At a fixed point on a beam

PHYSICS · Multi-part · Fermi University Physics · Optics & Photonics · Wave propagation and light in media · Wave propagation and light in media

Optics and Photonics, Ch Harmonic waves, phasors and group velocity

Problem

At a fixed point on a beam, two harmonic waves of the same frequency are represented by two phasors (arrows) drawn from a common origin. The first arrow has length E1=5.0 V m−1E_1 = 5.0\ \mathrm{V\,m^{-1}} and lies along the reference direction (angle 00). The second has length E2=12.0 V m−1E_2 = 12.0\ \mathrm{V\,m^{-1}} and is turned by δ=90∘\delta = 90^\circ from the first, in the sense of increasing phase constant. Both arrows turn together at the angular frequency ω\omega, so the angle between them is fixed. Translate the diagram into an equation: write the resultant as E=E0cos⁡(kx−ωt+ϕ)E = E_0\cos(kx - \omega t + \phi) and find ((a)) the resultant amplitude E0E_0; ((b)) the phase constant ϕ\phi of the resultant, in degrees, measured from the first arrow.

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