1998
DOI: 10.1007/bf02321650
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Dynamic response of strain gages up to 300 kHz

Abstract: ABSTRACT--Dynamic response of foil strain gages is investigated in the ranges of up to approximately 300 kHz in frequency, 2000 t~e in strain and 750 s -t in strain rate. Impulsive input is applied to the gages using elastic wave pulses in a circular bar. The input is determined by measuring the velocity of the bar end with a laser interferometer. It was confirmed that deviations from the static gage factors do not exceed -5 percent within the frequency range up to 45 kHz, 110 kHz and more than 290 kHz for 20-… Show more

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Cited by 20 publications
(10 citation statements)
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“…These gauges were recommended by the manufacturer for dynamic applications and were also consistent with Ueda and Umbera's [19] findings.…”
Section: General Outputsmentioning
confidence: 93%
“…These gauges were recommended by the manufacturer for dynamic applications and were also consistent with Ueda and Umbera's [19] findings.…”
Section: General Outputsmentioning
confidence: 93%
“…As can be observed, the reconstructed and actual curves compare very favourably. In the authors' opinion, the differences are to be attributed to the measurement method rather than to the reconstruction procedure.Finally the procedure was repeated using the data drawn from Ueda and Umeda [13]. 2 In this case there is excellent agreement between the actual and reconstructed curves (Figure 4).…”
mentioning
confidence: 85%
“…Finally the procedure was repeated using the data drawn from Ueda and Umeda [13]. 2 In this case there is excellent agreement between the actual and reconstructed curves (Figure 4).…”
Section: Validationmentioning
confidence: 98%
“…In the early 80s of last century, Robert D [1] in ENDEVCO corporation, Togami [2] and Ueda [3][4][5] had introduced the operation system for accelerometer calibration in the range of 10,000 g to greater than 100,000 g. This system works based on a Hopkinson bar, and calibration of an accelerometer is based on a strain gauge measurement of the wave. Li et al [6] also presents the modified Hopkinson bar system, this system can calibrate the accelerometer in a range from 5,000 g to 200,000 g. In this system, a half-sine acceleration pulse is obtained by impacting a parabolic pointed projectile.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, a more easy measuring method has been proposed, that is, we base on such a fact, the acceleration pulse is always located in first half of a loading strain pulse in the Hopkinson shock test [1][2][3][4][5][6], and combining with the relation between projectile shape and strain wave, two coaxial projectiles (outer circular tube and inner cylinder) are always fired by a single gun barrel during whole operation. This replace the coaxial double gun barrel, and the synchronization impact on the end surface of the bar is effectively ensured, so it is much more convenient for dynamic linearity measurement.…”
Section: Introductionmentioning
confidence: 99%