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When the magnetron hits (partial X), it reflects according to the standard "incidence angle equals reflection angle" law and thus the "particle" propagates along (partial X) with speed O(1) rather than (O(mu ^{-1})).
The agent did not avoid wall contact but reflected off the wall in such a manner that the reflection angle was equal to the incident angle.
In (g)–(i), the reflection angle of RER does not change sign since electron is reflected to the same side of the normal.
The increased reflection angle in the right leads to a farther propagation of the reflected wave into the crossing street.
For specular reflections, the reflection angle equals the angle of incidence.
This can easily be seen by considering the law of reflection (angle of incidence is equal to angle of reflection).
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Incident angles varying from −20° to 20°, the reflection angles are demonstrated in the oblique incidence.
The high energy response is achieved by use of relatively small reflection angles and by coating the mirrors with iridium.
In the first, reflection angles of 0; 1.38 and 2.76° were imposed.
(a)–(c) Group velocity vx; (d)–(f) group velocity vy; and (g)–(i) incident and reflection angles of an incident K valley electron at a given ky.
(c) The effect of dispersion for TE polarization in terms of the variation of reflection angles relative to those at λ=590 nm.
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