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A Preliminary Study of the Burgers Equation with Symbolic ...

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SYMBOLIC COMPUTATION OF THE BURGERS EQUATION 231<br />

The integer exponent <strong>of</strong> <strong>the</strong> amplitude factor, (10), embodies complex combinations <strong>of</strong><br />

harmonic interactions. Signifying <strong>the</strong> exponent as E = n1 + n2 + 2( j1 + j2 − 2) , several<br />

scenarios can be explored. If only <strong>the</strong> leading terms <strong>of</strong> an interacting harmonic pair are<br />

considered, <strong>the</strong>n j1 = j2 = 1, and <strong>the</strong> exponent reduces to E = n1 + n2. Various wavenumber<br />

pairs, (n1, n2), potentially comprise E. Obviously, <strong>the</strong> higher <strong>the</strong> value <strong>of</strong> E is, <strong>the</strong> greater<br />

<strong>the</strong> complexity. Except when n1 = n2, each ordered pair, (n1, n2), has a counterpart pair,<br />

(n2, n1), <strong>with</strong> <strong>the</strong> two elements in reversed order. This is evident in Table II, which shows<br />

that <strong>the</strong> companion pairs exist in separate terms that may or may not have common signs<br />

or multipliers. One pair <strong>of</strong> <strong>the</strong> set potentially yields an opposite sign in backscatter, which<br />

does not in general lead to canceling effects, as seen in <strong>the</strong> table. If n1 = n2, no backscatter<br />

is produced, as previously explained.<br />

If o<strong>the</strong>r than leading terms are considered in <strong>the</strong> preceding analysis (i.e., j1 = 1 and j2 = 1),<br />

<strong>the</strong>n <strong>the</strong> scenarios involving <strong>the</strong> exponent <strong>of</strong> <strong>the</strong> amplitude factor become more complex,<br />

but follow a similar line <strong>of</strong> reasoning. For example, assume j1 = 1 and j2 = 1 in (10).<br />

Since n1 + n2 = E − 2( j1 + j2 − 2), setting E = 14 and j1 + j2 = 5 yields n1 + n2 = 8.<br />

The companion harmonic pairs (i) (2, 6) and (6, 2), (ii) (3, 5) and (5, 3), and (iii) (4, 4)<br />

satisfy <strong>the</strong> criterion n1 + n2 = 8. But for each <strong>of</strong> <strong>the</strong>se, <strong>the</strong> following combinations <strong>of</strong> term<br />

pairs, [ j1, j2], satisfy j1 + j2 = 5: [1, 4], [4, 1], [2, 3], and [3, 2] in which element order in<br />

each pair is important. Because <strong>the</strong>re are a total <strong>of</strong> 5 harmonic pairs, and 4 term pairs for each<br />

harmonic pair, a total <strong>of</strong> 20 interactions satisfy <strong>the</strong> criterion E = 14. All <strong>of</strong> <strong>the</strong> harmonic<br />

pairs produce outscatter to <strong>the</strong> 7th harmonic, because n1 + n2 = 8, but <strong>the</strong> harmonic pairs<br />

(2, 6) and (6, 2) produce backscatter to <strong>the</strong> 3rd harmonic. The pairs (3, 5) and (5, 3) produce<br />

backscatter to <strong>the</strong> 1st harmonic, and (4, 4) produces no backscatter. It is evident <strong>the</strong>re is<br />

a large and complex combination <strong>of</strong> harmonic interactions at play in <strong>the</strong> solution to <strong>the</strong><br />

<strong>Burgers</strong> equation.<br />

Table III displays combinations <strong>of</strong> nonlinear harmonic interactions, (n1, n2), that potentially<br />

produce outscatter and backscatter in <strong>the</strong> fundamental and <strong>the</strong> 10 harmonics produced<br />

in <strong>the</strong> symbolic solution. However, <strong>the</strong> companion harmonic pairs denoted by (n2, n1) are<br />

omitted for presentational convenience, but self-interactions denoted by n1 = n2 are included.<br />

Note that outscatter combinations are fewer in number compared to backscatter<br />

combinations, and that <strong>the</strong> fundamental only experiences backscatter. However, solution<br />

TABLE III<br />

Combinations <strong>of</strong> Harmonic Pairs Producing Outscatter and Backscatter for Fundamental<br />

and Various Harmonics<br />

Affected Outscatter Backscatter<br />

harmonic combinations combinations<br />

Fundamental None (1,2) (2,3) (3,4) (4,5) (5,6) (6,7) (7,8) (8,9) (9,10) ...<br />

1st harmonic (1,1) (1,3) (2,4) (3,5) (4,6) (5,7) (6,8) (7,9) (8,10) (9,11) ...<br />

2nd harmonic (1,2) (1,4) (2,5) (3,6) (4,7) (5,8) (6,9) (7,10) (8,11) (9,12) ...<br />

3rd harmonic (1,3) (2,2) (1,5) (2,6) (3,7) (4,8) (5,9) (6,10) (7,11) (8,12) ...<br />

4th harmonic (1,4) (2,3) (1,6) (2,7) (3,8) (4,9) (5,10) (6,11) (7,12) (8,13) ...<br />

5th harmonic (1,5) (2,4) (3,3) (1,7) (2,8) (3,9) (4,10) (5,11) (6,12) (7,13) ...<br />

6th harmonic (1,6) (2,5) (3,4) (1,8) (2,9) (3,10) (4,11) (5,12) (6,13) (7,14) ...<br />

7th harmonic (1,7) (2,6) (3,5) (4,4) (1,9) (2,10) (3,11) (4,12) (5,13) (6,14) ...<br />

8th harmonic (1,8) (2,7) (3,6) (4,5) (1,10) (2,11) (3,12) (4,13) (5,14) (6,15) ...<br />

9th harmonic (1,9) (2,8) (3,7) (4,6) (5,5) (1,11) (2,12) (3,13) (4,14) (5,15) ...<br />

10th harmonic (1,10) (2,9) (3,8) (4,7) (5,6) (1,12) (2,13) (3,14) (4,15) (5,16) ...

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