| 21. | The dispersion relation for these waves is:
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| 22. | Their dispersion relation reads, for waves on the interface between two fluids of infinite depth:
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| 23. | In order to obtain the dispersion relation it is possible to proceed in two different ways.
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| 24. | The dispersion relation for extraordinary waves is
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| 25. | The group velocity therefore depends upon the dispersion relation connecting ? and " k ".
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| 26. | Each of these components travels with its own phase velocity, in accordance with the dispersion relation.
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| 27. | The underlying reason for the difference in dispersion relation is that ferromagnets violate time-reversal symmetry.
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| 28. | The parameter describes the frequency dependence of the sound velocity of the membrane ( dispersion relation ).
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| 29. | The frequency ? as a function of "'k "'is the dispersion relation.
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| 30. | The polarization dependent phase shift is also the reason why TE and TM guided modes have different dispersion relations.
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