Sensitivity Analysis for the Inductance Gradient of EMFY-3 Electromagnetic Launcher

ASELSAN Inc. has been working on electromagnetic launch technologies since 2014. The first prototype, EMFY-1, has a 25 mm \times25 mm square bore and 3-m-length rails. The second prototype, EMFY-2, has a 50 \times50 mm square bore and 3-m-length. This article presents a recently developed protot...

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Veröffentlicht in:IEEE transactions on plasma science 2022-02, Vol.50 (2), p.381-386
Hauptverfasser: Tosun, Nail, Civil, Anil, Oruc, Ahmet Yasin, Yildirim, Baran, Ozceylan, Bekir Mert, Bolat, Bora, Yurdakul, Emre Burak, Tan, Evren, Yurdakonar, Ferhat, Akdemir, Huseyin, Gungen, Ibrahim, Onur, Ibrahim, Karagoz, Mustafa, Cavbozar, Ozgur, Demirkol, Rasih Hakan, Gocmen, Ulas, Keysan, Ozan
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Sprache:eng
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Zusammenfassung:ASELSAN Inc. has been working on electromagnetic launch technologies since 2014. The first prototype, EMFY-1, has a 25 mm \times25 mm square bore and 3-m-length rails. The second prototype, EMFY-2, has a 50 \times50 mm square bore and 3-m-length. This article presents a recently developed prototype, EMFY-3, with a 50 \times75 mm rectangular bore and 6-m length. The input energy of the pulsed-power supply (PPS) is doubled to 8 MJ, and the 2.91 MJ muzzle energy is obtained. Velocity curves are captured with Doppler radar, enabling us to establish propulsive inductance gradient L^{\prime }_{\mathrm {pr}} transients empirically. The results confirm that L^{\prime }_{\mathrm {pr}} is constant throughout the launch, as no significant breaking mechanism occurs with the non-magnetic containment. However, a slight variation (2% at maximum) happens with different rails' current magnitudes from one launch to another. The transition phenomenon is a candidate for the drop in the L^{\prime }_{\mathrm {pr}} , as it occurs more likely at launches with higher linear current densities. Moreover, a sensitivity analysis is conducted to show the importance of L^{\prime }_{\mathrm {pr}} calculations. A deviation of 5% from the actual value can cause an error in muzzle velocity up to 6.2%. This fact indicates that simulation models are very susceptible to L^{\prime }_{\mathrm {pr}} calculations. Although L^{\prime }_{\mathrm {pr}} is calculated as 0.515 \mathrm {\mu H/m} with 3-D finite element method (FEM), the Kerrisk formula calculates as if 0.561~\mathrm {\mu H/m} ; the experimental measurement gives 0.575 \mathrm {\mu H/m}
ISSN:0093-3813
1939-9375
DOI:10.1109/TPS.2022.3140224