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Chapter 3 System Design Considerations Introduction POSSIBLE COMPONENT MOTIONS Retroreflector Interferometer Receiver Z YA W X LL O R P Y IT C H Laser Head Figure 3-1. Possible component motions 1. Motion of the receiver or laser head along the beam path (X) has no effect on the measurement since both f1 and f2 would exhibit Doppler shift. 2. Small motions of the laser head, receiver, interferometer, or retroreflector in a direction perpendicular to the beam path (Y or Z) have no effect on the measurement. The only restriction is that sufficient light returns to the receiver. 3. Angular motion (pitch or yaw) of the laser head about the Z or Y axis has the effects described below: a. It introduces a measurement error (cosine error). b. It may displace the laser beam so that insufficient light returns to operate the receiver. 4. Although the laser head or the receiver may be rotated in 90° increments about the beam axis (roll), other roll deviations from the four optimum positions degrade the measurement signal. If either the laser head or receiver is rotated 45° about the beam axis, all position information will be lost because the receiver will not be able to distinguish between the two frequencies. 5. Angular motion of the receiver about the Y or Z axis has no effect on the measurement, within alignment limits specified for the receiver. (Receiver specifications are given in Chapter 8, “Receivers,” of this manual.) 6. Angular motions of the interferometer and retroreflector depend on the particular components for limitations. User’s Manual 3-3