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 |
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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} |
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ISSN: | 0093-3813 1939-9375 |
DOI: | 10.1109/TPS.2022.3140224 |