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Methods for Solving Incorrectly Posed Problems [Paperback]

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  • Category: Books (Mathematics)
  • Author:  Morozov, V.A.
  • Author:  Morozov, V.A.
  • ISBN-10:  0387960597
  • ISBN-10:  0387960597
  • ISBN-13:  9780387960593
  • ISBN-13:  9780387960593
  • Publisher:  Springer
  • Publisher:  Springer
  • Binding:  Paperback
  • Binding:  Paperback
  • Pub Date:  01-Feb-1984
  • Pub Date:  01-Feb-1984
  • SKU:  0387960597-11-SPRI
  • SKU:  0387960597-11-SPRI
  • Item ID: 100831745
  • List Price: $54.99
  • Seller: ShopSpell
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  • Delivery by: Jul 03 to Jul 05
  • Notes: Brand New Book. Order Now.
Some problems of mathematical physics and analysis can be formulated as the problem of solving the equation f ? F, (1) Au = f, where A: DA C U + F is an operator with a non-empty domain of definition D , in a metric space U, with range in a metric space F. The metrics A on U and F will be denoted by P and P ' respectively. Relative u F to the twin spaces U and F, J. Hadamard P-06] gave the following defini? tion of correctness: the problem (1) is said to be well-posed (correct, properly posed) if the following conditions are satisfied: (1) The range of the value Q of the operator A coincides with A F ( sol vabi li ty condition); (2) The equality AU = AU for any u ,u ? DA implies the I 2 l 2 equality u = u ( uniqueness condition); l 2 (3) The inverse operator A-I is continuous on F ( stability condition). Any reasonable mathematical formulation of a physical problem requires that conditions (1)-(3) be satisfied. That is why Hadamard postulated that any ill-posed (improperly posed) problem, that is to say, one which does not satisfy conditions (1)-(3), is non-physical. Hadamard also gave the now classical example of an ill-posed problem, namely, the Cauchy problem for the Laplace equation.Some problems of mathematical physics and analysis can be formulated as the problem of solving the equation f ? F, (1) Au = f, where A: DA C U + F is an operator with a non-empty domain of definition D , in a metric space U, with range in a metric space F. The metrics A on U and F will be denoted by P and P ' respectively. Relative u F to the twin spaces U and F, J. Hadamard P-06] gave the following defini? tion of correctness: the problem (1) is said to be well-posed (correct, properly posed) if the following conditions are satisfied: (1) The range of the value Q of the operator A coincides with A F ( sol vabi li ty condition); (2) The equality AU = AU for any u ,u ? DA implies the I 2 l 2 equality u = u ( uniqueness condition); l 2 (3) The inverse operator A-I is continuous l3‹
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