at location x = advective time to reach point x = Dirac delta function = Heaviside function

  10. Transit Time Distributions: co(t) = time varying, tracer concentration at x = 0 c(x, t) = interior tracer concentration G(x, t) = TTD at location x = advective time to reach point x = Dirac delta function = Heaviside function

  11. u = 2 – 5 cm/s tmix = 1 – 8 y

  12. Conclusions • Boundary current model advection times (tadv) of 3–8 y (u = 5 and 2 cm/s, respectively) and mixing times (tmix) of 1–8 y (intermediate to low mixing regimes) are all consistent with 129I/CFC-11 results for the DWBC at Line W and the Labrador Sea. • Values of u = 5 cm/s; tmix = 1 y are consistent with best-fit values in models of Pickart et al., 1989; Doney and Jenkins, 1994; core velocity is similar to mean velocities from direct measurements. However, other tracer studies imply lower spreading rates. • Line W 129I/CFC-11 results (2008-2012) will further constrain advection and mixing times.

  13. 1997 1999 2005 Transit time = 2 y to Labrador Sea;  8 y to Sta. W for DSOW

  14. Sta. W

  15. 4 1 3 2 Arctic ventilation DSOW

  16. 4 1 3 2 Arctic ventilation DSOW

  17. 4 1 3 2 Arctic ventilation DSOW

  18. 4 1 3 2 Arctic ventilation DSOW

  19. S  34.5

  20. Artic ventilation DSOW N. Atlantic ventilation

More Related