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    <titleInfo>
        <title>Shear dispersion in the thermocline and the saline intrusion</title>
    </titleInfo>
    <name type="personal" ID="hwo1">
        <namePart type="family">Ou</namePart>
        <namePart type="given">Hsien Wang</namePart>
        <role>
            <roleTerm type="text">author</roleTerm>
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        <affiliation>Columbia University. Lamont-Doherty Earth Observatory</affiliation>
        <affiliation>Columbia University. Earth and Environmental Sciences</affiliation>
    </name>
    <name type="personal">
        <namePart type="family">Guan</namePart>
        <namePart type="given">Xiaorui</namePart>
        <role>
            <roleTerm type="text">author</roleTerm>
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    </name>
    <name type="personal">
        <namePart type="family">Chen</namePart>
        <namePart type="given">Dake</namePart>
        <role>
            <roleTerm type="text">author</roleTerm>
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    </name>
    <name type="corporate">
        <namePart>Columbia University. Lamont-Doherty Earth Observatory</namePart>
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        <dateIssued encoding="w3cdtf" keyDate="yes">2012</dateIssued>
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    <abstract>Over the mid-Atlantic shelf of the North America, there is a pronounced shoreward intrusion of the saltier slope water along the seasonal thermocline, whose genesis remains unexplained. Taking note of the observed broad-band baroclinic motion, we postulate that it may propel the saline intrusion via the shear dispersion. Through an analytical model, we first examine the shear-induced isopycnal diffusivity (&quot;shear diffusivity&quot; for short) associated with the monochromatic forcing, which underscores its varied even anti-diffusive short-term behavior and the ineffectiveness of the internal tides in driving the shear dispersion. We then derive the spectral representation of the long-term &quot;canonical&quot; shear diffusivity, which is found to be the baroclinic power band-passed by a diffusivity window in the log-frequency space. Since the baroclinic power spectrum typically plateaus in the low-frequency band spanned by the diffusivity window, canonical shear diffusivity is simply 1/8 of this low-frequency plateau — independent of the uncertain diapycnal diffusivity. Applied to the mid-Atlantic shelf, this canonical shear diffusivity is about 20 m2 s−1, which is sufficient to account for the observed tracer dispersion or saline intrusion in the thermocline.</abstract>
    <subject>
        <topic>Physical oceanography</topic>
    </subject>
    <relatedItem type="host">
        <titleInfo>
            <title>Continental Shelf Research</title>
        </titleInfo>
        <part>
            <detail type="volume">
                <number>43</number>
            </detail>
            <extent unit="page">
                <start>1</start>
                <end>9</end>
            </extent>
            <date>2012-07-15</date>
        </part>
        <identifier type="doi">http://dx.doi.org/10.1016/j.csr.2012.03.009</identifier>
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    <identifier type="hdl">http://hdl.handle.net/10022/AC:P:14395</identifier>
    
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        <recordCreationDate encoding="w3cdtf">2012-08-15 13:59:29 -0400</recordCreationDate>
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