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Earth’s Deep Water Cycle Suzan van der Lee Northwestern University

Earth’s Deep Water Cycle

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Earth’s Deep Water Cycle. Suzan van der Lee Northwestern University. Feng et al. (2007); Van der Lee and Wiens (EDWC). mantle wedge seismically slow and wet, dry below?. Rupke et al. (EDWC). Mantle outgassing 90% efficient; at least 10% stays in mantle, and likely more in slab. - PowerPoint PPT Presentation

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Page 1: Earth’s Deep Water Cycle

Earth’s Deep Water Cycle

Suzan van der Lee

Northwestern University

Page 2: Earth’s Deep Water Cycle

Fen

g et

al.

(200

7); V

an d

er L

ee a

nd W

iens

(E

DW

C)

mantle wedge seismically slow and wet, dry below?

Page 3: Earth’s Deep Water Cycle

Mantle outgassing 90% efficient; at least 10% stays in mantle, and likely more in slab

Rupke et al. (EDWC)

Page 4: Earth’s Deep Water Cycle

Son

g an

d H

elm

berg

er (

ED

WC

)

lvz on 410 (red o) right next to “normal” mantle (white o)

Page 5: Earth’s Deep Water Cycle

Kar

ato

et a

l. (E

DW

C)

melt on 410 from upwelling saturated wadselyite, but…

Page 6: Earth’s Deep Water Cycle

Hirschmann et al. (EDWC)

< 7 kmPredicted melt layer thinner than observed lvz

wd-->ol transition thickens with increasing H2O at undersaturated conditions

Page 7: Earth’s Deep Water Cycle

0 ppm

200 ppm

500 ppm

1000 ppm

35

40

45

30

25

20

15

10

5

0

Phase transition

interval (km)

velocity

(after Wood, 1995)

>25 km

Calculations at D=20 suggest that ol-->wd transition can be very thick at only 0.1 wt % water

Page 8: Earth’s Deep Water Cycle

VSL, Italy PAB, Spain KEG, Egypt

410

660

dep

th (k

m)

f = 0

.75 H

zf =

0.6

2 H

zf =

0.5

Hz

f = 0

.4 H

zf =

0.3

5 H

zf =

0.3

Hz

f = 0

.25 H

zf =

0.2

Hz

f = 0

.15 H

z

f = 0

.75 H

zf =

0.6

2 H

zf =

0.5

Hz

f = 0

.4 H

zf =

0.3

5 H

zf =

0.3

Hz

f = 0

.25 H

zf =

0.2

Hz

f = 0

.15 H

z

410

660

f = 0

.75 H

zf =

0.6

2 H

zf =

0.5

Hz

f = 0

.4 H

zf =

0.3

5 H

zf =

0.3

Hz

f = 0

.25 H

zf =

0.2

Hz

f = 0

.15 H

z

Water would thus be an explanation for puzzling receiver functions, but…

Page 9: Earth’s Deep Water Cycle

Hirs

chm

ann

et a

l. (E

DW

C)

<15 km

With D=5 and 0.1 wt % H2O transition would be less than 15 km thick

Page 10: Earth’s Deep Water Cycle

Conder and Wiens (2006); Roth et al. (1999); Van der Lee and Wiens (EDWC)

V low and Q very low in mantle wedge --> water

V low, but Q high below 200 km --> warm

Page 11: Earth’s Deep Water Cycle

velocity attenuation

temperature

water

major element chemistry

partial melting

grain-size

large*

modest*

small1

potentially large2

very small

large

large

very small

small*

small

Shito et al. (EDWC)

Separate effects of water from other effects

Page 12: Earth’s Deep Water Cycle

Shi

to e

t al.

(ED

WC

)

Water above 400 km, from upwelling TZ or from slab

Still some trade-off btw w and T

Page 13: Earth’s Deep Water Cycle

Use other seismic measurements to evaluate the relative role of w and T, such as transition-zone discontinuity properties:

Sm

yth

and

Jaco

bsen

(20

06)

Page 14: Earth’s Deep Water Cycle

Bra

unm

iller

et a

l. (E

DW

C)

TZ thickens but ol-->wd does not: deep SAm mantle dry (or saturated)

Page 15: Earth’s Deep Water Cycle

Suetsugu et al. (EDWC)

Vp and 660: >1 wt % water near slab

Page 16: Earth’s Deep Water Cycle

Courtier and Revenaugh (EDWC)

410, 520, and Vs: >0.2 wt % water

Page 17: Earth’s Deep Water Cycle

low Vs: < 1 wt% water

low Vs above slab in top of lower mantle

VdLee & Frederiksen (2005)

Grand (2002)

Page 18: Earth’s Deep Water Cycle

Inoue et al. (EDWC)

Experiments show that Shy-B is stable in TZ and cool slab

Page 19: Earth’s Deep Water Cycle

Komabayashi (EDWC)

Calculations show that abc phases are stable throughout upper mantle in cool slab; breakdown occurs in top of lower mantle.

Page 20: Earth’s Deep Water Cycle

Hydrous TZ likely less densethan dry TZ, and:

Water lowers the viscosity by 4-5 orders of magnitude, at least above 300 km.

Hydrous mantle can well up and hydrate lithosphere.

Karato and Jung (2003);

Karato (EDWC)

Page 21: Earth’s Deep Water Cycle

Deformation model Temperature and water-sensitive yield and thermal-mechanical feedback

Ocean continent Boundary

Sediment loading

Seafloor age turned into temperatures70 km thick Lithosphere cross section shown

Mid Atlantic

ridge

Regenauer-Lieb et al. (2001)

Page 22: Earth’s Deep Water Cycle

lithosphere

wet rheology dry rheology time0 km --

100 km --

Regenauer-Lieb et al. (2001)

lithosphere breaks only in wet conditions; subduction of dense lithosphere enabled.

Page 23: Earth’s Deep Water Cycle

Connecting past and future episodes of subduction

200-300 m.y.

subducting plate

(Farallon)

continent(N America)

subducti

ng plate

(Atla

ntic?)

continent(N America)

-- 660 km --

-- 0 km --

Page 24: Earth’s Deep Water Cycle

Connecting past and future episodes of subduction

Page 25: Earth’s Deep Water Cycle

Connecting past and future episodes of subduction

Page 26: Earth’s Deep Water Cycle

Connecting past and future episodes of subduction

Page 27: Earth’s Deep Water Cycle

Connecting past and future episodes of subduction

Page 28: Earth’s Deep Water Cycle

Connecting past and future episodes of subduction

Page 29: Earth’s Deep Water Cycle

Present

Page 30: Earth’s Deep Water Cycle

Conclusions

1. Deep water cycle may sustain plate tectonics over many Gy.

2. Water in mantle is detectable in various ways

seismic V from tomography or triplication branches

Q/attenuation

discontinuity depths and properties

3. More work is needed

mineral physics: elasticity at p, T, and C

seismology: benchmarking, denser data (USArray!)