Magnetic Levitation Effect of High-Tc Superconducting Bulk 㜞᷷⿥વዉ䊋䊦䉪䈱⏛᳇ᶋ਄․ᕈ㩷

㜞᷷⿥વዉ䊋䊦䉪䈱⏛᳇ᶋ਄․ᕈ㩷

㩷

᧻ᧄᵗ᣿

ቯ౗⚐ᐔ

ኅේ๺਽

ࠕࠠ࡜

ේ↰ ኡᴦ

㩷

Magnetic Levitation Effect of High-Tc Superconducting Bulk

Hiroaki MATSUMOTO

Junpei SADAKANE

Kazuya IEHARA

AKIRA

Kanji HARADA

Since the discovery of high-temperature superconductivity, it has been studied for the applications and the developments in various fields. The superconducting fault-current limiter (FCL) is one of the superconducting applications, witch reduces the current to the level that the circuit breaker can easily work. The temperature becomes high caused by a Joule heat when fault electric current is restrained. We need high cooling efficiency to restore the accidental status to the normal one immediately.

We took note of cavities in the bulk and measured magnetic levitation effect as the basics. I fabricated the bulks that have many cavities by varying the sintering temperature and the pressure. As the result, I understood that cooling effect was increased and levitation time improved by lowering the cavity density.

Key words:

Y123 superconductors, Magnetic Levitation Effect 㩷

㩷

㩷 䋱䋮䈲䈛䉄䈮㩷 㩷

㜞᷷⿥વዉ૕߇⊒⷗ߐࠇߡએ᧪㧘ࠃࠅ㜞޿⥃⇇᷷ᐲ 㧔6E㧕㧘ࠃࠅ㜞޿⥃⇇㔚ᵹኒᐲ㧔,E㧕ࠍ᳞߼ߡ㧘ᄙߊߩ

⎇ⓥ߇ߥߐࠇߡ߈ߚ

㧚߹ߚ㧘࡚ࠫ࠮ࡈ࠰ࡦធวࠍ↪

޿ߚ 537+& ߣ๭߫ࠇࠆ⿥㜞ᗵᐲߩ⏛᳇࠮ࡦࠨ࡯ߩ⎇ⓥ

߽⋓ࠎߦߥߐࠇߡ޿ࠆ

㧚

⿥વዉߩᔕ↪ߩ৻ߟߦ㒢ᵹེ߇޽ࠆޕ㒢ᵹེߣߪ㔚 ജ♽⛔ߦ߅ߌࠆ⪭㔗╬ߦࠃࠆ੐᡿⍴⛊㔚ᵹࠍ⍍ᤨߦᛥ

೙ߒߡޔㆤᢿࠍኈᤃߦߔࠆ㔚ജᯏེ ߩߎߣߢ޽ࠆޕㆊ 㔚ᵹ߇ᵹࠇߚߣ߈ߦ⿥વዉ⁁ᘒ߆ࠄᏱ㔚ዉ⁁ᘒߦォ⒖ ߔࠆߎߣࠍ೑↪ߒߡ↪޿ࠄࠇࠆޕߘߩߣ߈⿥વዉ૕ߪ

੐᡿㔚ᵹᛥ೙ᤨߦࠫࡘ࡯࡞ᾲߦࠃࠅ㜞᷷ߣߥࠆ

ޕ੐

᡿ᓟߩᓳᣥࠍㅦ߿߆ߦߔࠆߚ߼ߦ಄ළല₸ࠍ㜞߼ࠆᔅ ⷐ߇޽ࠆޕ

ߘߎߢᧄ⎇ⓥߢߪ Y123 ࡃ࡞ࠢߩኒᐲߦ⌕⋡ߒޔࡑ

ࠗࠬ࠽࡯ലᨐߦࠃࠆ⏛⍹ᶋ਄ᤨ㑆ࠍ᷹ቯߒޔኒᐲߣ಄

ළലᨐߩ㑐ଥࠍ⺞ߴߚޕኒᐲߪ὾ᚑ᷷ᐲߣࡃ࡞ࠢ૞ᚑ

ᤨߩࡊ࡟ࠬ࿶ߦࠃߞߡᄌൻߐߖߚޕߘߩ⚿ᨐޔૐኒᐲ ൻߔࠆߎߣߦࠃࠅᶧ૕⓸⚛ߦࠃࠆ಄ළലᨐ߇㜞߹ࠅᶋ

਄ᤨ㑆߇ะ਄ߔࠆߎߣ߇ࠊ߆ߞߚޕ

䋲䋮ታ㛎ᣇᴺ㩷 㩷 㪉㪅㪈㩷 ⹜ᢱ૞⵾ᣇᴺ㩷

⹜ᢱߩ૞⵾ߦߪ㉄ൻࠗ࠶࠻࡝࠙ࡓ (Y ₂ O ₃ ) ޔ὇㉄ࡃ࡝

࠙ࡓ (BaCO 3 ) ޔ㉄ൻ㌃ (CuO) ࠍ↪޿ࠆޕߎࠇࠄߩ᧚ᢱࠍ

⚵ᚑᲧ߇ Y 㧦 Ba 㧦 Cu㧩1 㧦 2 㧦 3 ߣߥࠆࠃ߁ߦᷙวߔࠆޕ ߪߓ߼⦡߇⇣ߥࠆ㉄ൻࠗ࠶࠻࡝࠙ࡓߣ㉄ൻ㌃ࠍ੃㋬ߦ

౉ࠇ⦡߇ဋ৻ߦߥࠆ߹ߢ⦟ߊᷙߗߚᓟޔ὇㉄ࡃ࡝࠙ࡓ ࠍട߃ߐࠄߦᷙߗࠆޕߎࠇࠍ὾⚿ߐߖࠆߎߣߦࠃࠅ⿥

વዉ‛⾰ߢ޽ࠆ㨅Ba 2 Cu 3 O 7 -x ࠍᓧࠆߎߣ߇ߢ߈ࠆޕ

ᰴߦਇ⚐‛ࠍขࠅ㒰߈⋡⊛ߩ⚵ᚑ‛ࠍᓧࠆߚ߼ߦ઒

὾ᚑࠍⴕߥ߁ޕ઒὾ᚑߦߪ㔚᳇Ἱࠍ↪޿ 10[ ͠ /min] ߢ 900 ͠߹ߢ᣹᷷ޔ 5 ᤨ㑆଻ᜬߒߚᓟ 10[ ͠ /min] ߢቶ᷷߹

ߢ㒠᷷ߔࠆޕဋ৻ᕈࠍ㜞߼ࠆߚ߼ߦ઒὾ᚑࠍ 5 ࿁ⴕߞ ߚޕ

ߘߒߡ὾ᚑ᷷ᐲߣኒᐲᲧߩ㑐ଥࠍ⺞ߴࠆߚ߼ߦዊဳ

ߩ㊄ဳ ( ⋥ᓘ 1.3cm) ࠍ↪޿ߡࡃ࡞ࠢ⁁ߦᚑဳߔࠆޕࡊ࡟

ࠬ࿶ߪ 8kN ߣߒޔ 850͠ޔ 900͠ޔ 950͠ߢᧄ὾ᚑࠍⴕ ߞߚޕᧄ὾ᚑߢߪ⋡⊛᷷ᐲ߹ߢߪ 10[ ͠ /min] ߢ᣹᷷ߒޔ 20 ᤨ㑆଻ᜬޔߘߒߡቶ᷷߹ߢ 1[ ͠ /min] ߢ㒠᷷ߒߚޕ

߹ߚࡊ࡟ࠬ࿶ߣኒᐲᲧߩ㑐ଥࠍ᳞߼ࠆߚ߼ᄢဳߩ㊄

ဳ(⋥ᓘ 6.0cm)ࠍ↪޿ߡᚑဳߒߚޕࡊ࡟ࠬ࿶ࠍ 25kNޔ

40kN ޔ 60kN ߣߒ 900 ͠ߢ਄⸥ߣหߓࡊࡠ࠮ࠬߢᧄ὾

ᚑࠍⴕߞߚޕ

ේⓂฃઃ ᐔᚑ 20 ᐕ 9 ᦬ 1 ᣣ 㧖 ኾ᡹⑼㔚ሶ࡮ᖱႎࠪࠬ࠹ࡓᎿቇኾ᡹

㧖㧖 㔚᳇㔚ሶᎿቇ⑼ 㧡ᐕ

㧖㧖㧖 㔚᳇㔚ሶᎿቇ⑼

㪉㪅㪉㩷 ⹜ᢱ䈱⹏ଔᣇᴺ㩷

ᧄ⎇ⓥߢߪ⿥વዉࡃ࡞ࠢౝߦ޽ࠆⓨሹߦ⌕⋡ߔࠆޕ ߘߩߚ߼ࡃ࡞ࠢߦߤߩߊࠄ޿ߩഀวߢⓨሹ߇ሽ࿷ߔࠆ ߆ࠍ⴫ߔߚ߼ߦኒᐲᲧࠍ↪޿ࠆޕ૞⵾ߒߚ⹜ᢱߩኒᐲ Ყࠍᰴᑼߦࠃࠅ᳞߼ߚޕ

ߎߎߢࡃ࡞ࠢ⾰㊂ߣߪታ㓙ߩࡃ࡞ࠢߩ㊀㊂ߢ޽ࠅޔℂ

⺰⾰㊂ߣߪ Y123 ߩᩰሶቯᢙߣࡃ࡞ࠢߩ૕Ⓧ߆ࠄ⸘▚

ߒߡ᳞߼ߚ୯ߢ޽ࠆޕߟ߹ࠅኒᐲᲧ߇ 100[%] ߩߣ߈ޔ

ⓨሹ߇ߥߊቢోߦኒߦ⹣߹ߞߡ޿ࠆߎߣࠍᗧ๧ߒޔ

50[%] ߩߣ߈ߪࡃ࡞ࠢߩඨಽߪⓨሹߢ޽ࠆߎߣࠍᗧ๧

ߔࠆޕ૕Ⓧߪࡁࠡࠬࠍ↪޿ߡࡃ࡞ࠢߩ⋥ᓘߣෘߐࠍ᷹

ቯߒޔ▚಴ߒߚޕ

ࡑࠗࠬ࠽࡯ലᨐߦࠃࠆ⏛⍹ߩᶋ਄․ᕈࠍ Fig.1 ߦ␜

ߔޕ߹ߕࡃ࡞ࠢࠍᶧ૕⓸⚛ਛߢ಄ළߒޔࡀࠝࡑ࠶ࠢࠬ

⏛⍹ߩ਄ߦਸ਼ߖޔᶋ਄ᤨ㑆߅ࠃ߮ᶋ਄㜞ߐࠍ⸘᷹ߒߚޕ ᄢဳࡃ࡞ࠢߩ႐วߪޔࡃ࡞ࠢߩ਄ߦ⏛⍹ࠍਸ਼ߖ᷹ቯߒ ߚޕ৻ߟߩ⹜ᢱߦኻߒ 5 ࿁᷹ቯߒޔߘߩᐔဋࠍ᳞߼ߚޕ ᶧ૕⓸⚛ߦࠃࠆ଻಄ലᨐࠍ⏕߆߼ࠆߚ߼ߦࡃ࡞ࠢߦ

଻ᜬߐࠇࠆᶧ૕⓸⚛ߩ㊂ࠍ᷹ቯߒߚޕ߹ߕ಄ළ೨ߦࡃ

࡞ࠢߩ㊀㊂ࠍ᷹ࠆޕᰴߦࡃ࡞ࠢࠍᶧ૕⓸⚛ਛߦ౉ࠇ᳇

ᵃ߇಴ߥߊߥࠆ߹ߢචಽߦ಄ළߒߚᓟޔౣ߮ࡃ࡞ࠢߩ

㊀㊂ࠍ᷹ቯߒޔߘߩ㊀㊂ߩᏅࠍ᳞߼ߚޕ

߹ߚ⿛ᩏဳ㔚ሶ㗼ᓸ㏜ 㧔 SEM 㧕ࠍ↪޿ߡ⹜ᢱ⴫ 㕙ߩ

ⷰኤࠍⴕߞߚޕ SEM ࠍ↪޿ߡࡃ࡞ࠢߩⓨሹߥߤࠍ⺞ߴ ߚޕ

㩷 㩷 㩷

䋳䋮ታ㛎⚿ᨐ䈫⠨ኤ㩷 㩷

㪊㪅㪈㩷 ὾ᚑ᷷ᐲ䈫ᶋ਄․ᕈ㩷

ᧄ὾ᚑ᷷ᐲߣኒᐲᲧߩ㑐ଥࠍ Fig.2 ߦ␜ߔޕߎߩ࿑

ࠃࠅ὾ᚑ᷷ᐲ߇㜞޿߶ߤኒᐲᲧ߽㜞ߊߥߞߡ޿ࠆߎߣ ߇ಽ߆ࠆޕߎࠇߪ㜞᷷ߢ὾⚿ߔࠆߣޔ⚿᥏☸߇ࠃࠅ෼

❗ߔࠆߚ߼ߛߣᕁࠊࠇࠆޕ

ኒᐲᲧߣᶋ਄ᤨ㑆ߩ㑐ଥࠍ Fig.3 ߦ␜ߔޕኒᐲᲧߩૐ ਅߦ઻޿ޔᶋ਄ᤨ㑆߇ะ਄ߔࠆ௑ะߦ޽ࠆߎߣ߇ࠊ߆ ࠆޕኒᐲᲧ߇ૐ޿ߣ޿߁ߎߣߪࡃ࡞ࠢߦᄙᢙߩⓨሹ߇

޽ࠆߣ⠨߃ࠄࠇࠆޕߎߩⓨሹౝߦᶧ૕⓸⚛߇౉ࠅㄟߺ

଻಄ലᨐ߇㜞߹ߞߚߚ߼ߢߪߥ޿߆ߣ⠨߃ࠄࠇࠆޕ ኒᐲᲧߣᶋ਄㜞ߐߩ㑐ଥࠍ Fig.4 ߦ␜ߔޕૐኒᐲൻߔ ࠆߎߣߦࠃࠅᶋ਄ᤨ㑆߇ะ਄ߒߚ৻ᣇޔᶋ਄㜞ߐߪૐ ߊߥࠆ⚿ᨐߣߥߞߚޕ

㨇㧑㨉 ℂ⺰⾰㊂

ࡃ࡞ࠢ⾰㊂

ኒᐲᲧ = × 100

㪍㪇 㪍㪌 㪎㪇 㪎㪌 㪏㪇

㪏㪇㪇 㪏㪌㪇 㪐㪇㪇 㪐㪌㪇 㪈㪇㪇㪇

㪪㫀㫅㫋㪼㫉㫀㫅㪾㩷㪫㪼㫄㫇㪼㫉㪸㫋㫌㫉㪼㪲㷄㪴

㪛㪼㫅㫊㫀㫋㫐㩷㫉㪸㫋㫀㫆㪲㩼㪴

Fig.2 The relation of sintering temperature and density ratio

㪇 㪈㪇 㪉㪇 㪊㪇 㪋㪇

㪍㪇 㪍㪌 㪎㪇 㪎㪌 㪏㪇

㪛㪼㫅㫊㫀㫋㫐㩷㫉㪸㫋㫀㫆㪲㩼㪴

㪣㪼㫍㫀㫋㪸㫋㫀㫆㫅㩷㫋㫀㫄㪼㪲㫊㪴

㪇 㪈 㪉 㪊 㪋 㪌

㪍㪇 㪍㪌 㪎㪇 㪎㪌 㪏㪇

㪛㪼㫅㫊㫀㫋㫐㩷㫉㪸㫋㫀㫆㪲䋦㪴

㪣㪼㫍㫀㫋㪸㫋㫀㫆㫅㩷㪿㪼㫀㪾㪿㫋㪲㫄㫄㪴

Fig.1 Magnetic levitation by Meissner effect Superconducting

Bulk

Magnet

Fig.3 The relation of density ratio and levitation time

Fig.4 The relation of density ratio

and levitation height

㪊㪅㪉㩷 䊒䊧䉴࿶䈫ᶋ਄․ᕈ㩷

ᄢဳࡃ࡞ࠢࠍ↪޿ߡ᷹ቯߒߚࡊ࡟ࠬ࿶ߣኒᐲᲧߩ㑐

ଥࠍ Fig.5 ߦ␜ߔޕߎߩ࿑߆ࠄࡊ࡟ࠬ࿶ࠍૐߊߔࠆߎ

ߣߦࠃߞߡኒᐲᲧ߇ਅ߇ࠆߎߣ߇ࠊ߆ߞߚޕߎࠇߦࠃ ࠅࡊ࡟ࠬߢߩᚑဳᤨߩኒᐲ߇ᧄ὾ᚑᓟߦ߽ᓇ㗀ߔࠆߎ ߣ߇ಽ߆ߞߚޕ

ᄢဳࡃ࡞ࠢࠍ↪޿ߡ᷹ቯߒߚኒᐲᲧߣᶋ਄ᤨ㑆ߩ㑐

ଥࠍ Fig.6 ߦ␜ߔޕࡊ࡟ࠬ࿶ߦࠃࠆኒᐲᲧߩᄌൻߢ߽

὾ᚑ᷷ᐲᄌൻᤨߣห᭽ߦૐኒᐲൻߔࠆߎߣߦࠃࠅᶋ਄

ᤨ㑆߇ะ਄ߔࠆߎߣ߇ಽ߆ߞߚޕ

ኒᐲᲧߣࡃ࡞ࠢౝߦ଻ᜬߐࠇࠆᶧ૕⓸⚛㊂ߩ㑐ଥࠍ

Fig.7 ߦ␜ߔޕ Fig.7 ࠃࠅࡃ࡞ࠢౝߦᶧ૕⓸⚛߇౉ࠅㄟ

ࠎߢ޿ࠆߎߣ߇⏕⹺ߢ߈ߚޕߎࠇߪኒᐲᲧߩૐਅߦ઻

޿ޔන૏૕Ⓧ޽ߚࠅߩᶧ૕⓸⚛଻ᜬ㊂߇Ⴧടߒߡ޿ࠆ ߎߣࠍ␜ߒߡ޿ࠆޕ

㪊㪅㪊㩷 䌓䌅䌍䈮䉋䉎⴫㕙ⷰኤ㩷

ᄢဳࡃ࡞ࠢߩ⹜ᢱ SEM ౮⌀ࠍ Fig.8 ߦ␜ߔޕSEM ౮⌀߆ࠄታ㓙ߦࡃ࡞ࠢౝߩⓨሹߩ᭽ሶࠍ⷗ࠆߎߣ߇ߢ ߈ࠆޕ⚂㧡Ǵ m ߩ⿥વዉߩ☸ሶ߇὾⚿ߔࠆߎߣߦࠃࠅ

⚿วߒߡࡃ࡞ࠢࠍᒻᚑߒߡ޿ࠆޕߘߩ☸ሶߣ☸ሶߩ㑆 ߦⓨሹ߇ሽ࿷ߒߡ޿ࠆޕߎࠇࠄߩⓨሹߪࡊ࡟ࠬ࿶߇ૐ

޿ߣ߈ߦߪᄢ߈ߊᄙᢙሽ࿷ߒߡ޿ࠆޕߎࠇߪࡊ࡟ࠬ࿶

߇ૐ޿ߣ߈ኒᐲᲧ߽ૐߊߥߞߚ⚿ᨐࠍⵣઃߌߡ޿ࠆޕ

㩷 䋴䋮 ⠨ ኤ㩷

㪌㪌 㪍㪇 㪍㪌 㪎㪇 㪎㪌

㪇 㪉㪇 㪋㪇 㪍㪇 㪏㪇

㪧㫉㪼㫊㫊㫌㫉㪼㪲㫂㪥㪴

㪛㪼㫅㫊㫀㫋㫐㩷㫉㪸㫋㫀㫆㪲䋦㪴

㪇 㪇㪅㪈 㪇㪅㪉 㪇㪅㪊 㪇㪅㪋 㪇㪅㪌 㪇㪅㪍

㪌㪌 㪍㪇 㪍㪌 㪎㪇 㪎㪌

㪛㪼㫅㫊㫀㫋㫐㩷㫉㪸㫋㫀㫆㪲㩼㪴 㪨㫌㪸㫅㫋㫀㫋㫐㩷㫆㪽 㩷㩷㩷㩷㩷㩷㩷㩷㩷㫃㫀㫈㫌㫀㪻㩷㪥㪉㩷㪲㪾㪆㪺㫄㪊㪴

㪇 㪉㪇 㪋㪇 㪍㪇 㪏㪇 㪈㪇㪇 㪈㪉㪇

㪌㪌 㪍㪇 㪍㪌 㪎㪇 㪎㪌

㪛㪼㫅㫊㫀㫋㫐㩷㫉㪸㫋㫀㫆㪲䋦㪴

㪣㪼㫍㫀㫋㪸㫋㫀㫆㫅㩷㫋㫀㫄㪼㪲㫊㪴

(c) Pressure 60[kN]

Fig.5 The relation of pressure and density ratio

Fig.6 The relation of density ratio and levitation time

Fig.7 The relation of density ratio and quantity of liquid N

Fig.8 SEM images of bulks (b) Pressure 40[kN]

(a) Pressure 25[kN]

ࡃ࡞ࠢ૞⵾ᤨߩᧄ὾ᚑ᷷ᐲ޽ࠆ޿ߪࡊ࡟ࠬ࿶ࠍᄌൻ ߐߖࠆߎߣߦࠃࠅޔኒᐲࠍᄌൻߐߖࠆߎߣ߇ߢ߈ࠆޕ ߘߒߡኒᐲࠍૐߊߔࠆߎߣߦࠃࠅࡃ࡞ࠢౝߦⓨሹ߇ߢ ߈ߘߎߦᶧ૕⓸⚛߇଻ᜬߐࠇᶋ਄ᤨ㑆߇ะ਄ߒߚޕߎ ࠇߪⓨሹౝߦᶧ૕⓸⚛߇౉ࠆߎߣߦࠃࠅ଻಄ലᨐ߇㜞

߹ߞߚߚ߼ߛߣᕁࠊࠇࠆޕ

ᶧ૕⓸⚛ਛߢ 77[K] ߦ಄ළߐࠇߚࡃ࡞ࠢߪ⥃⇇᷷ᐲ

ߢ޽ࠆ⚂ 90[K]ߦߥࠆ߹ߢᶋ਄ߒ⛯ߌࠆߣ⠨߃ࠄࠇࠆޕ

㨅 123 ߩਥᚑಽߢ޽ࠆ㌃ߣᶧ૕⓸⚛ߩන૏૕Ⓧ޽ߚࠅ ߩᲧᾲࠍߊࠄߴࠆߣ㌃㧦 3.392 [J/cm

㨯 K] ޔᶧ૕⓸⚛㧦 0.839[J/cm

㨯 K] ߢ޽ࠆޕ⿥વዉ߆ࠄᏱવዉߦォ⒖ߔࠆ

߹ߢߦ 13[K]ߩ᷷ᐲ਄᣹ࠍᔅⷐߣߔࠆߩߢޔߘࠇߙࠇ

ᔅⷐߥᾲ㊂ߪ㌃㧦 44.1[J/cm

] ޔᶧ૕⓸⚛㧦 10.9[J/cm

] ߣ㌃ߩ߶߁߇ᄢ߈޿ޕߒ߆ߒᶧ૕⓸⚛ߦߪ᳇ൻᾲ߇޽

ࠅන૏૕Ⓧ޽ߚࠅ 160.6[J/cm

] ߢ޽ࠆޕߘߩߚ߼ว⸘

ߔࠆߣ㌃㧦44.1 [J/cm

]ߦኻߒᶧ૕⓸⚛㧦 171.5 [J/cm

] ߣߥࠅᶧ૕⓸⚛ࠍࡃ࡞ࠢౝߦ଻ ᦭ߔࠆߎߣߦࠃࠅ଻಄

ലᨐ߇㜞߹ࠆޕ

ኒᐲᲧߩૐਅߦ઻޿ᶋ਄㜞ߐ߇ૐਅߒߚޕߘ߽ߘ߽

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ࠍឃ㒰ߒޔߘߩ෻⊒ജߢᶋ਄ߔࠆޕߎߎߢࡃ࡞ࠢࠍૐ ኒᐲൻߔࠆߣᏱવዉߢ޽ࠆⓨሹߩഀว߇ჇടߔࠆޕᏱ વዉߪ⏛ ᧤ࠍㅢߔߚ߼৻ㇱߢ⏛᧤߇⽾ㅢߒ෻⊒ജ߇ᒙ

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὾ᚑ᷷ᐲࠍૐߊߔࠆ߆ࡊ࡟ࠬ࿶ࠍૐߊߔࠆߎߣߦࠃ ࠅޔࡃ࡞ࠢߩኒᐲࠍૐߊߔࠆߎߣ߇ߢ߈ࠆޕૐኒᐲൻ ߢᄙᢙߩⓨሹ߇޽ࠆࡃ࡞ࠢߪޔⓨሹߦᶧ૕⓸⚛ࠍ଻ᜬ ߔࠆߎߣ߇ߢ߈଻಄ലᨐ߇㜞߹ࠆޕߘߩߚ߼ࡃ࡞ࠢߩ ᶋ਄ᤨ㑆߇ะ਄ߒߚޕ

߹ߚᶧ૕⓸⚛ਛߦ߅޿ߡᄙሹ⾰ߩࡃ࡞ࠢߪⓨሹౝߦ ᶧ૕⓸⚛߇౉ࠅㄟ߻ߚ߼಄ළല₸߇਄߇ࠆߣᕁࠊࠇࠆޕ ߚߛߒૐኒᐲൻߔࠆߎߣߦࠃࠅࡃ࡞ࠢߩᒝᐲߩૐਅ߿

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