2004
DOI: 10.1016/j.sigpro.2003.12.011
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The “switch-on” problem for linear time-invariant operators

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Cited by 2 publications
(2 citation statements)
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“…In our version of frequency filtering, we apply a convolution filter to the timeseries of velocity and steric SSH at each point in x , y , z . We choose to use a sinc function as the window function for this filter, because its Fourier transform is a top‐hat (see e.g., Lilly and Lettvin (2004)), so the field after ω ‐filtering, ϕ ω is given by ϕω(t)=ttwt+twϕ(t)0.17emsinc)(ffalse(tτfalse)1.1π0.17emnormaldτ, ${\phi }_{\omega }(t)=\int \nolimits_{t-{t}_{w}}^{t+{t}_{w}}\phi (t)\,\text{sinc}\left(\frac{f(t-\tau )}{1.1\,\pi }\right)\,\mathrm{d}\tau ,$ where ϕ is the unfiltered field and t w = 36 hr. The width of the sinc function is chosen to be f /1.1, where f is the local Coriolis parameter.…”
Section: Methodsmentioning
confidence: 99%
“…In our version of frequency filtering, we apply a convolution filter to the timeseries of velocity and steric SSH at each point in x , y , z . We choose to use a sinc function as the window function for this filter, because its Fourier transform is a top‐hat (see e.g., Lilly and Lettvin (2004)), so the field after ω ‐filtering, ϕ ω is given by ϕω(t)=ttwt+twϕ(t)0.17emsinc)(ffalse(tτfalse)1.1π0.17emnormaldτ, ${\phi }_{\omega }(t)=\int \nolimits_{t-{t}_{w}}^{t+{t}_{w}}\phi (t)\,\text{sinc}\left(\frac{f(t-\tau )}{1.1\,\pi }\right)\,\mathrm{d}\tau ,$ where ϕ is the unfiltered field and t w = 36 hr. The width of the sinc function is chosen to be f /1.1, where f is the local Coriolis parameter.…”
Section: Methodsmentioning
confidence: 99%
“…We choose to use a sinc function as the window function for this filter, because its fourier transform is a tophat (see e.g. Lilly and Lettvin (2004)), so the field after ω-filtering, ϕ ω is given by…”
Section: ω Filteringmentioning
confidence: 99%