Paperback. Condition: Very Good. No Jacket. May have limited writing in cover pages. Pages are unmarked. ~ ThriftBooks: Read More, Spend Less 0.65.
Seller: Zubal-Books, Since 1961, Cleveland, OH, U.S.A.
Condition: Fine. First edition, first printing, 257 pp., Paperback, a TINY bit of discoloration to fore edge else fine. - If you are reading this, this item is actually (physically) in our stock and ready for shipment once ordered. We are not bookjackers. Buyer is responsible for any additional duties, taxes, or fees required by recipient's country.
Condition: New. SUPER FAST SHIPPING.
Seller: BargainBookStores, Grand Rapids, MI, U.S.A.
Paperback or Softback. Condition: New. Methods for Solving Incorrectly Posed Problems 0.87. Book.
Condition: New.
Paper Bound. Condition: Near Fine. First Edition. Clean, unmarked copy.
£ 20.04
Convert currencyQuantity: 1 available
Add to basketSoftcover. Ex-library with stamp and library-signature. GOOD condition, some traces of use. C-02794 3540960597 Sprache: Englisch Gewicht in Gramm: 1050.
Seller: Ria Christie Collections, Uxbridge, United Kingdom
£ 50.82
Convert currencyQuantity: Over 20 available
Add to basketCondition: New. In.
£ 51.08
Convert currencyQuantity: 1 available
Add to basketTaschenbuch. Condition: Neu. Druck auf Anfrage Neuware - Printed after ordering - Some problems of mathematical physics and analysis can be formulated as the problem of solving the equation f EUR 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 EUR 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.
£ 65.93
Convert currencyQuantity: 2 available
Add to basketPaperback. Condition: Brand New. 280 pages. 9.10x5.90x0.50 inches. In Stock.
£ 42.31
Convert currencyQuantity: Over 20 available
Add to basketCondition: New.
£ 81.60
Convert currencyQuantity: 10 available
Add to basketPF. Condition: New.
Published by Springer-Verlag New York Inc., 1984
ISBN 10: 0387960597 ISBN 13: 9780387960593
Language: English
Seller: THE SAINT BOOKSTORE, Southport, United Kingdom
£ 56.09
Convert currencyQuantity: Over 20 available
Add to basketPaperback / softback. Condition: New. This item is printed on demand. New copy - Usually dispatched within 5-9 working days 427.
Published by Springer New York Nov 1984, 1984
ISBN 10: 0387960597 ISBN 13: 9780387960593
Language: English
Seller: BuchWeltWeit Ludwig Meier e.K., Bergisch Gladbach, Germany
£ 84.24
Convert currencyQuantity: 2 available
Add to basketTaschenbuch. Condition: Neu. This item is printed on demand - it takes 3-4 days longer - Neuware -Some problems of mathematical physics and analysis can be formulated as the problem of solving the equation f EUR 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 EUR 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. 280 pp. Englisch.