A cnoidal wave solution of the KP equation. Every cnoidal wave solution is one-dimensional, and it is time-independent in a uniformly translating coordinate system.
A two-phase KP solution. This solution is stationary, as are all two-phase solutions that are genuinely two-dimensional. (a) Perspective view of the solution. (b) Overhead view, with contour lines shown.
| z11 | 2 |
| z12 | 0.8 |
| z22 | 2.82 |
| (alpha) | (2) |
| (beta) | (2.5) |
| (lambda) | (0.4) |
| k1 | 0.6 |
| k2 | 0.8 |
| l1 | 0.2 |
| l2 | -0.8059 |
| omega1 | -1.9065 |
| omega2 | -4.0238 |
A symmetric two-phase solution. Every symmetric two-phase solution is periodic in x and in y, and it translates purely in the x-direction.
| alpha | 2 |
| beta | 1.68 |
| lambda | 0.4 |
| (z11) | (2) |
| (z22) | (2) |
| (z12) | (0.8) |
| k1 | 0.8 |
| k2 | 0.8 |
| l1 | 0.6155175 |
| l2 | -0.6155175 |
| omega1 | -5.924798 |
| omega2 | -5.924798 |
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| Figure 4a | Figure 4b | Figure 4c | Figure 4d | Figure 4e |
A three-phase KP solution. This solution is periodic in a moving frame, with a period T = 3.1908. It is shown at four times: (a) t = 0.0, (b) t = 0.5, (c) t = 1.5, (d) t = 3.1908, (e) t = 3.1908, but translated according to (1.14).
| alpha | 2 |
| beta | 4 |
| gamma | 4 |
| lambda | 0.5 |
| mu | 0.5 |
| nu | 0.1 |
| k1 | 0.5 |
| k2 | 1 |
| k3 | 1.2060 |
| l1 | -0.2 |
| l2 | -1.3974 |
| l3 | 0.6148 |
| omega1 | -1.1427 |
| omega2 | -6.2228 |
| omega3 | -0.3940 |
| square root | + |
A three-phase KP solution that is nearly stationary. The period matrix of this solution is completely symmetric: z11 = z22 = z33 = 3, zij = 6/5 for i != j. Consequently, there is another, identical solution with the same period matrix and with the phases renumbered: k1 = 0.574979, k2 = k3 = 1.0, l1 = 0, l2 = -l3 = 0.6412115.
| alpha | 3 |
| beta | 63/25 = 2.52 |
| gamma | 81/35 = 2.3143 |
| lambda | 0.4 |
| mu | 0.4 |
| nu | 2/7 = 0.2857 |
| k1 | 1 |
| k2 | 1 |
| k3 | 0.574979 |
| l1 | 0.6412115 |
| l2 | -0.6412115 |
| l3 | 0 |
| omega1 | -3.260237 |
| omega2 | -3.260237 |
| omega3 | -1.882164 |
| square root | + |
Another three-phase KP solution that is nearly stationary.
| alpha | 3/2 = 1.5 |
| beta | 63/25 = 2.52 |
| gamma | 81/35 = 2.3143 |
| lambda | 0.4 |
| mu | 0.4 |
| nu | 2/7 = 0.2857 |
| k1 | 0.3248453 |
| k2 | 1 |
| k3 | 1 |
| l1 | 0 |
| l2 | 0.818674 |
| l3 | -0.818674 |
| omega1 | -1.631909 |
| omega2 | -5.004516 |
| omega3 | -5.004516 |
| square root | - |