On the Ill-Posedness of the Prandtl Equation

David Gérard-Varet, Emmanuel Dormy · Journal of the American Mathematical Society / arXiv · 2010 · mathematics · 10.1090/S0894-0347-09-00652-3 · record gerardvaret2010-prandtl-illposedness
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Where this record's text came from. faceted 2026-08 by reading the locally held text (pdftext); every evidence string verified as an exact substring of that text before merging. Claim type is coded existence — the theorem asserts that strong linear ill-posedness (and the unstable quasimodes realising it) exists — but the paper also states an explicit mechanism ('Quotation withheld.'), so mechanism would be a defensible second reading. method is mathematical-proof, though the paper adds a numerical component ('A numerical study of this instability is also provided.'). The second limitation quote is deliberately truncated mid-sentence: in the PDF extraction the sentence 'So far, we have not managed to improve the approximation ... for general us. This explains the technical restriction µ ∈ [0, 1/2) of part i).' is interleaved with inline-math fragments, so only the leading clause is quotable character-for-character. Displayed equations throughout the extraction are heavily scrambled; all quoted material is from running prose. 2026-08-14, 2026-08-16 and 2026-08-28 schema-0.3 passes: every quote verified as an exact substring of the staged text and anchored at merge time; concept terms verified present; every edge endpoint an existing node.
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Other fields define these differently the same word, defined another way in another discipline
viscosity 2 fields

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Prandtl equation boundary layer ill-posedness Cauchy problem Sobolev spaces Navier-Stokes equations viscosity boundary layer separation critical point inviscid limit no-slip boundary condition vorticity field boundary layer phenomenon parabolic scaling normal direction Prandtl equations formal asymptotics Prandtl model functional spaces tangential variable x derivatives loss of one derivative horizontal diffusion term standard energy estimates analytic framework Rayleigh instability inviscid version finite loss of x-derivatives (weakly) well-posed strong destabilization mechanism base velocity profile monotonic data shear velocity profile linearization analytic regularity high tangential frequencies unstable quasimodes spectral condition reduced ODE instability process singular perturbation problem inviscid eigenelements strong instability heteroclinic orbits holomorphic solution complex change of variable formal analysis numerical illustrations Evans function shooting method Runge-Kutta scheme Newton-Raphson procedure direct simulations finite differences stretched grid Crank-Nicholson scheme initial random data excellent agreement 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 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 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 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 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 the corrector'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 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 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 the analytical result is accompanied by numerical computation whose stated purpose is to show the mechanism is EFFECTIVE rather than merely possible Prandtl ill-posed instability Sobolev viscous equation Navier-Stokes analytic mathematical-proof

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facettagfieldconf.whose words
claim_typeexistence
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claim_typethe paper's words
phenomenonill-posedness of the Prandtl boundary layer equation
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phenomenonthe paper's words
methodmathematical-proof
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methodthe paper's words
mechanismsmechanisms
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mechanisms[0]0.95the tagger's words
mechanismsmechanisms
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mechanisms[2]0.85the tagger's words
mechanismsmechanisms
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mechanismsmechanisms
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mechanisms[4]0.95the tagger's words
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mechanisms[5]0.95the tagger's words
mechanismsmechanisms
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about this quote: 2026-08-16: A FRAGMENT IS DISPLACED INSIDE THIS QUOTE - damage shape 5, a word-order scramble. The staged text reads "satisfies the above system. In both - m tau < 0. cases, back to the original system (2.6), condition (SC) gives a solution (tau, V ) with". The fragment "Im tau < 0" belongs at the END of the sentence, completing "gives a solution (tau, V) with Im tau < 0"; the extraction has lifted it out and dropped it between "In both" and "cases". Read as: "In both cases, back to the original system (2.6), condition (SC) gives a solution (tau, V) with Im tau < 0." The quote is an exact substring and the file is out of order here. No guard detects this shape; found by reading.
mechanisms[6]0.95the tagger's words
mechanismsmechanisms
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mechanismsmechanisms
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mechanisms[8]0.95the tagger's words
limitationsthe relevance of the asymptotics in Lp and in the absence of Rayleigh instabilities remains open
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what this limits: the asymptotic result's reach: THE RELEVANCE OF THIS ASYMPTOTICS IN Lp, OR ITS RELEVANCE IN THE ABSENCE OF RAYLEIGH INSTABILITIES, ARE STILL OPEN ISSUES
limitations[0]the tagger's words
limitationsThe negative result is confined to the viscous Sobolev setting and leaves the known positive (inviscid and monotonic-data) results intact.
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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
limitations[1]the tagger's words
limitationsThe 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.
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what this limits: the stronger part of the theorem: Quotation withheld general base profiles
limitations[2]the tagger's words
limitationsThe 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.
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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
limitations[3]1.0the tagger's words
limitationsThe empirical support for the description is bounded to one side of the separation zone, and the paper says which side.
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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
limitations[4]1.0the tagger's words
limitationsThe 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.
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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
limitations[5]1.0the tagger's words
conceptsPrandtl equation
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concepts[0]the paper's words
conceptsill-posedness
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also in: ill-posedness
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conceptsviscosity
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also in: viscosity
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conceptsboundary layer separation
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conceptscritical point
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conceptsinviscid limit
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conceptsno-slip boundary condition
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conceptsvorticity field
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conceptsboundary layer phenomenon
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conceptsparabolic scaling
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conceptsnormal direction
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conceptsPrandtl equations
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conceptsformal asymptotics
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conceptsPrandtl model
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conceptsfunctional spaces
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conceptstangential variable
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conceptsx derivatives
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conceptsloss of one derivative
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conceptshorizontal diffusion term
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conceptsstandard energy estimates
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conceptsanalytic framework
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conceptsRayleigh instability
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conceptsinviscid version
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about this quote: THE TERM IS NOT IN THE QUOTE - the quote's 'this equation' is the inviscid version of (1.3), named in the sentence just before it ('the inviscid version of (1.3) is analyzed'). That sentence is not quoted because a displaced fragment of the equation breaks it.
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conceptsfinite loss of x-derivatives
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concepts(weakly) well-posed
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conceptsstrong destabilization mechanism
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conceptsbase velocity profile
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conceptsmonotonic data
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conceptsshear velocity profile
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conceptslinearization
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conceptsanalytic regularity
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conceptshigh tangential frequencies
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conceptsunstable quasimodes
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conceptsspectral condition
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conceptsreduced ODE
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conceptsinstability process
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conceptssingular perturbation problem
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about this quote: THE TERM IS NOT IN THE QUOTE - text extraction moved part of the quote's first sentence out of it: the words 'yields a singular perturbation problem' now stand just after the quote.
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conceptsinviscid eigenelements
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conceptsstrong instability
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conceptsheteroclinic orbits
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conceptsholomorphic solution
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conceptscomplex change of variable
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conceptsformal analysis
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conceptsnumerical illustrations
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conceptsEvans function
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conceptsshooting method
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conceptsRunge-Kutta scheme
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conceptsdirect simulations
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conceptsfinite differences
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conceptsCrank-Nicholson scheme
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conceptsinitial random data
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conceptsexcellent agreement
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unhoused_relationsvorticity field → inviscid limit
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Lack of uniform vorticity bounds is the main mathematical difficulty in taking the inviscid limit. Difficulty-for is absent from the governed relation types.
unhoused_relations[0]0.95the tagger's words
unhoused_relationsparabolic scaling → normal direction
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The boundary-layer asymptotics applies a parabolic scaling in the normal direction. Applied-in-direction is absent from the governed relation types.
unhoused_relations[1]0.95the tagger's words
unhoused_relationsloss of one derivative → standard energy estimates
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The unbalanced loss of one tangential derivative prevents standard energy estimates from applying. Prevents is absent from the governed relation types.
unhoused_relations[2]0.95the tagger's words
unhoused_relationsRayleigh instability → formal asymptotics
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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.
unhoused_relations[3]0.95the tagger's words
unhoused_relationsfinite loss of x-derivatives → (weakly) well-posed
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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.
unhoused_relations[4]0.95the tagger's words
unhoused_relationsspectral condition → ill-posedness
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Ill-posedness of the PDE is reduced to a spectral condition for a reduced ODE. Reduces-to is absent from the governed relation types.
unhoused_relations[5]0.95the tagger's words
unhoused_relationsEvans function → spectral condition
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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
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unhoused_relationsshooting method → Newton-Raphson procedure
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Backward shooting supplies the function on which Newton-Raphson locates a zero. Sequential-input-to is absent from the governed relation types.
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unhoused_relationsfinite differences → Crank-Nicholson scheme
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The direct simulation combines finite-difference spatial discretization with Crank-Nicholson time stepping. Combined-with is absent from the governed relation types.
unhoused_relations[8]0.95the tagger's words
sensesill-posedness - LINEAR, and only that: the theorem is about the linearization around solutions with non-degenerate critical points, so the bare claim 'the Prandtl equation is ill-posed' drops the word that bounds the result
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senses[0]1.0the tagger's words
sensesthe 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
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senses[1]1.0the tagger's words
sensesthe 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
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senses[2]1.0the tagger's words
sensesInviscid-limit difficulty - no uniform vorticity bound as viscosity vanishes, corresponding physically to a boundary layer
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senses[3]0.95the tagger's words
sensesPrandtl asymptotics - formally natural but not uniformly valid because boundary-layer separation can occur
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senses[4]0.95the tagger's words
sensesTangential regularity obstacle - one derivative is lost without horizontal diffusion to balance it
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senses[5]0.95the tagger's words
sensesAnalytic setting - sufficient for local boundary-layer justification but filters instability mechanisms
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senses[6]0.95the tagger's words
sensesInviscid Cauchy problem - characteristic solution with finite tangential derivative loss and weak well-posedness
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senses[7]0.95the tagger's words
sensesViscous destabilization - viscosity and non-degenerate critical points jointly underlie the Sobolev failure
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senses[8]0.95the tagger's words
sensesStrong linear ill-posedness - high-frequency perturbations grow on a square-root-frequency timescale
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senses[9]0.95the tagger's words
sensesSpectral reduction - PDE ill-posedness is reduced to a condition on a lower-dimensional ODE
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senses[10]0.95the tagger's words
sensesSpectral-condition problem - existence of a heteroclinic orbit for the reduced ordinary differential equation
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senses[11]0.95the tagger's words
sensesEvans-function computation - shooting with Runge-Kutta integration followed by Newton-Raphson root finding
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senses[12]0.95the tagger's words
sensesDirect numerical test - finite differences on a stretched grid and Crank-Nicholson time stepping from random data
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senses[13]0.95the tagger's words
sensesNumerical confirmation - eigenvalue and eigenmode comparisons agree with theory and show the mechanism dominates linear dynamics
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senses[14]0.95the tagger's words
claim_relationsextends → prior well-posedness results for the Prandtl equation (analytic or monotone data)
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claim_relations[0]the tagger's words
claim_relationsbuilds-on → reference [8] (analysis of the inviscid version of the Prandtl equation)
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claim_relations[1]the tagger's words
claim_relationsbuilds-on → reference [8] (study of the inviscid spectral problem and its evolution equation)
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claim_relations[2]the tagger's words
concept_edgesviscosity —causes→ ill-posedness
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strength of the relation: 1
concept_edges[0]the tagger's words
concept_edgescritical point —causes→ ill-posedness
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strength of the relation: 1
concept_edges[1]the tagger's words
content_tagsThe 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.
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content_tags.findings[0]the tagger's words
content_tagsStrikingly, the strong instability is caused by VISCOSITY — consistent with well-posedness of the inviscid version of the equation.
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content_tags.findings[1]the tagger's words
content_tagsPrandtl equation
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about this quote: QUOTE RECOVERED FROM THE PAPER'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'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.
content_tags.definitions[0]the tagger's words
content_tagsill-posedness
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also in: ill-posedness
content_tags.definitions[1]the tagger's words
content_tagsinviscid limit
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content_tags.definitions[2]the tagger's words

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