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水中パルスパワー放電を用いた有機色素脱色のバブリングによる高効率化

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᳓ਛࡄ࡞ࠬࡄࡢ࡯᡼㔚ࠍ↪޿ߚ

᦭ᯏ⦡⚛⣕⦡ߩࡃࡉ࡝ࡦࠣߦࠃࠆ㜞ല₸ൻ

㗇⽴ᄥ৻㧘㋈ᧁᢥಷ㧘ධ⼱㕏ผ㧘᧲ጊ⑓ᄦ

㧔2007 ᐕ 8 ᦬ 31 ᣣฃઃ; 2008 ᐕ 2 ᦬ 1 ᣣฃℂ㧕

Improvement of Efficiency of Decolorizing Organic Dye

Using Pulsed Power Discharge by Air Bubbling

Taichi SUGAI, Ayato SUZUKI, Yasushi MINAMITANI and Yoshio HIGASHIYAMA *

(Received August 31, 2007; Accepted February 1, 2008)

Water pollution is one of the global environmental issues at present. We are studying water treatment using pulsed

power discharge in water and air mixture. In this paper, water in a pulsed discharge reactor was

i

njected with large

quantity of air for bubbling. Decololization time of indigo carmine in the treatment by the strong air bubbling is over

15 times faster than that of non-bubbling. As the airflow for the bubbling increased, the decolorization time

decreased. Likewise, as length of the electrode on water increased, the decolorization time decreased. These results

show that more discharge space in air leads to more decreasing of the decolorization time in the water treatment.

Additionally, as size of bubble is made small, the decolorization time decreased. This result shows that large surface

area of air contacting water solution for reaction of active species leads to decreasing of the decolorization time.

1. ߹߃߇߈ ࿾⃿ⅣႺ໧㗴ߩ৻ߟߣߒߡ᳓⾰ᳪᨴߩ໧㗴߇޽ࠅ 㧘ឃ ᳓ಣℂߦ߅޿ߡ૛೾ᳪᵆߩ೥ᷫ㧘㔍ಽ⸃ᕈ‛⾰ߩಽ⸃㧘∛ ේᕈ⚦⩶ߩᲕ⩶㧘㜞ല₸ൻ㧘⋭ࠛࡀ࡞ࠡ࡯ൻ߇᳞߼ࠄࠇߡ ޿ࠆ㧚⃻࿷ߩઍ⴫⊛ߥឃ᳓ಣℂᣇᴺߪᵴᕈᳪᵆᴺ  ߢ޽ ࠆ㧚ߎߩᣇᴺߪ㧘ᄙ⒳㘃ߩᅢ᳇ᕈᓸ↢‛ߦᦑ᳇ࠍⴕ߁ߎߣ ߢᵴᕈൻߐߖߡ㧘ᳪ᳓ਛߩ᦭ᯏ‛ࠍ᳓ߣੑ㉄ൻ὇⚛ߦಽ⸃ ߔࠆᣇᴺߢ޽ࠆ߇㧘ಣℂ⸳஻ߦᐢᄢߥ㕙Ⓧ߇ᔅⷐ㧘ಽ⸃ㅦ ᐲ߇ㆃ޿㧘ᄙ㊂ߩᳪᵆ߇↢ߓࠆߣ޿߁໧㗴߇޽ࠆ㧚 ߘߩߚ߼㧘ᦨㄭߪ㜞ᐲ᳓ಣℂߣߒߡࠝ࠱ࡦಣℂ  ߇૶ ࠊࠇᆎ߼ߡ޿ࠆ㧚ࠝ࠱ࡦߪ㕖Ᏹߦᒝ޿㉄ൻജࠍᜬߞߡ߅ ࠅ㧘ߎߩ㉄ൻജߦࠃࠅ᦭ᯏ‛ߩ㉄ൻ㧘⣕⦡㧘⣕⥇㧘ᶖᲥ߇ น⢻ߢ޽ࠆ㧚ߎߩᣇᴺߪ㧘ᳪᵆ߇↢ߓࠆߎߣ߽ߥߊ㧘ಣℂ ⸳஻ߩ㕙Ⓧ߇ዊߐ޿߁߃㧘ᓥ᧪ߪਇน⢻ߢ޽ߞߚシᐲߥႮ ⚛ൻว‛㧘ࠕࡦࡕ࠾ࠕߩಽ⸃߇น⢻ߢ޽ࠅ㧘Ⴎ⚛ᶖᲥߦ⠴ ᕈࠍ߽ߟ∛ේᕈᓸ↢‛ߩᲕ⩶ߦ߽ലᨐ⊛ߢ޽ࠆ㧚ߒ߆ߒ㧘 ࠝ࠱࠽ࠗࠩ߆ࠄಣℂጀ߳ߩࠝ࠱ࡦߩャㅍᤨߦࠝ࠱ࡦ߇ಽ ⸃ߒߡࠝ࠱ࡦߩ೑↪ല₸߇ਅ߇ࠆߣ޿߁໧㗴߇޽ࠆ㧚߹ ߚ㧘ࠝ࠱࠽ࠗࠩߪ㔚ᭂ㑆ߦ㜞๟ᵄ㜞㔚࿶ࠍශടߔࠆߎߣߢ ࡃ࡝ࡗ᡼㔚ࠍ⊒↢ߐߖ㧘㉄⚛߹ߚߪⓨ᳇ߩ৻ㇱࠍࠝ࠱ࡦൻ ߐߖߡ޿ࠆ߇㧘ߎߩߣ߈หᤨߦ⊒↢ߔࠆ᳓ಣℂߦ᦭ലߥ⍴ ኼ๮ߩᵴᕈ⒳߿⚡ᄖ✢ߪಣℂߦ೑↪ߔࠆߎߣ߇ߢ߈ߕή 㚝ߦߥߞߡߒ߹߁ߣ޿߁໧㗴߇޽ࠆ㧚 ߎࠇࠄߩ໧㗴ࠍ⸃᳿ߔࠆᚻᲑߣߒߡ᳓ਛࡄ࡞ࠬࡄࡢ࡯ ᡼㔚ߦࠃࠆ᳓ಣℂ߇⎇ⓥߐࠇߡ޿ࠆ 6-8)㧚᳓ਛߢࠬ࠻࡝࡯ ࡑࠍ⊒↢ߐߖࠆߣࠝ࠱ࡦ㧘ࡅ࠼ࡠࠠࠪ࡜ࠫࠞ࡞ߥߤߩᵴᕈ ⒳߇᳓ਛߢᄙᢙ↢ᚑߐࠇ8)㧘⚡ᄖ✢߿ⴣ᠄ᵄ߽᳓ਛߢ⊒↢ ߒ㧘ߎࠇࠄߔߴߡࠍಣℂߦ೑↪ߔࠆߎߣ߇ߢ߈ࠆ㧚 ߐࠄߦ᳓ਛࡄ࡞ࠬࡄࡢ࡯᡼㔚ߩ㔚ᭂ㑆ߦⓨ᳇ࠍㅍࠅㄟ ߺࡃࡉ࡝ࡦࠣߔࠆߎߣߢ㧘᳇ᵃౝߢ᡼㔚ࠍ⊒↢ߐߖߡಣℂ ࠍⴕ߁ᣇᴺ߇⎇ⓥߐࠇߡ޿ࠆ9-14)㧚ⓨ᳇ߩ⛘✼⠴ജߪ᳓ߦ Ყߴૐ޿ߩߢ㧘᡼㔚㐿ᆎ㔚࿶߇ਅ߇ࠆߣߣ߽ߦࠬ࠻࡝࡯ࡑ ߇ᒝߊ㐳ߊિ߮ࠆࠃ߁ߦߥࠆ㧚ߎࠇߦࠃࠅᵴᕈ⒳ߩ⊒↢㊂ ߇Ⴧ߃㧘ಣℂല₸߇਄᣹ߔࠆߎߣ߇⏕⹺ߐࠇߡ޿ࠆ㧚 ߎߩᣇᴺߦ߅޿ߡߪ᡼㔚㔚ᭂ㑆ߦሽ࿷ߔࠆⓨ᳇ߩ㊂߇ ಣℂߦኻߒߡ㊀ⷐߥ᧦ઙߢ޽ࠆߣ⠨߃ࠄࠇࠆ㧚ࡃࡉ࡝ࡦࠣ ߔࠆⓨ᳇ߩᵹ㊂ߦኻߔࠆಣℂ₸ߪ㧘㊎ᐔ᧼㔚ᭂ᭴ㅧߩ࡝ࠕ ࠢ࠲ߩ㔚ᭂ㑆ߦ .OKP એਅߩᵹ㊂ߢࡃࡉ࡝ࡦࠣߒߚ႐ว ߩ᦭ᯏ⦡⚛ߩ⣕⦡₸ߦ߅޿ߡ⺞ߴࠄࠇ㧘ᵹ㊂߇Ⴧ߃ࠆ߶ߤ ⣕⦡₸߇ࠃߊߥࠆߎߣ߇ႎ๔ߐࠇߡ޿ࠆ9)㧚ߒ߆ߒ㊎ᐔ᧼ 㔚ᭂ᭴ᚑߪ㊎ߣᐔ᧼㑆ߩᢙ EO ⒟ᐲߩࠡࡖ࠶ࡊ㐳ಽߒ߆᡼ 㔚ⓨ㑆ߦⓨ᳇ߩṛ⇐ߔࠆⓨ㑆߇ߥߊ㧘᡼㔚ߢ⊒↢ߔࠆᵴᕈ ⒳߿⚡ᄖ✢ߣಽ⸃ኻ⽎‛߇෻ᔕߔࠆⓨ㑆߇ዋߥ޿㧚߹ߚⓨ ᳇ߩᵹ㊂߇ዋߥ޿ߣ㧘㔚ᭂ㑆ߦሽ࿷ߔࠆ᳇ᵃߪ௖߆ߢ޽ࠅ ࠠ࡯ࡢ࡯࠼㧦ࡄ࡞ࠬࡄࡢ࡯㧘ࡃࡉ࡝ࡦࠣ㧘 ࠗࡦ࠺ࠖࠧࠞ࡞ࡒࡦ㧘᳓㕙਄㔚ᭂ㐳㧘᡼㔚ⓨ㑆 * ጊᒻᄢቇᄢቇ㒮ℂᎿቇ⎇ⓥ⑼㧔992-8510 ጊᒻ⋵☨ᴛᏒၔ ධ྾ৼ⋡3-16㧕

Graduate school of Science and Engineering, Yamagata University, (4-3-16 Jonan, Yonezawa, Yamagata 992-8510, Japan)

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᡼㔚߇⿠ߎࠅ߿ߔ޿ⓨ㑆߇೙㒢ߐࠇࠆ㧚ߎߩ໧㗴ࠍ⸃᳿ߔ ࠆߚ߼㧘ု⋥㈩⟎ߒߚ✢ኻ౞╴㔚ᭂࠍ↪޿᳇ᵃ߇਄᣹ߔࠆ ᣇะߩ᡼㔚ⓨ㑆ࠍ㐳ߊขࠆᣇᴺ߇޽ࠆ13,14)㧚ᧄ⎇ⓥߢߪု ⋥㈩⟎ߒߚ✢ኻ౞╴㔚ᭂࠍ↪޿㧘߆ߟ㔚ᭂ㑆㓒ߦᵹߔⓨ᳇ ᵹ㊂ࠍᄢ߈ߊߒߡ㔚ᭂ㑆ߩⓨ᳇ߩ㊂ࠍ⏕଻ߔࠆߎߣߢಣ ℂല₸ߩะ਄ࠍ࿑ߞߚ㧚ᧄ⺰ᢥߢߪࡃࡉ࡝ࡦࠣߔࠆⓨ᳇ߩ ᵹ㊂ࠍᄌ߃㧘㔚ᭂ㑆ߩⓨ᳇ߩ㊂ߦኻߔࠆಣℂ․ᕈࠍ᦭ᯏ⦡ ⚛ߩ⣕⦡ᐲ߆ࠄ᣿ࠄ߆ߦߒߚ㧚ߐࠄߦ᳓ਛߢߩࡃࡉ࡝ࡦࠣ ߦട߃㧘㔚ᭂߩ৻ㇱࠍ᳓㕙਄ߦ಴ߒߚ႐ว㧘ଏ⛎ߔࠆ᳇ᵃ ߩᄢ߈ߐࠍዊߐߊߒߚ႐วߦߟ޿ߡ᷹ቯߒߚ㧚 2. ታ㛎ⵝ⟎߅ࠃ߮ᣇᴺ ࿑ߦታ㛎ⵝ⟎࿑ࠍ␜ߔ㧚Ꮐ஥߇᡼㔚࡝ࠕࠢ࠲㧘ฝ஥߇ࡄ࡞ ࠬࡄࡢ࡯⊒↢࿁〝ߢ޽ࠆ㧚᡼㔚࡝ࠕࠢ࠲ߩ᭴ᚑߪ㧘ࠕࠢ࡝࡞ ౞╴(ౝᓘ40mm㧘ᄖᒻ60mm㧘㜞ߐ425mm)ߩౝოߦធߒߡ㧘 ౞╴⁁ߦߒߚࠬ࠹ࡦ࡟ࠬߩ㊄✂(⋥ᓘ40mm㧘ో㐳300mm㧘✂ ⋡ߩᄢ߈ߐ2mm˜2mm)ࠍ౞╴㔚ᭂߣߒߡࠕࠢ࡝࡞౞╴ߩ਄ ߆ࠄ67mmߩ૏⟎ߦᝌ౉ߒ㧘ਛᔃߦࠬ࠹ࡦ࡟ࠬ✢(⋥ᓘ 0.28mm)ࠍ✢㔚ᭂߣߒߡ⸳⟎ߒߚ✢ኻ౞╴ߩหゲ㔚ᭂ᭴ᚑߢ ޽ࠆ㧚᡼㔚࡝ࠕࠢ࠲ߩࠕࠢ࡝࡞౞╴ߪ.ߩ⹜ᢱ᳓ࠍ౉ࠇߚ྾ ⷺᩇߩ᳓ᮏ(❑65mm˜ᮮ65mm˜㜞ߐ600mm)ߩਛߦᝌ౉ߒߚ㧚 㔚ᭂ㑆ߦߪࠛࠕ࡯ࡐࡦࡊ(ዦኹⓨ࿶Ꮏᬺᩣᑼળ␠ TO5P5S17㧘 ᦨᄢᵹ㊂63L/min)ߣエ⾰Ⴎࡆࡎ࡯ࠬ(ౝᓘ8mm)ࠍ↪޿ߡࠕࠢ ࡝࡞౞╴ਅ߆ࠄⓨ᳇ࠍㅍࠅㄟߺࡃࡉ࡝ࡦࠣߒߚ㧚ߘ߁ߔࠆߣ ࡝ࠕࠢ࠲ౝࠍᄙ㊂ߩⓨ᳇߇਄᣹ߔࠆߚ߼㧘⹜ᢱ᳓ߪ㔚ᭂ㑆ࠍ ൓޿ࠃߊ็߈਄߇ࠅ㧘࡝ࠕࠢ࠲ߩࠕࠢ࡝࡞౞╴ࠍ⿧߃ࠆ㧚ߎ ߩߣ߈᳓߇᳓ᮏ߆ࠄḷࠇߥ޿ࠃ߁ߦ㧘ࠕࠢ࡝࡞౞╴ߩ਄┵ߦ ߪ᳓㓸߼ࠞࡃ࡯(ౝᓘ60mm ಴ญߩ⋥ᓘ20mm)ࠍ㧘ߘߩ਄ߦ ᳓࿁෼ࠞࡃ࡯ࠍขࠅઃߌߚ㧚ⓨ᳇ߩ൓޿ߢ࡝ࠕࠢ࠲౞╴ࠍ⿧ ߃ߚ⹜ᢱ᳓ߪ᳓㓸߼ࠞࡃ࡯ߦࠃࠅ᳓ߩྃ಴ߒࠍਛᄩߦ㓸߼ࠄ ࠇࠆ㧚᳓㓸߼ࠞࡃ࡯߆ࠄྃ಴ߒߚ⹜ᢱ᳓ߪ᳓࿁෼ࠞࡃ࡯ߦᒰ ߚࠅࠕࠢ࡝࡞౞╴ߣ᳓ᮏߩ㑆ߩ㓗㑆ߦᚯߐࠇࠆ㧚ߎࠇߦࠃࠅ ⹜ᢱ᳓ߪࠕࠢ࡝࡞౞╴ߩਛ߆ࠄᄖ߳ߣᓴⅣߔࠆ㧚 ࡄ࡞ࠬࡄࡢ࡯ߩ⊒↢ߦߪࡄ࡞ࠬ࠻࡜ࡦࠬᣇᑼࠍ↪޿ߚ㧚ࡄ ࡞ࠬ࠻࡜ࡦࠬߩࠦࠕߦߪࡈࠚ࡜ࠗ࠻(TDK PC40 T75×20×15) ࠍ↪޿㧘Ꮞ✢Ყߪ1ኻ6ߣߒߚ㧚ల㔚↪ࠠࡖࡄࠪ࠲ߦߪࡄ࡞ࠬ ↪࠮࡜ࡒ࠶ࠢࠬࠦࡦ࠺ࡦࠨ(᧛↰⵾૞ᚲ N4700 ⠴࿶30kV) ࠍ↪޿ߚ㧚ࡄ࡞ࠬࠍ⊒↢ߐߖࠆࠬࠗ࠶࠴ߦߪ࠻࡝ࠟࠡࡖ࠶ࡊ ࠬࠗ࠶࠴(⥄૞)ࠍ↪޿ߚ㧚ࡄ࡞ࠬ࠻࡜ࡦࠬߢ⊒↢ߒߚࡄ࡞ࠬ 㔚࿶ߪหゲࠤ࡯ࡉ࡞ߦࠃࠅ᡼㔚࡝ࠕࠢ࠲ߩ✢㔚ᭂߦශടߐࠇ ࠆ㧚ᧄ⺰ᢥߦ߅޿ߡߩࡄ࡞ࠬࡄࡢ࡯⊒↢࿁〝ౝߩల㔚↪ࠠࡖ ࡄࠪ࠲߳ߩల㔚㔚࿶ߪ25kVߣߒ㧘ࠠࡖࡄࠪ࠲ߩኈ㊂ߪ940߹ ߚߪ5400pFߣߒߚ㧚✢㔚ᭂ߳ශടߐࠇࠆࡄ࡞ࠬ㔚࿶ߪ1/2000 ߩ㜞㔚࿶ࡊࡠ࡯ࡉ(ࡄ࡞ࠬ㔚ሶᎿᬺ BP-1240)㧘᡼㔚㔚ᵹߪ 0.1V/Aߩࡠࠧࠬࠠ࡯ࠦࠗ࡞(ࡇࠕ࠰ࡦ model-110)ࠍ↪޿ߡ㧘ࠝ ࠪࡠࠬࠦ࡯ࡊ(Tektronix TDS784D)ߢߘࠇߙࠇߩᵄᒻࠍ᷹ቯ ߒߚ㧚ಣℂߔࠆ᦭ᯏ⦡⚛ߦߪࠗࡦ࠺ࠖࠧࠞ࡞ࡒࡦࠍ↪޿㧘⹜ ᢱ᳓ߩỚᐲࠍ20mg/Lߣߒ⣕⦡ಣℂࠍⴕߞߚ㧚ࠗࡦ࠺ࠖࠧࠞ࡞ ࡒࡦߣߪ㕍⦡ߩ⦡⚛ߢ޽ࠅ㧘⣕⦡ᐲߪๆశߐࠇࠆߣṁᶧ߇㕍 ⦡ࠍ␜ߔ610nmߩㅘㆊ₸ࠍ᷹ࠆߎߣߢ⹏ଔߒߚ㧚ㅘㆊ₸ߪశ 〝㐳10mmߩ⍹⧷࠮࡞ߦ෼߼⚡ᄖนⷞಽశశᐲ⸘(ፉᵤ⵾૞ᚲ UVmini-1240)ࠍ↪޿ߡ᷹ቯߒߚ㧚 ታ㛎ߪⓨ᳇ߩᵹ㊂ࠍ9߆ࠄ63L/min߹ߢᄌ߃ߡⴕߞߚ㧚ߎߩ ߣ߈ߩ࡝ࠕࠢ࠲ౝߩ᳓ߦኻߔࠆⓨ᳇ߩ㊂ߪ᳓૏᷹ቯ↪ߩ᳓߇ ౞╴ࠍ⿧߃ߥ޿㐳޿ࠕࠢ࡝࡞౞╴ౝߩ᳓૏ߩ਄᣹߆ࠄផቯߒ ߚ㧚߹ߚࡃࡉ࡝ࡦࠣ೨ߩ㔚ᭂ┵ㇱ߇᳓㕙਄ߦ಴ࠆ㐳ߐࠍ᳓㕙 ਄㔚ᭂ㐳ߣߒ㧘࡝ࠕࠢ࠲ߩࠕࠢ࡝࡞౞╴ࠍ᳓ᮏߦᏅߒㄟ߻㐳 ߐߦࠃࠅ–1߆ࠄ20cm߹ߢᄌ߃ߡታ㛎ࠍⴕߞߚ㧚ଏ⛎ߔࠆ᳇ᵃ ࠍዊߐߊߔࠆታ㛎ߢߪႮࡆࡎ࡯ࠬߩ಴ญߦࠬࡐࡦࠫ᧚⾰㧦ࡐ ࡝࠙࡟࠲ࡦ ࠍขࠅઃߌࠆߎߣߢ᳇ᵃࠍ᜛ᢔߐߖዊߐߊߒߚ㧚 3. ታ㛎⚿ᨐ 3.1 ࡃࡉ࡝ࡦࠣߒߚ႐วߣߒߥ޿႐วߩᲧセ ᧄ㔚ᭂ᭴ᚑߢߩ᳓ਛࡄ࡞ࠬࡄࡢ࡯᡼㔚ߦ߅ߌࠆࡃࡉ࡝ࡦࠣ ߩലᨐࠍ⏕⹺ߔࠆߚ߼㧘ࠛࠕ࡯ࡐࡦࡊࠍ↪޿ߡ㔚ᭂ㑆ࠍ 63L/min ߩⓨ᳇ߢࡃࡉ࡝ࡦࠣߒߚ႐วߣ㧘ࡃࡉ࡝ࡦࠣߖߕߦ ᳓ਛ᡼㔚ࠍ⊒↢ߐߖߚ႐วߢ㧘ߘࠇߙࠇಣℂᤨ㑆ߏߣߩࠗࡦ ࠺ࠖࠧࠞ࡞ࡒࡦṁᶧߦኻߔࠆశߩㅘㆊ₸ࠍ᷹ቯߒߚ㧚ࡃࡉ࡝ ࡦࠣήߒߩ႐ว㧘᳓ߩ⺃㔚₸ߦࠃࠅ㔚ᭂ㑆ߩ㕒㔚ኈ㊂߇ᄢ߈ ߊࡄ࡞ࠬࡄࡢ࡯⊒↢࿁〝ౝߩల㔚↪ࠠࡖࡄࠪ࠲ኈ㊂߇ዊߐ޿ ߣ㔚ᭂ㑆ߦශടߐࠇࠆ㔚࿶߇㜞ߊߥࠄߥ޿㧚ߘߩߚ߼ల㔚↪ ࠠࡖࡄࠪ࠲ኈ㊂ߪࡃࡉ࡝ࡦࠣ᦭ࠅήߒ౒ߦ5400pF ߣߒߚ㧚 ߹ߚࡃࡉ࡝ࡦࠣήߒߩ႐ว㧘✢㔚ᭂߩ⋥ᓘ߇0.28mm ߢߪ᳓ ਛߢ᡼㔚߇⿠߈ߥ߆ߞߚߚ߼㧘✢㔚ᭂߦߪࡃࡉ࡝ࡦࠣ᦭ࠅή ߒ౒ߦ0.1mm ߩ㌃✢ࠍ↪޿ߚ㧚᡼㔚➅ࠅ㄰ߒᢙߪ 17.4pps㧘 ᳓㕙਄㔚ᭂ㐳ߪ–1cm ߣߒߚ㧚࿑ 2 ߣ࿑ 3 ߦࠛࠕ࡯ࡐࡦࡊߦࠃ ࠅ㔚ᭂ㑆ࠍ63L/min ߩⓨ᳇ߢࡃࡉ࡝ࡦࠣߒߚ႐วߣߒߥ߆ߞ 㪘㫀㫉 㫇㫌㫄㫇 㪚㫆㫍㪼㫉 㪮㫀㫉㪼 㪼㫃㪼㪺㫋㫉㫆㪻㪼 㪦㪛㪑㱢㪇㪅㪉㪏㫄㫄 㪤㪼㫊㪿 㪼㫃㪼㪺㫋㫉㫆㪻㪼 㪣㪑㪊㪇㪇㫄㫄 㪘㫀㫉 㪿㫆㫊㪼 㪜㫃㪼㪺㫋㫉㫆㪻㪼 㫃㪼㫅㪾㫋㪿 㫆㫅 㫎㪸㫋㪼㫉 㪚㫆㫍㪼㫉 㪽㫆㫉 㪺㫆㫃㫃㪼㪺㫋㫀㫅㪾 㫎㪸㫋㪼㫉 㪠㫅㪻㫀㪾㫆 㪺㪸㫉㫄㫀㫅㪼 㫊㫆㫃㫌㫋㫀㫆㫄䋨㪈㪣䋩 㪦㫊㪺㫀㫃㫃㫆㫊㪺㫆㫇㪼 㪫㫉㫀㪾㪾㪼㫉 㪺㫀㫉㪺㫌㫀㫋 㪭㫆㫃㫋㪸㪾㪼 㪻㫀㫍㫀㪻㪼㫉 㪚㪸㫇㪸㪺㫀㫋㫆㫉 䋨㪐㪋㪇㫇㪝䌾㪌㪋㪇㪇㫇㪝䋩 㪩㪼㫊㫀㫊㫋㫆㫉 䋨㪊㪤㱅䋩 㪭㫆㫃㫋㪸㪾㪼 㫊㫌㫇㫇㫃㫐 㪚㫌㫉㫉㪼㫅㫋 㫇㫉㫆㪹㪼 㪧㫌㫃㫊㪼 㫋㫉㪸㫅㫊㪄 㪽㫆㫉㫄㪼㫉 㪫㫉㫀㪾㪾㪼㫉 㪾㪸㫇 㫊㫎㪿㫀㪺㪿 㪧㫌㫃㫊㪼㪻 㫇㫆㫎㪼㫉 㪺㫀㫉㪺㫌㫀㫋 㪦㫌㫋㫃㪼㫋 㫆㪽 㪸㫀㫉 ࿑㧝 ࡄ࡞ࠬࡄࡢ࡯᡼㔚᳓ಣℂታ㛎ⵝ⟎

Fig.1 Experimental setup for water treatment by pulsed power discharge.

(3)

ߚ႐วߩ᡼㔚౮⌀߅ࠃ߮㔚࿶㔚ᵹᵄᒻࠍ␜ߔ㧚Ⴎࡆࡎ࡯ࠬࠍ ಴ߚ⋥ᓟߩ᳇ᵃߩᓘߪ10~20mm ⒟ᐲߢ޽ࠆ㧚࿑ 2(b)ߩࡃࡉ ࡝ࡦࠣߖߕߦ᳓ਛߢ᡼㔚ߐߖߚ႐วߪ✢㔚ᭂߩઃㄭߢ᡼㔚߇ ⿠ߎߞߡ޿ࠆߩߺߢ޽ࠆ߇㧘࿑2(a)ߩࡃࡉ࡝ࡦࠣߒߚ႐วߦ ߅޿ߡߪ㔚ᭂ㑆ߢỗߒߊ᡼㔚ߒߡ߅ࠅ㧘ࡃࡉ࡝ࡦࠣߔࠆߎߣ ߢ᡼㔚ߒ߿ߔߊߥࠅ᡼㔚ⓨ㑆߇ᐢ߇ߞߡ޿ࠆߎߣ߇ࠊ߆ࠆ㧚 ߻ߒࠈᄙᢙߩἫ⧎᡼㔚߇⊒↢ߒߡ߅ࠅ㧘5400pF ߣ޿߁ࠠࡖࡄ ࠪ࠲ኈ㊂ߪᄢ߈ߔ߉ߢ޽ࠆ㧚࿑3(b)ߩࡃࡉ࡝ࡦࠣߒߥ߆ߞߚ ႐วߩ㔚ᵹߪ⍍ᤨߦ┙ߜ਄߇ࠅ㧘㔚ᭂ㑆ߦߪਥߦᄌ૏㔚ᵹ߇ ᵹࠇ㧘᡼㔚ߦࠃࠆ㔚ᵹߪዋߒߒ߆ᵹࠇߡ޿ߥ޿㧚࿑3(a)ߩࡃ ࡉ࡝ࡦࠣߒߚ႐วߪ㔚࿶߇ශടߐࠇߚᓟ㧘㔚ᵹ߇ᵹࠇᆎ߼㧘 ߘߩᓟ㔚࿶਄᣹ߦᓥߞߡ㔚ᵹ߽Ⴧ߃ࠆ߇㧘㔚࿶ශടᓟ 150ns ઃㄭߢ㔚࿶߇ᕆỗߦᷫዋߒ㧘หᤨߦ300A ࠍ⿧߃ࠆ㔚ᵹ߇ᵹ ࠇߡ޿ࠆ㧚ߎߎߢࠬ࠻࡝࡯ࡑ᡼㔚߆ࠄἫ⧎᡼㔚߳᡼㔚߇⒖ⴕ ߒ㧘ᄙߊߩࠛࡀ࡞ࠡ࡯߇ή㚝ߦߥߞߡ޿ࠆߣ⠨߃ࠄࠇࠆ㧚࿑ 4 ߦⓨ᳇ߢࡃࡉ࡝ࡦࠣߒߚ႐วߣࡃࡉ࡝ࡦࠣߖߕ᳓ਛ᡼㔚ࠍ ⊒↢ߐߖߚ႐วߩಣℂᤨ㑆ߏߣߩᵄ㐳ߦኻߔࠆ 610nm ߩㅘ ㆊ₸ࠍ␜ߔ㧚࿑4 ࠍᢛℂߒߡ㧘࿑ 5 ߦࡃࡉ࡝ࡦࠣߒߚ႐วߣ ߒߥ޿႐วߩᵄ㐳 610nm ߦ߅ߌࠆಣℂᤨ㑆ߦ߅ߌࠆㅘㆊ₸ ߩᄌൻࠍ␜ߒߚ㧚ࡃࡉ࡝ࡦࠣߒߥ޿႐วߪ㧘࿑2(b)ߦ␜ߔ᳓ ਛࠬ࠻࡝࡯ࡑ᡼㔚ߦࠃߞߡಣℂ߇ⴕࠊࠇࠆ߇㧘15 ಽߩಣℂߢ ߪㅘㆊ₸ߪ 4%⒟ᐲߒ߆਄߇ࠄߥ߆ߞߚ㧚ߒ߆ߒࡃࡉ࡝ࡦࠣ ߒߚᣇߩㅘㆊ₸ߪ1 ಽᓟߦߪ ਄᣹ߒ㧘 ಽᓟߦߪ♖⵾᳓ߣ ߶߷หߓߦߥߞߚ㧚ߎࠇࠃࠅ63L/min ߩⓨ᳇ߢࡃࡉ࡝ࡦࠣߔ ࠆߎߣߦࠃࠅ᳓ಣℂല₸߇15 ୚⦟ߊߥࠆߎߣ߇ࠊ߆ࠆ㧚ߎࠇ ߪࡃࡉ࡝ࡦࠣߔࠆߎߣߢ᡼㔚ⓨ㑆߇ᐢ߇ߞߚߎߣߦࠃࠅ㧘⣕ ⦡ߦነਈߔࠆᵴᕈ⒳ߩ⊒↢߇ᄙߊߥߞߚߚ߼ߣ⠨߃ࠄࠇࠆ㧚 (a) ࡃࡉ࡝ࡦࠣߒߚ႐ว (b) ࡃࡉ࡝ࡦࠣߒߥ߆ߞߚ႐ว ࿑2 ࡃࡉ࡝ࡦࠣߒߚ႐วߣߒߥ߆ߞߚ႐วߩ᡼㔚౮⌀

Fig.2 Appearances of discharges in water with air bubbling and without air bubbling.

㪄㪈㪇㪇 㪄㪏㪇 㪄㪍㪇 㪄㪋㪇 㪄㪉㪇 㪇 㪉㪇 㪋㪇 㪍㪇 㪇 㪌㪇㪇 㪈㪇㪇㪇 㪈㪌㪇㪇 㪫㫀㫄㪼㩿㫅㫊㪀 㪭 㫆 㫃㫋 㪸㪾 㪼 㩿㫂 㪭 㪀 㪄㪊㪇㪇 㪄㪈㪌㪇 㪇 㪈㪌㪇 㪊㪇㪇 㪋㪌㪇 㪍㪇㪇 㪎㪌㪇 㪐㪇㪇 㪚 㫌 㫉㫉 㪼 㫅 㫋㩿 㪘 㪀 (a) ࡃࡉ࡝ࡦࠣߒߚ႐ว 㪄㪈㪇㪇 㪄㪏㪇 㪄㪍㪇 㪄㪋㪇 㪄㪉㪇 㪇 㪉㪇 㪋㪇 㪍㪇 㪇 㪌㪇㪇 㪈㪇㪇㪇 㪈㪌㪇㪇 㪫㫀㫄㪼㩿㫅㫊㪀 㪭 㫆 㫃㫋 㪸㪾 㪼 㩿㫂 㪭 㪀 㪄㪊㪇㪇 㪄㪈㪌㪇 㪇 㪈㪌㪇 㪊㪇㪇 㪋㪌㪇 㪍㪇㪇 㪎㪌㪇 㪐㪇㪇 㪚 㫌 㫉㫉 㪼 㫅 㫋㩿 㪘 㪀 (b) ࡃࡉ࡝ࡦࠣߒߥ߆ߞߚ႐ว ࿑3 ࡃࡉ࡝ࡦࠣ᦭ࠅߣήߒߩ႐วߩ㔚࿶㔚ᵹᵄᒻ

Fig. 3. Voltage and current waveforms with air bubbling and without air bubbling.

               OKP OKP OKP OKP OKP 6 T C P U O K VV C PE G  9CXGNGPIVJPO (a) ࡃࡉ࡝ࡦࠣߒߚ႐ว                OKP OKP OKP OKP OKP 6T C PU OK VV CP E G  9CXGNGPIVJPO (b) ࡃࡉ࡝ࡦࠣߒߥ߆ߞߚ႐ว ࿑ 4 ࡃࡉ࡝ࡦࠣ᦭ࠅߣήߒߩ႐วߩᵄ㐳ߦኻߔࠆㅘㆊ ₸

Fig. 4. Transmittance for wavelength with air bubbling and without air bubbling.

(4)

3.2 ⣕⦡ᐲߩࠛࠕ࡯ࡐࡦࡊᵹ㊂ଐሽᕈ ࠛࠕ࡯ࡐࡦࡊ߆ࠄㅍࠆⓨ᳇ߩᵹ㊂ࠍ9㨪63L/minߣߒ㧘ಣℂ ᤨ㑆ߦኻߔࠆ㕍⦡ߩ⣕⦡ᐲࠍ␜ߔ610nmߩㅘㆊ₸ࠍ᷹ቯߒߚ㧚 ߎߩߣ߈ߩࠠࡖࡄࠪ࠲ኈ㊂ߪ940pF㧘᡼㔚➅ࠅ㄰ߒᢙߪ100pps㧘 ᳓㕙㔚ᭂ㐳ߪ–1cmߣߒ㧘✢㔚ᭂߪࠬ࠹ࡦ࡟ࠬ⵾ߦᚯߒߚ㧚࿑ 6ߦ᳓㕙਄㔚ᭂ㐳–1cmߦ߅ߌࠆⓨ᳇ᵹ㊂ࠍᄌ߃ߚᤨߩᐔဋߩ ᳓ߦኻߔࠆⓨ᳇ߩഀวߩᄌൻࠍ␜ߔ㧚ⓨ᳇ߩᵹ㊂ࠍ9L/min߆ ࠄ63L/min߳Ⴧ߿ߔߎߣߦࠃߞߡ㧘ᐔဋߩ᳓ߦኻߔࠆⓨ᳇ߩഀ ว߇17%߆ࠄ53%߳ߣᄢ߈ߊߥࠆ㧚࿑7ߦฦⓨ᳇ᵹ㊂ߦ߅ߌࠆ ಣℂᤨ㑆ߦኻߔࠆㅘㆊ₸ߩᄌൻࠍ␜ߔ㧚ⓨ᳇ᵹ㊂ࠍᄙߊߔࠆ ߶ߤᤨ㑆ߦኻߔࠆㅘㆊ₸ߩ਄᣹ᐲ߇ᄢ߈ߊߥࠅ㧘ᧄታ㛎ߢ૶ ↪ߒߚࠛࠕ࡯ࡐࡦࡊߩᦨᄢᵹ㊂63L/min߇ᦨ߽610nmߩㅘㆊ ₸ߩ਄᣹߇ㅦߊ㧘ಣℂᤨ㑆10ಽߢ75%㧘15ಽߢ85%ߩㅘㆊ₸ ߣߥߞߚ㧚࿑6㧘7ࠃࠅⓨ᳇ߩᵹ㊂߇ᄙߊߥࠆߦᓥ޿㧘᡼㔚ⓨ 㑆߇Ⴧߒಣℂߦነਈߔࠆᵴᕈ⒳߇Ⴧ߃㧘⣕⦡ᐲ߇਄᣹ߒߚߣ ⠨߃ࠄࠇࠆ㧚 3.3 ⣕⦡ᐲߩ᳓㕙਄㔚ᭂ㐳ଐሽᕈ 䈘䉌䈮㔚ᭂ㑆䈱᳓䈮ኻ䈜䉎ⓨ᳇䈱ഀว䉕ᄙ䈒䈜䉎䈢䉄䈮䋬 ᳓㕙਄䈮䈪䉎㔚ᭂ㐳䉕–1䌾19cm䈱㑆䈪ᄌ䈋䋬ಣℂᤨ㑆䈮ኻ 䈜䉎610nm䈱ㅘㆊ₸䉕᷹ቯ䈚䈢䋮䉨䊞䊌䉲䉺ኈ㊂䈲940pF䋬➅ 䉍㄰䈚ᢙ䈲100pps䋬ⓨ᳇ᵹ㊂䈲63L/min䈫䈚䈢䋮࿑8䈮᳓㕙਄ 㔚ᭂ㐳䉕–1cm䈎䉌19䌣䌭䈮ᄌ䈋䈢ᤨ䈱ᐔဋ䈱㔚ᭂ㑆䈱᳓䈮ኻ           6 TC P U O K V VC P E G  6TGCVOGPV VKOGOKP .OKP YKVJ DWDDNKPI .OKP YKVJQWV DWDDNKPI &KUVKNNGF YCVGT

(Capacitance; 5400pF, Repetition rate; 17.4pps)

࿑ 5 ࡃࡉ࡝ࡦࠣߒߚ႐วߣߒߥ߆ߞߚ႐วߩ᡼㔚ಣℂ

ᤨ㑆ߦ߅ߌࠆᵄ㐳610nm ߩㅘㆊ₸ߩᄌൻ

Fig.5 Time variations of the transmittance of the wavelength of 610nm for the treatment time by discharge in water with air bubbling and without air bubbling.

              4C V KQ Q H C KT K P Y C VG T  #KT HNQY TCVG .OKP ࿑6 ⓨ᳇ᵹ㊂ߦኻߔࠆ࡝ࠕࠢ࠲ౝߩ᳓ߦኻߔࠆⓨ᳇ߩഀว

Fig.6 The ratio of air in water for air flow rate.

          6T CP U OK V VC P E G  6TGCVOGPV VKOGOKP .OKP .OKP .OKP .OKP .OKP .OKP &KUVKNNGF YCVGT

(Capacitance; 940pF, Repetition rate; 100pps)

7 ࠛࠕ࡯ࡐࡦࡊߩᵹ㊂ࠍᄌ߃ߚߣ߈ߩಣℂᤨ㑆ߦኻ

ߔࠆᵄ㐳610nm ߩㅘㆊ₸ߩᄌൻ

Fig.7 Variations of the transmittance of the wavelength of 610nm for the treatment time at several flow rate of air.. .            4 C V K Q Q H C K T  K P YC V G T  6JGNGPIVJQHVJGGNGEVTQFGCDQXGVJGYCVGTEO ࿑8 ᳓㕙਄㔚ᭂ㐳ߦኻߔࠆ࡝ࠕࠢ࠲ౝߩ᳓ߦኻߔࠆⓨ᳇ߩ ഀว

Fig.8 The ratio of air in water for the length of electrode above the water.

(5)

- 5 - 䈜䉎ⓨ᳇䈱ഀว䈱ᄌൻ䉕␜䈜䋮᳓㕙਄㔚ᭂ㐳䈏–1cm䈎䉌 12.5䌣䌭䉁䈪䈲㐳䈒䈭䉎䈮ᓥ䈦䈩䋬ᐔဋ䈱᳓䈮ኻ䈜䉎ⓨ᳇䈱ഀ ว䈲53%䈎䉌65%䈻䈫ᄢ䈐䈒䈭䈦䈢䋮12.5cm䉋䉍㐳䈇႐ว䈲ᐔ ဋ䈱᳓䈮ኻ䈜䉎ⓨ᳇䈱ഀว䈲ᄌൻ䈏䈭䈒䈭䈦䈢䋮䈖䉏䈲䊋䊑䊥 䊮䉫䈜䉎૏⟎䈏᳓㕙䈮ㄭ䈒䈭䉍䋬䊋䊑䊥䊮䉫䈮䉋䈦䈩᳓䈱็䈐 ਄䈏䉎൓䈇䈏ᒙ䈒䈭䈦䈢䈖䈫䈪᳓䈱೔㆐㜞䈘䈏ૐ䈒䈭䉍ⓨ᳇䈱 ഀว䈏Ⴧ䈋䈭䈎䈦䈢䈢䉄䈫⠨䈋䉌䉏䉎䋮࿑9䈮–1䌾19cm䈱᳓㕙 ਄㔚ᭂ㐳䈮䈍䈔䉎ಣℂᤨ㑆䈮ኻ䈜䉎610nm䈱ㅘㆊ₸䈱ᄌൻ 䉕␜䈜䋮᳓㕙਄㔚ᭂ㐳–1cm䈎䉌12.5cm䉁䈪䈲᳓㕙਄㔚ᭂ㐳 䉕㐳䈒䈜䉎䈫610nm䈱ㅘㆊ₸䈲䉋䈒䈭䉍䋬12.5cm䈪䈲ಣℂᤨ㑆 10ಽ䈪90%䈮㆐䈚䈢䋮䈖䉏䈲᳓㕙਄䈮㔚ᭂ䉕৻ㇱ಴䈜䈖䈫䈪䋬 㔚ᭂ㑆䈱᳓䈮ኻ䈜䉎ⓨ᳇䈱ഀว䈏Ⴧ䈋䈢䈢䉄䈪䈅䉎䋮䈚䈎䈚䋬 12.5cm䉋䉍᳓㕙਄㔚ᭂ㐳䉕㐳䈒䈚䈩䈇䈒䈫610nm䈱ㅘㆊ₸䈲ૐ ਅ䈚䈢䋮䈖䉏䈲᳓㕙਄㔚ᭂ㐳䉕㐳䈒䈚䈩䉅㔚ᭂ㑆䈱᳓䈮ኻ䈜䉎 ⓨ᳇䈱ഀว䈏ᄌ䉒䉌䈭䈇䈖䈫䈮ട䈋䋬᳓䈱ᓴⅣ䈱䈢䉄䈮⿧䈋 䈭䈔䉏䈳䈭䉌䈭䈇䊥䉝䉪䉺䈱䉝䉪䊥䊦౞╴䈱᳓㕙䈎䉌䈱㜞䈘䈏 㜞䈒䈭䈦䈩䈚䉁䈦䈢䈖䈫䈫䋬䊋䊑䊥䊮䉫䈜䉎૏⟎䉅᳓㕙䈮ㄭ䈒䈭䈦 䈩䈚䉁䈉䈢䉄䊋䊑䊥䊮䉫䈮䉋䈦䈩็䈐਄䈏䉎᳓䈱㜞䈘䈏ૐ䈒䈭䈦 䈩䈚䉁䈦䈢䈖䈫䈪䋬᳓䈏䉝䉪䊥䊦౞╴䉕⿧䈋䉌䉏䈭䈇䈫䈇䈉䈖䈫䈏 ⿠䈖䉍䋬᳓䈏ᓴⅣ䈚䈨䉌䈒䈭䈦䈩䈚䉁䈦䈢䈖䈫䈮䉋䉎䈫⠨䈋䉌䉏 䉎䋮 3.4 ࠕࠢ࡝࡞౞╴ਅㇱࠍ㐳ߊߒߚ႐วߩ⣕⦡ᐲ ᳓㕙਄㔚ᭂ㐳ࠍ㐳ߊߒߚ႐วߢ߽็߈਄߇ࠆ᳓ߩ㜞ߐࠍᄌ ߃ߕ㧘߆ߟ᳓ߩᓴⅣ߇⿠ߎࠆࠃ߁ߦߔࠆߣಣℂല₸ߩะ਄߇ ᦼᓙߢ߈ࠆ㧚ߘߎߢ᳓㕙਄㔚ᭂ㐳ࠍᄌ߃ߚ႐วߦ߅޿ߡ߽ࠕ ࠢ࡝࡞౞╴ߩਅㇱࠍ᳓㕙਄㔚ᭂ㐳–1cmߩ႐วߣหߓࠃ߁ߦ 㪘㫀㫉 㫇㫌㫄㫇 㪫㫆㩷㫋㪿㪼㩷㫇㫌㫃㫊㪼㪻㩷 㫇㫆㫎㪼㫉㩷㪺㫀㫉㪺㫌㫀㫋 㪘㫀㫉 㫇㫌㫄㫇 㪫㫆㩷㫋㪿㪼㩷㫇㫌㫃㫊㪼㪻㩷 㫇㫆㫎㪼㫉㩷㪺㫀㫉㪺㫌㫀㫋 (a) ⍴޿ਅㇱ (b) 㐳޿ਅㇱ ࿑10 ࠕࠢ࡝࡞౞╴ਅㇱ߇⍴޿࡝ࠕࠢ࠲ߣ㐳޿࡝ࠕࠢ࠲

Fig.10 The reactors with the short and long underpart of the acrylic cylinder.

           6 TC P UO KV V CP E G  6JGNGPIVJQHVJG GNGEVTQFGCDQXGVJGYCVGTEO &KUVKNNGFYCVGT OKP OKP 6TGCVOGPVVKOGD[FKUEJCTIG ࿑ 12 ࡝ࠕࠢ࠲ਅㇱࠍ㐳ߊߒߚ႐วߩ᳓㕙਄㔚ᭂ㐳ߦኻߔ ࠆᵄ㐳610nm ߩㅘㆊ₸

Fig.12 Transmittance of the wavelength of 610nm for the length of the electrode above the water of the reactor with the long underpart of the acrylic cylinder.

           4 C V K Q Q H C K T  KP  Y C VG T  6JGNGPIVJQHVJGGNGEVTQFGCDQXGVJGYCVGTEO ࿑ 11 ࡝ࠕࠢ࠲ਅㇱࠍ㐳ߊߒߚ႐วߩ᳓㕙਄㔚ᭂ㐳ߦኻߔ ࠆ࡝ࠕࠢ࠲ౝߩ᳓ߦኻߔࠆⓨ᳇ߩഀว

Fig.11 The ratio of air in water for the length of electrode above the water of the reactor with the long underpart of the acrylic cylinder.            6T C PU O KV V CP E G  6JGNGPIVJQHVJGGNGEVTQFGQPVJGYCVGTEO &KUVKNNGFYCVGT OKP OKP 6TGCVOGPVVKOGD[ FKUEJCTIG ࿑9 ᳓㕙਄㔚ᭂ㐳ߦኻߔࠆᵄ㐳 610nm ߩㅘㆊ₸

Fig.9 Transmittance of the wavelength of 610nm for the length of the electrode above the water.

(6)

- 6 - ᳓ᮏߩᐩ߹ߢ㐳ߊߒߡ㧘ࡃࡉ࡝ࡦࠣߦࠃߞߡ็߈਄߇ࠆ᳓ߩ 㜞ߐ߇ᄌࠊࠄߥ޿ࠃ߁ߦߒߚ㧚ࠠࡖࡄࠪ࠲ኈ㊂ߪ940pF㧘➅ ࠅ㄰ߒᢙߪ100pps㧘ⓨ᳇ᵹ㊂ߪ63L/minߣߒߚ㧚࿑10ߦࠕࠢ࡝ ࡞౞╴ࠍ㐳ߊߔࠆ೨ᓟߩ࡝ࠕࠢ࠲ࠍ␜ߔ㧚࿑11ߦߎߩߣ߈ߩ ᳓㕙਄㔚ᭂ㐳ߣᐔဋߩ㔚ᭂ㑆ߩ᳓ߦኻߔࠆⓨ᳇ߩഀวࠍ␜ߔ㧚 ᳓㕙਄㔚ᭂ㐳߇–1cm߆ࠄ19㨏㨙ߦ㐳ߊߥࠆߦᓥߞߡ㧘ᐔဋߩ ᳓ߦኻߔࠆⓨ᳇ߩഀว߇53%߆ࠄ73%߳ߣᄢ߈ߊߥߞߚ㧚࿑ 12ߦࠕࠢ࡝࡞౞╴ਅㇱࠍ᳓ᮏߩᐩ߹ߢિ߫ߒߚߣ߈ߩ᳓㕙਄ 㔚ᭂ㐳ߦኻߔࠆ5ಽ߅ࠃ߮10ಽ᡼㔚ᓟߩᵄ㐳610nmߩㅘㆊ₸ ࠍ␜ߔ㧚ࠕࠢ࡝࡞౞╴ਅㇱࠍ᳓ᮏߩᐩ߹ߢિ߫ߒߚߎߣߦࠃ ࠅ᳓㕙਄㔚ᭂ㐳߇19cm߹ߢ610nmߩㅘㆊ₸ߪ਄߇ࠆࠃ߁ߦ ߥࠅ㧘᳓㕙਄㔚ᭂ㐳19cmߩߣ߈10ಽߢ92%ߦ㆐ߒߚ㧚ߒ߆ߒ 19cmࠃࠅ߽㐳ߊߔࠆߣㅘㆊ₸ߪਅ߇ߞߚ㧚࡝ࠕࠢ࠲ߩࠕࠢ࡝ ࡞౞╴ࠍ᳓ᮏߩᐩ߹ߢ㐳ߊߒߡ߽63L/minߢ᳓ߩᓴⅣ߇໧㗴 ߥߊ⿠ߎࠆ᳓㕙਄㔚ᭂߩ㜞ߐߪ19cm߹ߢߢ޽ࠆߣ⠨߃ࠄࠇ ࠆ㧚 3.5 ⓨ᳇ࠍ᜛ᢔߐߖߚ႐วߩ⣕⦡ᐲ ࡝ࠕࠢ࠲ߦଏ⛎ߔࠆ᳇ᵃߩᄢ߈ߐߦࠃࠆಣℂല₸ࠍ⺞ ߴࠆߚ߼Ⴎࡆࡎ࡯ࠬߩⓨ᳇ߩ಴ญߦࠬࡐࡦࠫ᧚⾰㧦ࡐ࡝ ࠙࡟࠲ࡦ ࠍขࠅઃߌߡⓨ᳇ࠍ᜛ᢔߐߖߚ႐วߩಣℂᤨ㑆 ߦኻߔࠆ610nmߩㅘㆊ₸ࠍ᷹ቯߒߚ㧚ߎߩߣ߈ߩ᳓㕙਄㔚 ᭂ㐳ߪ12.5cm㧘࡝ࠕࠢ࠲ߩࠕࠢ࡝࡞౞╴ߩ㐳ߐߪਅㇱࠍ㐳 ߊߒߡ޿ߥ޿425mmߣߒ㧘ࠠࡖࡄࠪ࠲ኈ㊂ߪ940pF㧘᡼㔚 ➅ࠅ㄰ߒᢙߪ100pps㧘ⓨ᳇ᵹ㊂ߪ63L/minߣߒߚ㧚᳇ᵃߩ ᓘߪࠬࡐࡦࠫขࠅઃߌ೨߇10㨪20mm㧘ࠬࡐࡦࠫࠍขࠅઃ ߌᓟ߇3㨪5mmߣߥߞߚ㧚࿑13ߦಣℂᤨ㑆ߦ߅ߌࠆㅘㆊ₸ ߩᄌൻࠍ␜ߔ㧚ࠬࡐࡦࠫࠍขࠅઃߌࠆߎߣߦࠃࠅㅘㆊ₸߇ 2~3%ߢߪ޽ࠆ߇਄᣹ߒߚ㧚ߎࠇߪࠬࡐࡦࠫࠍขࠅઃߌࠆ ߎߣߦࠃࠅ᳇ᵃ߇᜛ᢔߒߚߎߣߢⓨ᳇ߣṁᶧߣߩធ⸅⴫ 㕙Ⓧ߇ᄢ߈ߊߥࠅ㧘᡼㔚ߦࠃࠅ⊒↢ߒߚᵴᕈ⒳ߣࠗࡦ࠺ࠖ ࠧࠞ࡞ࡒࡦߣߩ෻ᔕ㕙Ⓧ߇ᐢߊߥߞߚߚ߼ߢ޽ࠆߣ⠨߃ ࠄࠇࠆ㧚 4. ޽ߣ߇߈ ᳓ਛࡄ࡞ࠬࡄࡢ࡯᡼㔚᳓ಣℂߩ᡼㔚㔚ᭂ㑆ࠍⓨ᳇ߢࡃࡉ࡝ ࡦࠣߔࠆᣇᴺߦ߅޿ߡ㧘ု⋥㈩⟎ߒߚ✢ኻ౞╴㔚ᭂߦᄢᵹ㊂ ߩⓨ᳇ߦࠃࠆࡃࡉ࡝ࡦࠣࠍⴕ߁ߎߣߢ㔚ᭂ㑆ߦሽ࿷ߔࠆⓨ᳇ ߩ㊂ࠍჇ߿ߒಣℂ₸ߩะ਄ࠍ࿑ߞߚ㧚 ࡃࡉ࡝ࡦࠣߔࠆߎߣߦࠃߞߡࠗࡦ࠺ࠖࠧࠞ࡞ࡒࡦߩ㕍⦡ߩ ⣕⦡ㅦᐲߪࡃࡉ࡝ࡦࠣߒߥ޿႐วࠃࠅ୚એ਄ㅦߊߥߞߚ㧚 ߎࠇߪ᳓ࠃࠅⓨ᳇ߩ⛘✼⠴ജ߇ዊߐ޿ߚ߼㧘ࡃࡉ࡝ࡦࠣߔࠆ ߎߣߢ᡼㔚߇⊒↢ߒ߿ߔߊߥߞߡࠬ࠻࡝࡯ࡑ߇㐳ߊિ߮㧘ಣ ℂߦ૶ࠊࠇࠆᵴᕈ⒳ߩ⊒↢㊂߇Ⴧ߃ߚߚ߼ߣ⠨߃ࠄࠇࠆ㧚ߘ ߒߡ᡼㔚ⓨ㑆ߦࡃࡉ࡝ࡦࠣߔࠆⓨ᳇ᵹ㊂߇ᄙ޿߶ߤ㧘᳓㕙਄ 㔚ᭂ㐳߇㐳޿߶ߤ㔚ᭂ㑆ߦሽ࿷ߔࠆⓨ᳇ߩഀวࠍᄢ߈ߊߥࠅ ⣕⦡ᐲ߇㜞ߊߥߞߚ㧚ߚߛߒ᳓㕙਄㔚ᭂ㐳߇㐳ߊߥࠅߔ߉ࠆ ߣ᳓ߩᓴⅣ߇ᖡߊߥࠅ⣕⦡ᐲߪ਄߇ࠄߥߊߥߞߚ㧚߹ߚ㧘ࡃ ࡉ࡝ࡦࠣߔࠆ᳇ᵃߩᄢ߈ߐࠍዊߐߊߔࠆߎߣߦࠃߞߡ⣕⦡₸ ߇㜞ߊߥߞߚ㧚ߎࠇߪṁᶧߣᵴᕈ⒳ߩ෻ᔕߩߚ߼ߩធ⸅⴫㕙 Ⓧ߇Ⴧ߃ߚߚ߼ߣ⠨߃ࠄࠇࠆ㧚ࡄ࡞ࠬࡄࡢ࡯᡼㔚ߦࠃࠆ᳓ಣ ℂߦ߅޿ߡ㧘㜞ല₸ߢಣℂࠍⴕ߁ߚ߼ߦߪ㧘ᄢ߈ߥ᡼㔚ⓨ㑆 ߩ⏕଻ߣᵴᕈ⒳ߩ฽߹ࠇࠆⓨ㑆ߣṁᶧߣߩ෻ᔕ㕙ⓍࠍჇ߿ߔ ߎߣ߇㊀ⷐߢ޽ࠆ㧚 ෳ⠨ᢥ₂ 1) G. Felleberg ⪺࡮ศ↰ᵏᒾ࡮ᴰసᐘ࡮ᄢᎹේᱞ࡮ട⮮⟤ᕺ ሶ࡮᧖ᶆ౏ᤘ࡮⷏ጊ⡡ሶ࡮⑔ፉᐽᱜ࡮⮮ᴧᒄ࡮෶㊀⧷৻࡮ ᧄጊᱜᄦ ⸶㧦ੱ㘃ᧂ᧪ߩߚ߼ߩⅣႺൻቇ, pp.81-116, ਣ ༀᩣᑼળ␠ (2002) 2) ࠲ࠢࡑⅣႺᛛⴚ⎇ⓥળ㧦᳓ಣℂ⛗ߣ߈ၮᧄ↪⺆㧘pp.70-71㧘 ࠝ࡯ࡓ␠(2000) 3) ㊁᧛ṑ↵㧦᳓⾰ᳪỘߣ㜞ᐲಣℂᛛⴚ-3 ᰴಣℂᛛⴚߣߘߩ ᔕ↪㧘pp.15-25㧘ൻቇᎿᬺ␠(1986) 4) ’⼾㧦᳓⾰ᳪỘߣ㜞ᐲಣℂᛛⴚ-3 ᰴಣℂᛛⴚߣߘߩᔕ↪㧘 pp.162-195㧘ൻቇᎿᬺ␠(1986) 5) દ⮮ᵏ㇢㧦ࠝ࠱ࡦߩਇᕁ⼏㧘⻠⺣␠(2000) 6) ૒⮮ᱜਯ㧦ᔕ↪‛ℂ㧘69 (2000) 301 7) ᑝጟ㆐਽㧘ኹర㓶੺㧘ൎᧁᷕ㧘⑺ጊ⑲ౖ㧦㔚᳇ቇળ⎇ⓥ ળ⾗ᢱED-01-34 (2001) 93

8) B. Sun, M. Sato, J.S. Clements: Jounal of Electrostatics, 39 (1997) 189

9) ࠕࡦ࠻ ࠻࡝ ࠬࠡࠕ࡞࠻㧘૒⮮ᱜਯ㧦㕒㔚᳇ቇળ⻠Ṷ⺰ ᢥ㓸'02 (2002) 235

10) Jie Li, Masayuki Sato, Takayuki Ohshima: Thin Solid Films:

515 (2007) 4283

11) ⷗Ꮢ⍮ᤘ㧘ᨋା຦㧘ⁿේື㧘૒⮮ਃ㇢㧘ጊㇱ㐳౓ⴡ㧦㔚

᳇ቇળ⺰ᢥ⹹A, Vol.121 (2001) 448

12) M. Kurahashi, S. Katsura, A. Mizuno: Journal of Electrostatics,

42 (1997) 93

13) S. Espie, L. Marsili, S J. MacGregor, J G. Anderson: Proc. 13th IEEE Intern. Pulsed Power Conf. (2001) 616

14) T. Namihara, D. Wang, T. Takashima, S. Katsuki, H. Akiyama: Proc. 14-th IEEE Intern. Pulsed Power Conf. (2003) 1266

          6 T C P U O K V VC P E G  6TGCVOGPVVKOG 9KVJURQPIG 9KVJQWVURQPIG &KUVKNNGF YCVGT ࿑13 ⓨ᳇ࠍ᜛ᢔߐߖߚಣℂߦ߅ߌࠆᵄ㐳 610nm ߩㅘㆊ₸ ߩᤨ㑆ᄌൻ

Fig.13 Time variations of the transmittance of the wavelength of 610 nm for the treatment diffusing air by the sponge.

Fig. 4. Transmittance for wavelength with air bubbling and without air bubbling.

参照

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