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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Journal of mathematical biology 38 (1999), S. 262-284 
    ISSN: 1432-1416
    Keywords: Key words: Tumors ; Parabolic equations ; Free boundary problems
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology , Mathematics
    Notes: Abstract.  In this paper we study a recently proposed model for the growth of a nonnecrotic, vascularized tumor. The model is in the form of a free-boundary problem whereby the tumor grows (or shrinks) due to cell proliferation or death according to the level of a diffusing nutrient concentration. The tumor is assumed to be spherically symmetric, and its boundary is an unknown function r=s(t). We concentrate on the case where at the boundary of the tumor the birth rate of cells exceeds their death rate, a necessary condition for the existence of a unique stationary solution with radius r=R 0 (which depends on the various parameters of the problem). Denoting by c the quotient of the diffusion time scale to the tumor doubling time scale, so that c is small, we rigorously prove that (i) lim inf t→∞ s(t)〉0, i.e. once engendered, tumors persist in time. Indeed, we further show that (ii) If c is sufficiently small then s(t)→R 0 exponentially fast as t→∞, i.e. the steady state solution is globally asymptotically stable. Further, (iii) If c is not “sufficiently small” but is smaller than some constant γ determined explicitly by the parameters of the problem, then lim sup t→∞ s(t)〈∞; if however c is “somewhat” larger than γ then generally s(t) does not remain bounded and, in fact, s(t)→∞ exponentially fast as t→∞.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Applied mathematics & optimization 15 (1987), S. 65-85 
    ISSN: 1432-0606
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract The dam problem with general geometry is considered. Fluid is drawn from the bottomS 1 at a ratek where 0 ≤k ≤ N, ∫ S 1 k ≤ M; the objective is to minimize the “total pressure” of the fluid in the dam. A bang-bang principle is established for any optimal controlk 0, that is,k 0 = 0 on a setA andk 0 =N on the complement setS 1 ∖A. In the case of a rectangular dam the structure ofA is determined and the uniqueness of the minimizerk 0 is established.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Applied mathematics & optimization 13 (1985), S. 59-78 
    ISSN: 1432-0606
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract Consider the variational inequality for the rectangular dam problem and assume that fluid can be withdrawn from the bottom at a rate proportional tok(x). Denote byp(x, y) the pressure of the fluid in the dam corresponding to a particular choice ofk. Consideringk(x) as a control variable varying in a class {0⩽k(x)⩽N, ∫k(x)dx⩽M}, we introduce the functionalJ(k)=∫∫g(y)p(x, y) whereg(y) is a given positive and monotone nondecreasing function. We characterize the controlsk 0 which minimizeJ(k).
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Archive for rational mechanics and analysis 107 (1989), S. 85-97 
    ISSN: 1432-0673
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Archive for rational mechanics and analysis 11 (1962), S. 62-96 
    ISSN: 1432-0673
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Archive for rational mechanics and analysis 132 (1995), S. 49-72 
    ISSN: 1432-0673
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract Suppose the 3-dimensional space is filled with three materials having dielectric constants ɛ 1 above S 1={x 2=f 1(x 1), x 3 arbitrary}, ɛ 2 below S 2 = {x 2 =f 2(x 1), x 3 arbitrary} and ɛ o in {f 2(x 1) 〈x 2 〈f1(x 1), x 3 arbitrary} where f 1 f 2 are periodic functions. Suppose for a plane wave incident on S 1 from above we can measure the reflected and transmitted waves of the corresponding time-harmonic solution of the Maxwell equations, say at x 2=±b,b large. To what extent can we infer from these measurements the location of the pair (S 1, S 2 ? In this paper, we establish a local stability: If ( $$\tilde S_1 ,\tilde S_2$$ ) is another pair of periodic curves “close” to (S 1, S2), then, for any δ〉0, if the measurements for the two pairs are δ-close, then $$\tilde S_1$$ and $$\tilde S_2$$ are 0(δ)-close to S 1 and S 2, respectively.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Archive for rational mechanics and analysis 10 (1962), S. 180-188 
    ISSN: 1432-0673
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Archive for rational mechanics and analysis 101 (1988), S. 57-83 
    ISSN: 1432-0673
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract We construct an optical lens in the (x, y)-plane which focuses two pairs of points, i.e., all the rays from a given point X i are focused by the lens at a given point y i , for i = 1, 2. The points X 1, X 2, Y 1, Y 2 lie on the x-axis and the lens has the form $$\left\{ {\gamma _{\text{1}} {\text{ }} + {\text{ }}f_{\text{1}} {\text{(}}y{\text{) }}\underline \leqslant {\text{ }}x{\text{ }}\underline \leqslant {\text{ }}\gamma _{\text{2}} {\text{ }} + {\text{ }}f_{\text{2}} {\text{(}}y{\text{)}},{\text{ }}\left| y \right|{\text{ }}\underline \leqslant {\text{ }}y_{\text{0}} } \right\}$$ where γ 1, γ 2 are given, and f i (0) = 0, f i (−y) = f i (y). We then let X 2 → X 1, Y 2 → Y 1 and investigate the limiting lens. We show that this limit is generally not a symmetric lens, i.e., f 1 + f 2 ≇ 0.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Archive for rational mechanics and analysis 123 (1993), S. 259-303 
    ISSN: 1432-0673
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract The formation of a visual image in electrophotography can be modeled as a time-dependent free boundary problem. The electric potential &-u satisfies Δu=1 in the toner region and Δu=0 outside this region, whereas on the interface (which is a moving boundary)-∂u/∂N=velocity of the interface, N being the outward normal to the toner region. It is proved that this problem has a smooth solution for a small time interval; furthermore, for a certain version of the free boundary condition, the solution is unique.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Archive for rational mechanics and analysis 101 (1988), S. 143-160 
    ISSN: 1432-0673
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Type of Medium: Electronic Resource
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