Download Integrated Optomechanical Analysis by Keith B. Doyle, Victor L. Genberg, Gregory J. Michels PDF
By Keith B. Doyle, Victor L. Genberg, Gregory J. Michels
This educational offers optomechanical modeling concepts to successfully layout and research high-performance optical platforms. It discusses thermal and structural modeling equipment that use finite-element research to foretell the integrity and function of optical parts and optical help buildings. contains accompanying CD-ROM with examples.
Contents
- creation to Mechanical research utilizing Finite Elements
- Optical Fundamentals
- Optomechanical Displacement research Methods
- built-in Optomechanical Analyses
- Modeling the consequences of Temperature
- Adaptive Optics research Methods
- Optimization of Optomechanical Systems
- instance Telescope Analysis
- built-in Optomechanical research of a Lens Assembly
- Index
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Extra resources for Integrated Optomechanical Analysis
Example text
Org/terms 30 CHAPTER 1 If the area (A) under the response curve is determined from integration, the RMS of the response quantity is found from: rms = 1σ value = A. 7% of the time For more detailed discussion of vibration analysis, see Refs. [11] and [12]. 4 Damping In the harmonic response equations above, viscous damping is represented by the term “C”. The presence of damping causes the response throughout a structure to reach peak values at different times, which may be referred to as a delay (in time units) or as a phase angle (in degrees).
19 (a) Transfer Function of Image Motion (TF or FRF), (b) PSDP of base shake input, and (c) PSDR of image motion response. org/terms 30 CHAPTER 1 If the area (A) under the response curve is determined from integration, the RMS of the response quantity is found from: rms = 1σ value = A. 7% of the time For more detailed discussion of vibration analysis, see Refs. [11] and [12]. 4 Damping In the harmonic response equations above, viscous damping is represented by the term “C”. The presence of damping causes the response throughout a structure to reach peak values at different times, which may be referred to as a delay (in time units) or as a phase angle (in degrees).
This is achieved by multiplying the transfer function by the harmonic input, which yields the spectral content of the output. An inverse Fourier transform is performed to convert back into the temporal or spatial domain. For example, the image of a bar target of infinite extent, shown in Fig. 21, is computed using the frequency domain. The object is described using harmonic spatial frequencies computed using a Fourier series. . 7) Several of the individual frequency components are plotted and graphically summed to illustrate how spatial frequencies may be used to represent the object in Fig.