High Resolution Schemes for Hyperbolic Conservation
High Resolution Schemes for Hyperbolic Conservation
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In our eReader you can find the full English version of the book. Read High Resolution Schemes for Hyperbolic Conservation Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book High Resolution Schemes for Hyperbolic Conservation
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5). We srj^ll discuss consistency with the entix^py condition iii Section 5 .
- 20 - (2) Condition (3. 6) is only a necessary condition for second order accuracy. It becanes a sufficient condition if the coefficient in the 0(A ) term in (3. 6) is different iable, except possibly at a firjLte nunnber of points N(t, At), such that NAt -> as At -> for all t. It is clear from (3. 13) and (3. 9) that the troublescine points where the scheme (3. 8) + (3. 11) may degenerate locally to 2 OCa ) truncati...on error are those vjhere s.^, ,„ (3. 11c) is discontinuous, i. E.
2 ^ere Q(v) -v =0 oru^=0. The fact that the scheme is TV14I controls the possible increase of the number of local extremum points in the conputed solution. The schen^. Es that v;e consider in section 5 all have the monotonicity piroperty (see section 2); i. E. The number of local extremum points in the conputed solution is nonincreasing in time, and thus bounded by that of the initial data.
(3) The modified equation of the scheme (3.
What to read after High Resolution Schemes for Hyperbolic Conservation?
You can find similar books in the "Read Also" column, or choose other free books by A Harten to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
5). We srj^ll discuss consistency with the entix^py condition iii Section 5 .
- 20 - (2) Condition (3. 6) is only a necessary condition for second order accuracy. It becanes a sufficient condition if the coefficient in the 0(A ) term in (3. 6) is different iable, except possibly at a firjLte nunnber of points N(t, At), such that NAt -> as At -> for all t. It is clear from (3. 13) and (3. 9) that the troublescine points where the scheme (3. 8) + (3. 11) may degenerate locally to 2 OCa ) truncati...on error are those vjhere s.^, ,„ (3. 11c) is discontinuous, i. E.
2 ^ere Q(v) -v =0 oru^=0. The fact that the scheme is TV14I controls the possible increase of the number of local extremum points in the conputed solution. The schen^. Es that v;e consider in section 5 all have the monotonicity piroperty (see section 2); i. E. The number of local extremum points in the conputed solution is nonincreasing in time, and thus bounded by that of the initial data.
(3) The modified equation of the scheme (3.
What to read after High Resolution Schemes for Hyperbolic Conservation?
You can find similar books in the "Read Also" column, or choose other free books by A Harten to read onlineMoreLess
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