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        <title>On the Ill-Posedness of the Prandtl Equation</title>
        <author>David Gérard-Varet</author>
        <author>Emmanuel Dormy</author>
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          <title>On the Ill-Posedness of the Prandtl Equation</title>
          <date>2010</date>
          <publisher>Journal of the American Mathematical Society / arXiv</publisher>
          <idno type="DOI">10.1090/S0894-0347-09-00652-3</idno>
          <idno type="arXiv">0904.0434</idno>
          <idno type="record">gerardvaret2010-prandtl-illposedness</idno>
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          <note type="rights">arxiv-open</note>
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        <label>existence</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>ill-posedness of the Prandtl boundary layer equation</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t2" type="method" ana="#method" resp="#paper">
        <label>mathematical-proof</label>
        <term>mathematical-proof</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>mechanisms</label>
        <term>THE EXPECTED ANSWER IS STATED BEFORE IT IS OVERTURNED: on the strength of the inviscid result the authors say it seems reasonable to bet on well-posedness, and then show the equation is linearly ill-posed in that very setting</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t4" type="mechanisms" ana="#mechanisms[1]" resp="#tagger" cert="0.95">
        <label>mechanisms</label>
        <term>the destabilisation is attributed to TWO ingredients together - viscosity, and critical points in the base velocity profile - and the authors immediately state what that conjunction buys them: the result does not contradict the positive results for the inviscid case or for monotonic data</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t5" type="mechanisms" ana="#mechanisms[2]" resp="#tagger" cert="0.85">
        <label>mechanisms</label>
        <term>THE PDE QUESTION IS REDUCED TO A CONDITION ON AN ORDINARY DIFFERENTIAL EQUATION: an asymptotic analysis in the high tangential frequency limit turns ill-posedness for the linearised system into a spectral condition for a reduced ODE</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t6" type="mechanisms" ana="#mechanisms[3]" resp="#tagger" cert="0.95">
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        <term>the instability is located at a SCALE rather than at a place: it happens at high tangential frequencies with a typical time that shrinks with them, and at that timescale the time dependence of the base velocity does not matter - which lets the authors replace the real equation with a simpler frozen one</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>mechanisms</label>
        <term>A FREE PARAMETER IS ADDED TO THE ANSATZ PRECISELY BECAUSE THE SYSTEM IS OVERDETERMINED - the jump and boundary conditions supply too many constraints - and the paper says that this is what justifies introducing it</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <term>the corrector&#x27;s ROLE IS STATED AS CANCELLATION: the inviscid solution is not smooth at the critical point, and the shear layer term, which concentrates there, exists to cancel the discontinuities the regular part leaves behind</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <term>the sign of a second derivative would split the argument in two, and a change of variables collapses the split: if the condition holds for one sign then a transformed pair satisfies the other, so BOTH CASES yield a solution with the property the instability needs</term>
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        <term>WELL-POSEDNESS IN THE ANALYTIC SETTING IS PROVED IN THE SAME PAPER, as a foil: the Cauchy problem for the linearised equation is locally well-posed there, which is what makes the Sobolev result a statement about the function space rather than about the equation</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t11" type="mechanisms" ana="#mechanisms[8]" resp="#tagger" cert="0.95">
        <label>mechanisms</label>
        <term>the analytical result is accompanied by numerical computation whose stated purpose is to show the mechanism is EFFECTIVE rather than merely possible</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t12" type="limitations" ana="#limitations[0]" resp="#tagger">
        <label>the relevance of the asymptotics in Lp and in the absence of Rayleigh instabilities remains open</label>
        <note>what this limits: the asymptotic result&#x27;s reach: THE RELEVANCE OF THIS ASYMPTOTICS IN Lp, OR ITS RELEVANCE IN THE ABSENCE OF RAYLEIGH INSTABILITIES, ARE STILL OPEN ISSUES</note>
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        <label>The negative result is confined to the viscous Sobolev setting and leaves the known positive (inviscid and monotonic-data) results intact.</label>
        <note>what this limits: the ill-posedness result, which is confined to its setting: IT DOES NOT CONTRADICT THE POSITIVE RESULTS OBTAINED IN THE INVISCID CASE AND FOR MONOTONIC DATA</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>The refined approximation behind the stronger part of the theorem could not be obtained for general base profiles, forcing a restriction to special quadratic-near-the-critical-point profiles.</label>
        <note>what this limits: the stronger part of the theorem: Quotation withheld general base profiles</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>The originator of the model is cited as doubting that it holds uniformly, and the paper states outright that the validity of the asymptotics is not clear.</label>
        <note>what this limits: the boundary-layer asymptotics as a description of the flow: the paper states its validity is not clear and that physicists including Prandtl himself emphasised it may not hold uniformly in space and time</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>The empirical support for the description is bounded to one side of the separation zone, and the paper says which side.</label>
        <note>what this limits: experimental agreement with the boundary-layer description: it is stated to fit many experiments upstream from the separation zone, which does not extend to the separated region</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>The instability mechanism is derived with the time variation of the base velocity dropped, and carrying it back to the real system is stated to require modification.</label>
        <note>what this limits: the mechanism as described in section 2: it is derived for a base velocity whose time variation is neglected, and accounting for the original system requires modifications</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>Prandtl equation</label>
        <term>Prandtl equation</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <term>Prandtl equations</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>inviscid version</label>
        <term>inviscid version</term>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>finite loss of x-derivatives</label>
        <term>finite loss of x-derivatives</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>(weakly) well-posed</label>
        <term>(weakly) well-posed</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>strong destabilization mechanism</label>
        <term>strong destabilization mechanism</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>high tangential frequencies</label>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <term>instability process</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>singular perturbation problem</label>
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        <note>about this quote: THE TERM IS NOT IN THE QUOTE - text extraction moved part of the quote&#x27;s first sentence out of it: the words &#x27;yields a singular perturbation problem&#x27; now stand just after the quote.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t55" type="concepts" ana="#concepts[41]" resp="#paper" cert="0.95">
        <label>inviscid eigenelements</label>
        <term>inviscid eigenelements</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t56" type="concepts" ana="#concepts[42]" resp="#paper" cert="0.95">
        <label>strong instability</label>
        <term>strong instability</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t57" type="concepts" ana="#concepts[43]" resp="#paper" cert="0.95">
        <label>heteroclinic orbits</label>
        <term>heteroclinic orbits</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t58" type="concepts" ana="#concepts[44]" resp="#paper" cert="0.95">
        <label>holomorphic solution</label>
        <term>holomorphic solution</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t59" type="concepts" ana="#concepts[45]" resp="#paper" cert="0.95">
        <label>complex change of variable</label>
        <term>complex change of variable</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t60" type="concepts" ana="#concepts[46]" resp="#paper" cert="0.95">
        <label>formal analysis</label>
        <term>formal analysis</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t61" type="concepts" ana="#concepts[47]" resp="#paper" cert="0.95">
        <label>numerical illustrations</label>
        <term>numerical illustrations</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t62" type="concepts" ana="#concepts[48]" resp="#paper" cert="0.95">
        <label>Evans function</label>
        <term>Evans function</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t63" type="concepts" ana="#concepts[49]" resp="#paper" cert="0.95">
        <label>shooting method</label>
        <term>shooting method</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>Runge-Kutta scheme</label>
        <term>Runge-Kutta scheme</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t65" type="concepts" ana="#concepts[51]" resp="#paper" cert="0.95">
        <label>Newton-Raphson procedure</label>
        <term>Newton-Raphson procedure</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t66" type="concepts" ana="#concepts[52]" resp="#paper" cert="0.95">
        <label>direct simulations</label>
        <term>direct simulations</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t67" type="concepts" ana="#concepts[53]" resp="#paper" cert="0.95">
        <label>finite differences</label>
        <term>finite differences</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t68" type="concepts" ana="#concepts[54]" resp="#paper" cert="0.95">
        <label>stretched grid</label>
        <term>stretched grid</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t69" type="concepts" ana="#concepts[55]" resp="#paper" cert="0.95">
        <label>Crank-Nicholson scheme</label>
        <term>Crank-Nicholson scheme</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t70" type="concepts" ana="#concepts[56]" resp="#paper" cert="0.95">
        <label>initial random data</label>
        <term>initial random data</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t71" type="concepts" ana="#concepts[57]" resp="#paper" cert="0.95">
        <label>excellent agreement</label>
        <term>excellent agreement</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t72" type="unhoused_relations" ana="#unhoused_relations[0]" resp="#tagger" cert="0.95">
        <label>vorticity field → inviscid limit</label>
        <note>Lack of uniform vorticity bounds is the main mathematical difficulty in taking the inviscid limit. Difficulty-for is absent from the governed relation types.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t73" type="unhoused_relations" ana="#unhoused_relations[1]" resp="#tagger" cert="0.95">
        <label>parabolic scaling → normal direction</label>
        <note>The boundary-layer asymptotics applies a parabolic scaling in the normal direction. Applied-in-direction is absent from the governed relation types.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t74" type="unhoused_relations" ana="#unhoused_relations[2]" resp="#tagger" cert="0.95">
        <label>loss of one derivative → standard energy estimates</label>
        <note>The unbalanced loss of one tangential derivative prevents standard energy estimates from applying. Prevents is absent from the governed relation types.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t75" type="unhoused_relations" ana="#unhoused_relations[3]" resp="#tagger" cert="0.95">
        <label>Rayleigh instability → formal asymptotics</label>
        <note>Rayleigh instability was used in prior work to show that the boundary-layer asymptotics does not always hold in a Sobolev space. Invalidates-in-a-setting is absent.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t76" type="unhoused_relations" ana="#unhoused_relations[4]" resp="#tagger" cert="0.95">
        <label>finite loss of x-derivatives → (weakly) well-posed</label>
        <note>Only finite tangential derivative loss is the stated basis for calling the inviscid Cauchy problem weakly well-posed. Supports-status is absent from the governed types.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t77" type="unhoused_relations" ana="#unhoused_relations[5]" resp="#tagger" cert="0.95">
        <label>spectral condition → ill-posedness</label>
        <note>Ill-posedness of the PDE is reduced to a spectral condition for a reduced ODE. Reduces-to is absent from the governed relation types.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t78" type="unhoused_relations" ana="#unhoused_relations[6]" resp="#tagger" cert="0.95">
        <label>Evans function → spectral condition</label>
        <note>The spectral condition is reformulated with an Evans function for numerical checking. Reformulates is absent from the governed relation types. — the relation stated: Quotation withheld 5.1 Quotation withheld</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t79" type="unhoused_relations" ana="#unhoused_relations[7]" resp="#tagger" cert="0.95">
        <label>shooting method → Newton-Raphson procedure</label>
        <note>Backward shooting supplies the function on which Newton-Raphson locates a zero. Sequential-input-to is absent from the governed relation types.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t80" type="unhoused_relations" ana="#unhoused_relations[8]" resp="#tagger" cert="0.95">
        <label>finite differences → Crank-Nicholson scheme</label>
        <note>The direct simulation combines finite-difference spatial discretization with Crank-Nicholson time stepping. Combined-with is absent from the governed relation types.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t81" type="senses" ana="#senses[0]" resp="#tagger" cert="1.0">
        <label>ill-posedness - LINEAR, and only that: the theorem is about the linearization around solutions with non-degenerate critical points, so the bare claim &#x27;the Prandtl equation is ill-posed&#x27; drops the word that bounds the result</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t82" type="senses" ana="#senses[1]" resp="#tagger" cert="1.0">
        <label>the expected answer - STATED AND THEN OVERTURNED: the paper records that the inviscid result made well-posedness the reasonable bet, and then proves the opposite in this framework</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t83" type="senses" ana="#senses[2]" resp="#tagger" cert="1.0">
        <label>the source of instability - VISCOSITY, which is the term usually read as stabilising: the paper names viscosity and critical points in the base profile as the two ingredients</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t84" type="senses" ana="#senses[3]" resp="#tagger" cert="0.95">
        <label>Inviscid-limit difficulty - no uniform vorticity bound as viscosity vanishes, corresponding physically to a boundary layer</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t85" type="senses" ana="#senses[4]" resp="#tagger" cert="0.95">
        <label>Prandtl asymptotics - formally natural but not uniformly valid because boundary-layer separation can occur</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t86" type="senses" ana="#senses[5]" resp="#tagger" cert="0.95">
        <label>Tangential regularity obstacle - one derivative is lost without horizontal diffusion to balance it</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t87" type="senses" ana="#senses[6]" resp="#tagger" cert="0.95">
        <label>Analytic setting - sufficient for local boundary-layer justification but filters instability mechanisms</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t88" type="senses" ana="#senses[7]" resp="#tagger" cert="0.95">
        <label>Inviscid Cauchy problem - characteristic solution with finite tangential derivative loss and weak well-posedness</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t89" type="senses" ana="#senses[8]" resp="#tagger" cert="0.95">
        <label>Viscous destabilization - viscosity and non-degenerate critical points jointly underlie the Sobolev failure</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t90" type="senses" ana="#senses[9]" resp="#tagger" cert="0.95">
        <label>Strong linear ill-posedness - high-frequency perturbations grow on a square-root-frequency timescale</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t91" type="senses" ana="#senses[10]" resp="#tagger" cert="0.95">
        <label>Spectral reduction - PDE ill-posedness is reduced to a condition on a lower-dimensional ODE</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t92" type="senses" ana="#senses[11]" resp="#tagger" cert="0.95">
        <label>Spectral-condition problem - existence of a heteroclinic orbit for the reduced ordinary differential equation</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t93" type="senses" ana="#senses[12]" resp="#tagger" cert="0.95">
        <label>Evans-function computation - shooting with Runge-Kutta integration followed by Newton-Raphson root finding</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t94" type="senses" ana="#senses[13]" resp="#tagger" cert="0.95">
        <label>Direct numerical test - finite differences on a stretched grid and Crank-Nicholson time stepping from random data</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t95" type="senses" ana="#senses[14]" resp="#tagger" cert="0.95">
        <label>Numerical confirmation - eigenvalue and eigenmode comparisons agree with theory and show the mechanism dominates linear dynamics</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t96" type="claim_relations" ana="#claim_relations[0]" resp="#tagger">
        <label>extends → prior well-posedness results for the Prandtl equation (analytic or monotone data)</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t97" type="claim_relations" ana="#claim_relations[1]" resp="#tagger">
        <label>builds-on → reference [8] (analysis of the inviscid version of the Prandtl equation)</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t98" type="claim_relations" ana="#claim_relations[2]" resp="#tagger">
        <label>builds-on → reference [8] (study of the inviscid spectral problem and its evolution equation)</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t99" type="concept_edges" ana="#concept_edges[0]" resp="#tagger">
        <label>viscosity —causes→ ill-posedness</label>
        <term>viscosity</term>
        <term>ill-posedness</term>
        <note>strength of the relation: 1</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t100" type="concept_edges" ana="#concept_edges[1]" resp="#tagger">
        <label>critical point —causes→ ill-posedness</label>
        <term>critical point</term>
        <term>ill-posedness</term>
        <note>strength of the relation: 1</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t101" type="content_tags" ana="#content_tags.findings[0]" resp="#tagger">
        <label>The Prandtl equation is linearly ill-posed in Sobolev-type spaces, shown by constructing unstable quasimodes at high tangential frequencies around solutions with non-degenerate critical points.</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t102" type="content_tags" ana="#content_tags.findings[1]" resp="#tagger">
        <label>Strikingly, the strong instability is caused by VISCOSITY — consistent with well-posedness of the inviscid version of the equation.</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t103" type="content_tags" ana="#content_tags.definitions[0]" resp="#tagger">
        <label>Prandtl equation</label>
        <term>Prandtl equation</term>
        <note>about this quote: QUOTE RECOVERED FROM THE PAPER&#x27;S OWN CHARACTERS. The recorded quote was LETTERS-ONLY IDENTICAL to this stretch of the staged text but not an exact substring of it - spaces, hyphens, ligature glyphs or mathematical operators differed, so it could never anchor. This is the file&#x27;s own text between the same two letters: not produced by a rule about the damage, copied out of the file. Round-trip checked (the recovered span is letters-only equal to the original) and length-checked. The text as originally recorded is kept in evidence as extracted.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t104" type="content_tags" ana="#content_tags.definitions[1]" resp="#tagger">
        <label>ill-posedness</label>
        <term>ill-posedness</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t105" type="content_tags" ana="#content_tags.definitions[2]" resp="#tagger">
        <label>inviscid limit</label>
        <term>inviscid limit</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
    </spanGrp>
  </standOff>
  <text>
    <body>
      <p><note type="rights">The full text of this article is not redistributable, so it is
      not included here. The evidence sentences are withheld with it; the tag layer and its
      grounding status remain. The article itself is at https://doi.org/10.1090/S0894-0347-09-00652-3.</note></p>
    </body>
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