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The Art of Practical and Precise Strain Based ... - Webprofile.info

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<strong>Strain</strong>-<strong>Based</strong> Measurement Introduction:H( w)=1--------------------------------------------------------------æ w1 -----èÐ èæ w 0øö2 ö 2 2z w ø+ -----èæ w 0øö2(EQ 1-28)<strong>and</strong>jw ( )=2zatan------------------------æ w w----- Ð ----- 0 öè w øw 0(EQ 1-29)Where:j(w) = <strong>The</strong> phase relationship between the output <strong>and</strong> the input forcingfunction.w 0=K----MRadians/SecondWhere: w 0 = 2p f 0(EQ 1-30)RMz = ----------------2 MK(EQ 1-31)<strong>The</strong> implications <strong>of</strong> equations (1-28) <strong>and</strong> (1-29) are shown graphicallyin Figure 1-28 <strong>and</strong> are stated as follows:1. As w approaches zero radians/second: <strong>The</strong> second-order system is stiffness-dominated orÒspring-controlledÓ where the transfer function H(w) approaches unity in value.2. As w approaches infinity radians/second: <strong>The</strong> second-order system is mass-dominatedwhere the reaction <strong>of</strong> the mass to the input approaches zero, or the value <strong>of</strong> the transferfunction value itself approaches zero.3. As w approaches infinity: <strong>The</strong> phase angle between the input <strong>and</strong> the output approaches180 degrees.4. When the phase angle between the input <strong>and</strong> the output equals 90 degrees, w = w 0 which istermed the natural frequency <strong>of</strong> the system.5. If this system possessed zero damping (an impossibility), the value <strong>of</strong> the transfer functionwill approach infinity at the natural frequency <strong>of</strong> the system.CHAPTER 1-54 <strong>The</strong> <strong>Art</strong> <strong>of</strong> <strong>Practical</strong> <strong>and</strong> <strong>Precise</strong> <strong>Strain</strong> <strong>Based</strong> Measurement 2nd Edition © 1999

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