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Sun. Sep 8, 2024

Mon. Sep 9, 2024

Tue. Sep 10, 2024

Wed. Sep 11, 2024

Thu. Apr 3, 2025

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両面で温度分布を受けるD<sub>∞</sub>圧電無限帯板の非定常熱電気弾性場の理論解析

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

機能材料と構造の力学 (2)

金沢テスト学会

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[S031-11]両面で温度分布を受けるD_∞圧電無限帯板の非定常熱電気弾性場の理論解析

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[S031-11]両面で温度分布を受けるD∞圧電無限帯板の非定常熱電気弾性場の理論解析

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[S031-11]両面で温度分布を受けるD_∞圧電無限帯板の非定常熱電気弾性場の理論解析