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๊ฒ€์ฆ๋œ ํŒŒํŠธ๋„ˆ ์ œํœด์‚ฌ ์ž๋ฃŒ

The Finite Element Formulation and Its Classification of Dynamic Thermeoelastic Problems of Solids

๋ฐฉ๋Œ€ํ•œ 850๋งŒ๊ฑด์˜ ์ž๋ฃŒ ์ค‘ ์ฃผ์ œ๋ณ„๋กœ ๋งŒ๋“ค์ˆ˜ ์žˆ๋Š” ์ตœ์ ์˜ ์‚ฐ์ถœ๋ฌผ์„ ํ•ดํ”ผ ์บ ํผ์Šค์—์„œ ์ฒดํ—˜ ํ•˜์„ธ์š” ์ „๋ฌธ๊ฐ€์˜ ์ง€์‹๊ณผ ์ธ์‚ฌ์ดํŠธ๋ฅผ ํ™œ์šฉํ•˜์—ฌ ์‰ฝ๊ณ  ํญ๋„“๊ฒŒ ์ดํ•ดํ•˜๊ณ  ์ ์šฉํ• ์ˆ˜ ์žˆ๋Š” ๊ธฐํšŒ๋ฅผ ๋†“์น˜์ง€ ๋งˆ์„ธ์š”
14 ํŽ˜์ด์งฟ’
์–ด๋„๋น„ PDF
์ตœ์ดˆ๋“ฑ๋ก์ผ 2023.04.05 ์ตœ์ข…์ ฟ’์ž‘์ผ 2000.03
14P ๋ฏธ๋้ฉ๋ณด๊ธฐ
The Finite Element Formulation and Its Classification of Dynamic Thermeoelastic Problems of Solids
  • * ๋ณธ ๋ฌธ์„œ๋Š” ๋ฐฐํฌ์šฉ์œผ๋กœ ๋ณต์‚ฌ ๋ฐ ํŽธ์ง‘์ด ๋ถˆ๊ฐ€ํ•ฉ๋‹ˆ๋‹ค.

    ๋ฏธ๋้ฉ๋ณด๊ธฐ

    ์„œ์่ง์ •๋ต–

    ยท ๋ฐœํ–‰๊ธฐ๊ด€ : ํ•œ๊ตญ์ „์‚ฐ๊ตฌ์กฐ๊ณตํ•™ํšŒ
    ยท ์ˆ˜๋ก์ง€ ์ •๋ณด : ํ•œ๊ตญ์ „์‚ฐ๊ตฌ์กฐ๊ณตํ•™ํšŒ ๋…ผ๋ๅฉ์ง‘ / 13๊ถŒ / 1ํ˜ธ
    ยท ์ €์ž๋ช… : Yun Seong Ho

    ์ดˆ๋ก

    ํŒ ๋…ผ๋ๅฉ์€ ๊ตฌ์กฐ๋ญ„์˜ ๋™์—ญํ•™ ๋ฐ ์—ด๋‹จ์„ฑ ์—ฐ์„ฑ๋ฌธ์ œ ํ•ด์„์„ ์œ„ ํ•œ ํ†ตํ•ฉ๋œ ์œ ํ•œ์š”์†Œ๋ฒ•์„ ๊ฐœ ๋ฐœํ•˜๋…ผ๋ฐ ์ดˆ์ ‘์„ ๋ˆ„๊ณ 
    ์žˆ๋‹ค. ์ฒซ ์งธ๋กœ. ์—ด์ „๋„ ๋ฐฉ์ •์‹์ดl ์—ด๋ณ€์œ„๋ผ๋Š” ๋ฌต๋ฆฌ๋Ÿ‰์„ ๋„์—ฝํ•˜์—ฌ ํ’์—ญํ•™์˜ ์šด๋™ ๋น™์ •์‹ํŒŒ ์œ ์‚ฌํ•˜๋„๋ก ์œ ๋„ํ•œ ํ›„.
    ๋ณ€๋ถ„๋ฒ•๊ณผ ์ผ๋ฐ˜์ขŒํ‘œ๊ณ„๋ฅผ ์ด์šฉํ•˜์—ฌ ์‹œ๊ฐ„์˜์—ญ์—์„œ ์ •์‹ํ™”ํ•˜์˜€๋‹ค ๋‘˜์งธํฌ๏ผŒ ๋‘ ๋ฑ…์ •์‹์–ด] ๋ผ๋ธ”๋ผ์Šค ๋ณ€ ํŒ์„ ๋™์‹œ์— ๋„
    ์ž…ํ•˜๊ณ  - ๊ณต๊ฐ„๋ณ€์ˆ˜์•ˆ์„ ๊ฐ–๋Š” ํ˜•์„ฑํ•จ์ˆ˜์งœ ๊ฐ€์ฆ์ž”์—ฌ๋ฒˆ์„ ์ ์šฉํ•˜์—ฌ ์œ ํ•œ์š”์†Œ์‹์„ ๋ณ€ํ™˜์˜์—ญ์—์„œ ํ‘œ ํ—Œ ํ•˜์˜€๋‹ค. ์—ฐ์„ฑ๋œ
    ๋น™์ • ์‹ ์„ ์šด์ง€l ์˜ ํŠน์„ฑ์— ๋”ฐ๋ผ์„œ ๋ถ„๋ฅ˜ํ•˜์˜€๊ณ  ์ •์‹ํ™” ํŒŒ์ •์„ ๊ฒ€์ˆญํ•˜์˜€๋‹ค ๋˜ํ•œ ์ˆ˜์น˜ํ•ด์„ ์•Œ๊ณ ๋ฆฌ ๋Š  ์ด ๊ฐ–๋Š” ์ˆ˜์น˜ ์—ญ
    ๋ณ€ํ™˜์˜ ์ •์„ฑ์ ์ธ ๊ฒฝํ–ฅ์— ๋Œ€ํ•˜์—ฌ ๊ฒ€ํ† ํ•˜์˜€๋‹ค-

    ์˜์–ด์ดˆ๋ก

    This paper is for the first essential study on the development of unified finite element formulations
    for solving problems related to the dynamics/thermoelastics behavior of solids. 1n the first paฯ€ of
    fOI111Ulations, the finite element method is based on the int:roduction of a new quantity defin์–ด as heat
    displacement. which allows the heat conduction equations to be ใ€;vTitten in a form equivaJent to the
    equation of motion. and the equations of coupled thermoelasticity to be written in a unified form. The
    equations obtajned are used to express a vmiational formulation which. together with the concept of
    generalized coordinates, yields a set of differentiaJ equations with the time as an independent val๋ )le
    Using the LapJace transfonn. the resuJting finite eJement equations aJ.โ€˜e described in the tranSf0l111
    dom๋ฉฐn. In the second. the Laplace transform is applied to both the equation of heat conduction derived
    in the first pm1 and the equations of motions and their corresponding boundmฮณ conditions, ใ€;v'hi ch is
    refelTed to the tra.nsformed equation. SeJections of intell)oJation functions dependent on only the space
    variable and an application of the weighted residuaJ method to the coupled equation result in the
    necessa.ry fi ๋ te eJement matrices in the transformed domain. Fin๋ฉฐ l y. to 11rove the validity of two
    approaches. a compmison with one finite eJement equation and the other is made tenn by teml.

    ์ฐธ๊ณ ์ž๋ฃŒ

    ยท ์—†์Œ

    ํƒœ๊ทธ

  • ์ž๋ฃŒํ›„๊ธฐ

    Ai ๋ฆฌ๋ทฐ
    ์ด ์ž๋ฃŒ๋ฅผ ํ†ตํ•ด ์ƒˆ๋กœ์šด ์ง€์‹๊ณผ ํ†ต์ฐฐ์„ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๊ณ , ๊ณผ์ œ๋ฅผ ๋ฅผ ๋ณด์™„ํ•˜๋Š” ๋ฐ ํฐ ๋„์›€์ด ๋˜์—ˆ์Šต๋‹ˆ๋‹ค. ๋งค์šฐ ๋งŒ์กฑ์Šค๋Ÿฌ์› ์Šต๋‹ˆ๋‹ค. ์ถ”์ฒœํ•  ๋งŒํ•œ ์ž๋ฃŒ์ž…๋‹ˆ๋‹ค.
    • ์ž์ฃผ๋ฌป๋Š”์งˆ๋ๅฉ์˜ ๋‹ต๋ณ€์„ ํ™•์ธํ•ด ์ฃผ์„ธ์š”

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      • ๋ณธ ํ•™์ˆ ๋…ผ๋ๅฉ์€ (์ฃผ)์ฝ”๋้ฉ์•„์Šค์นผ๋ผ์™ฟ’ ๊ฐ ํ•™ํšŒ๊ฐ„์— ์ €์ž‘๊ถŒ๊ณ„์•ฝ์ด ์ฒด๊ฒฐ๋œ ๊ฒƒ์œผ๋กœ AgentSoft๊ฐ€ ์ œ๊ณต ํ•˜๊ณ  ์žˆ์Šต๋‹ˆ๋‹ค.
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      • ํ•ดํ”ผ์บ ํผ์Šค๋Š” ๊ตฌ๋งค์ž์™ฟ’ ํŒ๋งค์ž ๋ชจ๋‘๊ฐ€ ๋งŒ์กฑํ•˜๋Š” ์„œ๋น„์Šค๊ฐ€ ๋˜๋„๋ก ๋…ธ๋ ฅํ•˜๊ณ  ์žˆ์œผ๋ฉฐ, ์•„๋ž˜์˜ 4๊ฐ€์ง€ ์ž๋ฃŒํ™˜๋ถˆ ์กฐ๊ฑด์„ ๊ผญ ํ™•์ธํ•ด์ฃผ์‹œ๊ธฐ ๋ฐ”๋ž๋‹ˆ๋‹ค.
        ํŒŒ์ผ์˜ค๋ฅ˜ ์ค‘๋ณต์ž๋ฃŒ ์ €์ž‘๊ถŒ ์—†์Œ ์„ค๋ช…๊ณผ ์‹ค์ œ ๋‚ด์šฉ ๋ถˆ์ผ์น˜
        ํŒŒ์ผ์˜ ๋‹ค์šด๋กœ๋“œ๊ฐ€ ์ œ๋Œ€๋กœ ๋˜์ง€ ์•Š๊ฑฐ๋‚˜ ํŒŒ์ผํ˜•์‹์— ๋งž๋Š” ํ”„๋กœ๊ทธ๋žจ์œผ๋กœ ์ •์ƒ ์ž‘๋™ํ•˜์ง€ ์•Š๋Š” ๊ฒฝ์šฐ ๋‹ค๋ฅธ ์ž๋ฃŒ์™ฟ’ 70% ์ด์ƒ ๋‚ด์šฉ์ด ์ผ์น˜ํ•˜๋Š” ๊ฒฝ์šฐ (์ค‘๋ณต์ž„์„ ํ™•์ธํ•  ์ˆ˜ ์žˆ๋Š” ๊ทผ๊ฑฐ ํ•„์š”ํ•จ) ์ธํ„ฐ๋„ท์˜ ๋‹ค๋ฅธ ์‚ฌ์ดํŠธ, ์—ฐ๊ตฌ๊ธฐ๊ด€, ํ•™๊ป“, ์„œ์  ๋“ฑ์˜ ์ž๋ฃŒ๋ฅผ ๋„์šฉํ•œ ๊ฒฝ์šฐ ์ž๋ฃŒ์˜ ์„ค๋ช…๊ณผ ์‹ค์ œ ์ž๋ฃŒ์˜ ๋‚ด์šฉ์ด ์ผ์น˜ํ•˜์ง€ ์•Š๋Š” ๊ฒฝ์šฐ

    โ€œํ•œ๊ตญ์ „์‚ฐ๊ตฌ์กฐ๊ณตํ•™ํšŒ ๋…ผ๋ๅฉ์ง‘โ€์˜ ๋‹ค๋ฅธ ๋…ผ๋ๅฉ๋„ ํ™•์ธํ•ด ๋ณด์„ธ์š”!

    ๋ฌธ์„œ ์ดˆ์•ˆ์„ ์ƒ์„ฑํ•ด์ฃผ๋Š” EasyAI
    ์•ˆ๋…•ํ•˜์„ธ์š”. ํ•ดํ”ผ์บ ํผ์Šค์˜ ๋ฐฉ๋Œ€ํ•œ ์ž๋ฃŒ ์ค‘์—์„œ ์„ ๋ณ„ํ•˜์—ฌ ๋‹น์‹ ๋งŒ์˜ ์ดˆ์•ˆ์„ ๋งŒ๋“ค์–ด์ฃผ๋Š” EasyAI ์ž…๋‹ˆ๋‹ค.
    ์ €๋Š” ์•„๋ž˜์™ฟ’ ๊ฐ™์ด ์ž‘์—…์„ ๋„์™ฟ’๋“œ๋ฆฝ๋‹ˆ๋‹ค.
    - ์ฃผ์ œ๋งŒ ์ž…๋ ฅํ•˜๋ฉด ๋ชฉ์ฐจ๋ถ€ํ„ฐ ๋ณธ๋ฌธ๋‚ด์šฉ๊นŒ์ง€ ์ž๋™ ์ƒ์„ฑํ•ด ๋“œ๋ฆฝ๋‹ˆ๋‹ค.
    - ์žฅ๋ฌธ์˜ ์ฝ˜ํ…์ธ ๋ฅผ ์‰ฝ๊ณ  ๋น ๋ฅด๊ฒŒ ์ž‘์„ฑํ•ด ๋“œ๋ฆฝ๋‹ˆ๋‹ค.
    - ์Šคํ† ์–ด์—์„œ ๋ฌด๋ฃŒ ์บ์‹œ๋ฅผ ๊ณ„์ •๋ณ„๋กœ 1ํšŒ ๋ฐœ๊ธ‰ ๋ฐ›์„ ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค. ์ง€๊ธˆ ๋ฐ”๋กœ ์ฒดํ—˜ํ•ด ๋ณด์„ธ์š”!
    ์ด๋Ÿฐ ์ฃผ์ œ๋“ค์„ ์ž…๋ ฅํ•ด ๋ณด์„ธ์š”.
    - ์œ ์•„์—๊ฒŒ ์ ํ•ฉํ•œ ๋ฌธํ•™์ž‘ํ’ˆ์˜ ๊ธฐ์ค€๊ณผ ํŠน์„ฑ
    - ํ•œ๊ตญ์ธ์˜ ๊ฐ€์น˜๊ด€ ์ค‘์—์„œ ์ •์‹ ์  ๊ฐ€์น˜๊ด€์„ ์ด๋ฃจ๋Š” ๊ฒƒ๋“ค์„ ๋ฌธํ™”์  ๋ฌธ๋ฒ•์œผ๋กœ ์ •๋ฆฌํ•˜๊ณ , ํ˜„๋Œ€ํ•œ๊ตญ์‚ฌํšŒ์—์„œ ์ผ์–ด๋‚˜๋Š” ์‚ฌ๊ฑด๊ณผ ์‚ฌ๊ณ ๋ฅผ ๋น„๊ตํ•˜์—ฌ ์ž์‹ ์˜ ์˜๊ฒฌ์œผ๋กœ ๊ธฐ์ˆ ํ•˜์„ธ์š”
    - ์ž‘๋ณ„์ธ์‚ฌ ๋…ํ›„๊ฐ
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