Βroadband and narrowband variability in abyssal hill bathymetry
Cristian Proistosescu (University of Washington, Harvard University) May 17, 2017 VOICE meeting LDEO, Columbia University
roadband and narrowband variability in abyssal hill bathymetry - - PowerPoint PPT Presentation
roadband and narrowband variability in abyssal hill bathymetry Cristian Proistosescu (University of Washington, Harvard University) May 17, 2017 VOICE meeting LDEO, Columbia University Pleistocene sea level variability characterized by
Cristian Proistosescu (University of Washington, Harvard University) May 17, 2017 VOICE meeting LDEO, Columbia University
1/41 kyr-1 1/23 kyr-1 1/100 kyr-1
Pleistocene sea level variability characterized by Milankovitch frequencies
(Crowley et al., 2015,Science)
Australian-Antarctic ridge
Milankovitch frequency variability identified in abyssal hill bathymetry
model bathymetry
Milankovitch frequency variability identified in abyssal hill bathymetry
(Huybers et al., 2015,Science)
Chilean Rise
Stay tuned: Comprehensive Survey
(Olive et al., 2015,Science)
Tectonic processes imply a decrease in abyssal hill wavelength with increasing spreading rate
(Goff et al., 2015,Science)
Wavelength defined as covariance length scale
(Goff 1998)
Kν : modified Bessel function C(r) = σ2 · [(r/λ)ν · Kν(r/λ)/Kν(0)] Commonly referred to as Matérn process λ
200 400 600 800 1000
bath [normalized]
5 20 40 60 80 100 120
freq
10-3 10-2 10-1
PSD [m2/cycle]
100 102 10-2 10-1 100
lag
50 100
acf
0.5 1-15
5 10 15
Matérn process is a broadband process yielding a spectral continuum
kyr km kyr km 1/kyr 1/km
S=6.6 cm/yr
ν λ 2πλ
Three parameters
σ2, ν, λ
200 400 600 800 1000
bath [normalized]
5 20 40 60 80 100 120
freq
10-3 10-2 10-1
PSD [m2/cycle]
100 10-2 10-1 100
lag
50 100
acf
0.5 1-15
5 10 15
Influence of characteristic length scale
kyr km kyr km 1/kyr 1/km
S=6.6 cm/yr
λ 2πλ
ν, λ 2πλ
200 400 600 800 1000
bath [normalized]
5 20 40 60 80 100 120
freq
10-3 10-2 10-1
PSD [m2/cycle]
100 10-2 10-1 100
lag
50 100
acf
0.5 1-15
5 10 15
Influence of smoothness
kyr km kyr km 1/kyr 1/km
S=6.6 cm/yr
λ
2, ν,
ν = 2 ν = 0
Broadband variability can arise from filtering of anomalies
freq
10-3 10-2 10-1
PSD [m2/cycle]
10-1 100 101 102 10-2 10-1 100
⇥ r2 + λ−2⇤(ν+1)/2 | {z } b(r) = εσ2(r) F−1 b(f) = F(f) · ε(f)
(Olive et al., 2015,Science)
Melt flux Crustal thickness Filter
∆h(τ) = Fw(τ) · φ(τ) ∆h
Filtering by width of emplacement
(adapted from Olive et al., 2015,Science)
Filtering by flexural compensation
λ[km] Fc[%] b(λ) = Fc(λ) · ∆h(λ) λ = τ · S
(adapted from Olive et al., 2015,Science)
Continuum variability: Summary
length scale/ frequency:
✦ Excursions above/below mean bathymetry last, on
average, λ.
consequence of integrating perturbations
Characteristic length scale
Fit to bathymetry transects
Matérn fit
ν = 0.25 2π · λ/S = 95 ± 45[kyr]
Null Hypothesis for a single transect
db/dt b
Null hypothesis distribution for 16 transects
Each Monte Carlo draw: average over 16 Matern process realizations, each with λ set to λ of profile
db/dt b
Work in progress
…provided one has access to a reasonable amount of time
significance is something one never need be without. G.A. Bamard. 1963
Glacial Cycles: Ice Sheet Dynamics filters Insolation forcing
V (f) = F(f) · I(f)
(Huybers & Tziperman 2008)
Glacial Cycles
1/41 kyr-1 1/23 kyr-1 1/100 kyr-1
Pre-whitening highlights higher frequency
1/41 kyr-1 1/23 kyr-1 1/100 kyr-1
100kyr cycle contains most of the variance
5% 18% 45%
Narrowband variability
likely mechanism is pacing by Obliquity and Precision of thresholding processes in Ice-Sheets (Calving?) or Carbon Cycle.
2006).
additional variance at lower frequencies
Last thoughts: Thresholding process faulting
likely mechanism is pacing by Obliquity and Precision of thresholding processes in Ice-Sheets (Calving?) or Carbon Cycle.
2006). Can lead to quasi-periodic features:
Abyssal hill bathymetry
(Science News, 2015)