Transverse Wave Polarization States - Ask a Question

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Each transverse wave has two possible polarization states, which are represented by vectors in a plane perpendicular to the direction of wave propagation. These polarization states can be visualized as two orthogonal directions within that plane, such as the y and z axes when the wave propagates along the x-axis. The discussion highlights that transverse waves can be decomposed into two components, unlike compressional waves, which only require one component for description. This distinction is important in fields like seismology, where understanding wave behavior is crucial for analyzing material disturbances. Overall, the two polarization states of transverse waves are fundamental to their behavior and representation in three-dimensional space.
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Hi all, i want to ask a simple question which is not so for me. Actually while studying transverse waves, a line is written:-"EACH TRANSVERSE WAVE HAS TWO POSSIBLE POLARISATION STATES". Can anybody tell me please which are those two possible polarisation states refer here (either up and down or something else).Please help
Thanks
 
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The definition of transversal wave is that the deviation vector (or another vector quantity in a general case) is perpendicular to the line of wave propagation. Since our space is 3 dimensional, the set of all vectors perpendicular to a certain direction is 2 dimensional (a plane). Any vector in that plane can be expressed as a linear combination of 2 vectors, that are perpendicular to each other and the line of propagation: these are the 2 possible polarizations. For example: if the wave propagates in x direction, then the vector quantity lies in yz plane (if it is a transversal wave) so it can have a direction y or z (or a linear combination of them).
 
The definition above is spot on. In seismology it was recognized by expansion of Newton's second law that by conservation of momentum, a disturbance in the strain of an elastic material will propagate a field of disturbance involoving two scalar potentials. One of these scalar potentials is involved with the divergence of the strain field and is manifest as a compressional wave, the other scalar potential relates to the curl of the strain field which is manifest as a transverse wave. Thus the transverse wave is an order higher than the compressional wave and can be decomposed into two components as opposed to the one which is sufficient to describe the directionality of compressionally induced particle momentum.
 
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