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歩行時の人体帯電電位変化に関する等価回路的検討

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ᱠⴕᤨߩੱ૕Ꮺ㔚㔚૏ᄌൻߦ㑐ߔࠆ╬ଔ࿁〝⊛ᬌ⸛

⪤ ᧄ ቟ ᤘ*

,1

㧘᧻ ੗

ḩ**㧘᧛ 㦮 ᙗ 㓶***

㧔2005 ᐕ 5 ᦬ 6 ᣣฃઃ; 2005 ᐕ 8 ᦬ 30 ᣣฃℂ㧕

A Study on the Variance of Electrostatic Potential of a Walking

Human Body with an Equivalent Circuit

Yasuaki HAGIMOTO*

,1

, Mitsuru MATSUI** and Norio MURASAKI***

(Received May 6, 2005; Accepted August 30, 2005)

A series of experiments using different types of footwear showed that an electrostatic potential of a human body

sometimes changes polarity during walking and after stopping. Another measurement of the voltage decay of a

stationary human body showed that the decay curve differs in accordance with the polarity of the initial voltage. An

equivalent circuit was developed on the basis of these experimental results. Numerical calculations of the human body

voltage were performed for various values of the resistors in the circuit. The calculation results showed good

agreement with features observed in actual experimental results. These results are discussed with reference to each

other.

1. ߪߓ߼ߦ ᱠⴕᤨߦ↢ߓࠆੱ૕ߩ㕒㔚᳇Ꮺ㔚ߪ㧘Ἣἴ῜⊒੐᡿ߩේ࿃ ߣߥࠆߛߌߢߥߊ㧘㔚ሶ࠺ࡃࠗࠬߩ ESD ኻ╷ߦ߅޿ߡ߽㊀ᄢ ߥ໧㗴ߢ޽ࠆ㧚ੱ૕ߩᏪ㔚ߪ㧘ጁ‛㧘ᐥߥߤߩ᭽ޘߥⅣႺ᧦ ઙߦࠃߞߡᓇ㗀ߐࠇࠆߚ߼1㧕㧘․⇣ߥ⃻⽎߇ߺࠄࠇࠆߎߣ߇ ޽ࠆ㧚଀߃߫㧘ࠞ࡯ࡍ࠶࠻਄ߩᱠⴕਛ߿ᱠⴕ஗ᱛᓟߦੱ૕㔚 ૏ߩ╓ภ߇ᄌࠊࠆߣ޿߁⃻⽎߇⍮ࠄࠇߡ޿ࠆ2-5㧕㧚ߣߎࠈ߇㧘 ੱ૕ߩᏪ㔚ߦ߅ߌࠆᐥ߿ጁ‛ߩᓇ㗀ߦߟ޿ߡᬌ⸛ߒߚ⎇ⓥ ႎ๔ߪᄙ޿߇6-9)㧘ੱ૕㔚૏ߩ╓ว߇ᄌࠊࠆ⃻⽎ߦߟ޿ߡߩ╬ ଔ࿁〝⊛ߥᬌ⸛ߪⴕࠊࠇߡ޿ߥ޿㧚 ᧄ⎇ⓥߢߪታ㛎ቶߩᐥࠍᱠⴕߔࠆታ㛎ߦ߅޿ߡ㧘ᱠⴕਛ޽ ࠆ޿ߪᱠⴕ஗ᱛᓟߩੱ૕㔚૏ߩᄌൻㆊ⒟ߢ㔚૏ߩ╓ภ߇ᄌ ࠊࠆ⃻⽎߇⹺߼ࠄࠇߚ㧚ߘߎߢ㧘ጁ‛ߩ⒳㘃ࠍᄌ߃ߚᱠⴕታ 㛎ࠍⴕ޿㧘ੱ૕㔚૏ߩᄌൻߦߤߩࠃ߁ߥ㆑޿߇↢ߓࠆ߆⺞ߴ ࠆߣߣ߽ߦ㧘Ꮺ㔚㔚૏ߩ╓ภ߇ᄌࠊࠆේ࿃ߦߟ޿ߡᬌ⸛ߒߚ㧚 ߐࠄߦ㧘ߎߩ⚿ᨐߦၮߠ޿ߡᱠⴕᤨߩੱ૕ࠍࡕ࠺࡞ൻߒߚ࿁ 〝ࠍ૞ᚑߒ㧘⸘▚ߦࠃࠆࠪࡒࡘ࡟࡯࡚ࠪࡦࠍⴕߞߚ㧚ߘߩ⚿ ᨐ㧘⸘▚਄ߢ߽Ꮺ㔚㔚૏ߩ╓ภ߇ᄌࠊࠆߎߣࠍ␜ߒߚ㧚߹ߚ ࿁〝ቯᢙࠍᄌ߃ߚ႐วߦߟ޿ߡ㧘Ꮺ㔚ࡕ࠺࡞ߦࠃࠆ⸘▚⚿ᨐ ߣታ㛎࠺࡯࠲ߣߩᲧセࠍⴕߞߚ㧚 2. ᱠⴕᏪ㔚ߩታ㛎 2.1 ታ㛎ᣇᴺ ᱠⴕਛ߅ࠃ߮ᱠⴕ஗ᱛᓟߩੱ૕㔚૏ߩ᷹ቯߪ㧘ࠬ࠻ࡠ࡯࡞ ᴺߦḰߓߡⴕߞߚ10㧕㧚᷹ቯེߪ㧘࿑ 1 ߦ␜ߔ౞᧼㔚ᭂߦኻะ ߐߖߚ࿁ォ࠮ࠢ࠲ᒻ㔚⇇⸘ߢ޽ࠆ㧚ߎࠇߣኻะߐߖߚ౞᧼㔚 ᭂߦ࡝࡯࠼✢ࠍធ⛯ߒ㧘ⵍ㛎⠪߇ߘߩ┵ࠍ⚛ᚻߢីߞߚ㧚ߎ ߩ᷹ቯ♽ߩ㕒㔚ኈ㊂ߪ⚂ 30pF ߢ޽ࠆ㧚 ࠠ࡯ࡢ࡯࠼㧦ੱ૕Ꮺ㔚㧘ᱠⴕᏪ㔚㧘╬ଔ࿁〝 * ⑼ቇ⼊ኤ⎇ⓥᚲ㧔277-0882 ජ⪲⋵ᨰᏒᨰߩ⪲ 6-3-1㧕 National Research Institute of Police Science, 6-3-1 Kashiwanoha, Kashiwa 277-0882, Japan

** Zao ES Lab.㧔989-0916 ችၔ⋵⬿₺↸㆙ಿ↰᷷ᴰ਄ࡁේ 3-320㧕

Zao Electrostatic System Laboratory, 3-320 Uenohara, Togattaonsen, Zaomachi, Miyagi 989-0916, Japan

***᧲੩ㄘᎿᄢቇฬ⹷ᢎ᝼㧔187-0045 ᧲੩ㇺዊᐔᏒቇ࿦⷏↸ 2-25-7㧕

Emeritus Prof., Tokyo University of Agriculture and Technology, 2-25-7 Gakuen-nishimachi, Kodaira Tokyo 187-0045, Japan

1 [email protected]

࿑ 1 ᷹ቯⵝ⟎

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ታ㛎ߪ,ቶ᷷⚂ 24͠㧘Ḩᐲ 35㨪40㧑ߩቶౝߢⴕߞߚ㧚ᱠⴕ ߒߚ႐ᚲߪ㧘ታ㛎ቶౝߩᐥ㧔Ⴎൻࡆ࠾࡞♽ࠪ࡯࠻㧕ߢ޽ࠆ㧚 ᱠⴕ▸࿐ߪ⚂ 1.5㨙˜3m ⒟ᐲ㧘ᱠⴕ⚻〝ߪ 8 ߩሼᒻߢ޽ࠆ㧚 ᱠⴕ▸࿐ߦ㒢⇇߇޽ࠆ߇㧘಴᧪ࠆ㒢ࠅᣂߒ޿ᐥ㕙ࠍᱠⴕߒߚ㧚 ታ㛎ߦ૶↪ߒߚጁ‛ߪ㧘⴫ 1 ߦ␜ߔ 14 ⒳㘃ߢ޽ࠅ㧘޿ߕ ࠇ߽ᣂຠߦㄭ޿⁁ᘒߢ޽ࠆ㧚ታ㛎ᤨߣหߓ᷷Ḩᐲߩቶౝߦ 1 ㅳ㑆એ਄᡼⟎ߒߡ߆ࠄታ㛎ߦ૶↪ߒߚ㧚⌕⴩ߪ㧘✎߹ߚߪ ✎࡮ࡐ࡝ࠛࠬ࠹࡞ᷙ⚜ߩ⴩㘃ߢ޽ࠆ㧚ⵍ㛎⠪ߪり㐳⚂ 170cm㧘 ૕㊀⚂ 60kg ߩ↵ᕈߢ޽ࠆ㧚⴫ 1 ߦ␜ߔ㕒㔚ኈ㊂ߦߪ㧘᷹ቯ ♽ߩ㕒㔚ኈ㊂߇฽߹ࠇߡ޿ࠆ㧚ᐥߣጁ‛ߪ㧘1 ࿁ߩ᷹ቯ߇⚳ ੌߔࠆߏߣߦ᫔⁁ߩ㔚࿶ශടᑼ㒰㔚ེߢ㒰㔚ߒ㧘ߐࠄߦࠕ࡞ ࠦ࡯࡞ࠍᨴߺㄟ߹ߖߚ✎Ꮣߢ⴫㕙ࠍ᜞ߞߚ㧚 ⴫ 1 ታ㛎ߦ૶↪ߒߚጁ‛ Table 1 Footwear used for experiments.

No. ጁ ‛ 㕒㔚ኈ㊂ ާpFި 1 ‐⊹㕟⵾⚩჻㕦㧔⊹ᐩ㧕 200 2 วᚑ⊹㕟⵾⚩჻㕦㧔⎬⾰ࠧࡓᐩ㧕 200 3 ‐⊹㕟⵾⚩჻㕦㧔エ⾰ࠧࡓᐩ㧕 160 4 ㆇേ㕦㧔޽߼⦡ࠧࡓᐩ㧕 180 5 ࠧࡓ㐳㕦 200 6 ࠬ࡝࠶ࡄ㧔⊒ᵃ EVA ᐩ㧕 170 7 ࠬ࡝࠶ࡄ㧔Ⴎൻࡆ࠾࡞࡟ࠩ࡯⾍ࠅᐩ㧕 170 8 ࠨࡦ࠳࡞㧔⊒ᵃႮൻࡆ࠾࡞৻૕ဳ㧕 180 9 ࠨࡦ࠳࡞㧔⊒ᵃวᚑࠧࡓᐩ㧕 130 10 ࡆ࡯࠴ࠨࡦ࠳࡞㧔⊒ᵃ EVA ৻૕ဳ㧕 130 11 㘑ํ႐↪ࡉ࡯࠷㧔ᧄ૕ߪ EVA,ᐩߪห⊒ᵃ㧕 150 12 㘑ํ႐↪ࡉ࡯࡞ߩ਄ߦߐࠄߦ No. 6 ࠍጁߊ 140 13 㘑ํ႐↪ࡉ࡯࠷ߩᐩ᧚ࠍขࠅ㒰ߊ 220 14 㘑ํ႐↪ࡉ࡯࠷ߩᐩߦ No. 6 ߩᐩ᧚ࠍ⾍ࠆ 170 㧔ᵈ㧕EVA㧦ࠛ࠴࡟ࡦ ㈶㉄ࡆ࠾࡞౒㊀ว᮸⢽ 2.2 ᱠⴕᤨ߅ࠃ߮ᱠⴕ஗ᱛᓟߩੱ૕㔚૏ᄌൻ ᱠⴕߦ઻߁ੱ૕㔚૏ߩ᷹ቯ⚿ᨐࠍ࿑ 2(a)㨪(n)ߦ␜ߔ㧚࿑ 2 ਛߦߪ㧘ᱠⴕ஗ᱛᓟߩ✭๺ᦛ✢߆ࠄ✭๺ᤨ㑆ߩ᭎⇛୯ࠍ⺒ߺ ขࠅ㧘ߎࠇࠍ⴫ 1 ߩ㕒㔚ኈ㊂ߢഀߞߡ᳞߼ߚᛶ᛫୯ R ࠍ૬⸥ ߒߚ㧚 ࿑ 2 ߩੱ૕㔚૏ߩᄌൻߪ㧘ᄢ߈ߊ 3 ߟߦಽߌࠄࠇࠆ㧚╙ 1 ߪ㧘ᱠⴕਛߦੱ૕㔚૏߇਄᣹ߒ㧘஗ᱛᓟߪᷫ⴮ߔࠆㅢᏱߩᄌ ൻߢ޽ࠆ㧚╙ 2 ߪ㧘ᱠⴕ஗ᱛᓟߦੱ૕㔚૏ߩ╓ภ߇ᄌࠊࠆ࿑ 2(d)㧘(f)߅ࠃ߮(n)ߩࠃ߁ߥᄌൻߢ޽ࠆ㧚╙ 3 ߪ㧘ᱠⴕਛߩੱ ૕㔚૏߇ 0V ઃㄭߢផ⒖ߒ㧘ᱠⴕ஗ᱛᓟߦ⛘ኻ୯߇ᄢ߈ߊߥ ࠆ࿑ 2(i)߅ࠃ߮(k)ߩࠃ߁ߥᄌൻߢ޽ࠆ㧚 ᱠⴕ஗ᱛᓟߦੱ૕㔚૏ߩ╓ภ߇ᄌࠊߞߚ╙ 2 ߩ႐วߪ㧘࿑ 3(b)㧘(c)ߩࠃ߁ߦA ߣ B ߩ 2 ߟᦛ✢ߢ⴫ࠊߐࠇࠆᄌൻ߇㊀⇥ ߒߚ⚿ᨐ߇ੱ૕㔚૏ߩᦛ✢C ߦ⋧ᒰߒߡ޿ࠆߩߢߪߥ޿߆ ߣ⠨߃ࠄࠇߚ㧚ᱠⴕਛߩੱ૕㔚૏߇Ⴧᄢߒߥ޿╙ 3 ߩ႐ว߽㧘 ห᭽ߩ⠨߃ᣇߢ⺑᣿ߔࠆߎߣ߇ߢ߈ࠆ㧚

࿑ 2 ߩጁ‛ No.11 ߣ No.6 ࠍ㊀ߨวࠊߖߚጁ‛ No.12 ߿ No.14㧘޽ࠆ޿ߪጁ‛ No.11 ߩᐩ᧚ࠍขࠅ㒰޿ߚጁ‛ No.13 ߩੱ૕㔚૏ᄌൻࠍߺࠆߣ㧘ߘࠇߙࠇࠝ࡝ࠫ࠽࡞ߩጁ‛ߩ․ᓽ (a)ጁ‛ ͳ1 R=0.5˜1010ǡ (b)ጁ‛ ͳ2 R=1.0˜1010ǡ (c)ጁ‛ ͳ3 R=1.6˜1010 ǡ (d)ጁ‛ ͳ4 R=2.5˜1010ǡ (e)ጁ‛ ͳ5 R=0.5˜1010 ǡ (f)ጁ‛ ͳ6 R=1.5˜1010 ǡ (g)ጁ‛ ͳ7 R=0.5˜1010ǡ (h)ጁ‛ ͳ8 R=1.3˜1010ǡ (i)ጁ‛ ͳ9 R=0.8˜1010 ǡ (j)ጁ‛ ͳ10 R=2.2˜1011 ǡ (k)ጁ‛ ͳ11 R=1.5˜1011 ǡ (l)ጁ‛ ͳ12 R=1.7˜1011ǡ (m)ጁ‛ ͳ13 R=0.5˜1011ǡ (n)ጁ‛ ͳ14 R=1.2˜1010ǡ ࿑ 2 ᱠⴕਛ߅ࠃ߮ᱠⴕ஗ᱛᓟߩੱ૕Ꮺ㔚㔚૏ߩᄌൻ Fig. 2 Human body voltage curves during walking and after

stopping. A C B 0 v t v A C B 0 t A C B 0 v t A+BݿC (a) (b) (c) ࿑ 3 㔚૏ᷫ⴮ࡄ࠲࡯ࡦߩ㊀⇥

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3 ߇⃻ࠊࠇߡ޿ࠆߎߣ߇ࠊ߆ࠆ㧚ߎߩߎߣ߆ࠄ߽㧘ੱ૕ߩᏪ㔚 㔚૏ߪⶄᢙߩ㔚૏ᄌൻ߇㊀⇥ߐࠇߚ߽ߩߢ޽ࠆߣផቯߐࠇ ࠆ㧚 ࿑ 4 ߪ㧘ᱠⴕߣ஗ᱛࠍ➅ࠅ㄰ߒߚߣ߈ߩੱ૕㔚૏ߩ᷹ቯ଀ ߢ޽ࠆ㧚ߎߩߣ߈ߩጁ‛ߪ No.6 ߢ޽ࠅ㧘ታ㛎ቶᐥߩ਄ߦᢝ ޿ߚෘߐ⚂ 1mm ߩࡐ࡝ࡊࡠࡇ࡟ࡦࠪ࡯࠻਄ࠍᱠⴕߒߚ㧚࿑ ਛߩ⍫ශA ߢ␜ߔࠃ߁ߦ㧘ᱠⴕ஗ᱛᓟߦੱ૕㔚૏߇ᱜ߆ࠄ⽶ ߦᄌൻߔࠆ᭽ሶ߇ߺࠄࠇߚ㧚ᱠⴕߣ஗ᱛࠍ➅ࠅ㄰ߔߚ߮ߦ㧘 ᱠⴕ஗ᱛᓟߩੱ૕㔚૏߇⽶ᣇะ߳ߕࠇߡ޿ߊࠃ߁ߦߺ߃ࠆ㧚 ߹ߚ㧘ᱠⴕਛߦੱ૕ࠍ৻⍍ࠕ࡯ࠬߒߚߣ߈㧘ੱ૕㔚૏߇ 0V ߦߥߞߡ޿ߥ޿ߎߣ߇ࠊ߆ࠆ㧚ߎࠇࠄߩᄌൻࠍ⺑᣿ߔࠆߚ߼ ߦߪ㧘ጁ‛߿ᐥߩᓇ㗀ࠍ฽߼ߚ╬ଔ࿁〝⊛ᬌ⸛߇ᔅⷐߢ޽ࠆ ߣ⠨߃ࠄࠇߚ㧚 2.3 ᒝ೙Ꮺ㔚ߐߖߚ㕒ᱛਛߩੱ૕㔚૏ᄌൻ ࿑ 5 ߪ㧘ᒝ೙⊛ߦᏪ㔚ߐߖߚੱ૕㔚૏ߩᷫ⴮․ᕈߢ޽ࠆ㧚 ጁ‛ No.9 ߦࠃࠆᱠⴕ⚳ੌ⋥ᓟߦ㧘ᐥߩ㒰㔚ࠍⴕࠊߥ޿߹߹ ߩ⁁ᘒߢ⋥ᵹ㔚Ḯߦ৻⍍⸅ࠇߡੱ૕ࠍᒝ೙⊛ߦᱜ߹ߚߪ⽶ ߦᏪ㔚ߐߖ㧘ߘߩᓟߩ㕒ᱛ⁁ᘒߦ߅ߌࠆੱ૕ߩ㔚૏ᄌൻࠍ᷹ ቯߒߚ߽ߩߢ޽ࠆ㧚ߘߩ⚿ᨐ㧘࿑ 5 ߦ␜ߔࠃ߁ߦ㧘ᱜߩ႐ว ߣ⽶ߩ႐วߣߢ㔚૏ᄌൻߦ㆑޿߇ߺࠄࠇ㧘⽶ߩ႐วߦߪ⛘ኻ ୯߇ᤨ㑆ߣ౒ߦჇᄢߒߚ㧚 ߎߩࠃ߁ߥ㔚૏ᄌൻߪ㧘Rxߣ Cxࠍട߃ߚ࿑ 6 ߩ࿁〝ࡕ࠺ ࡞ߦࠃߞߡ⺑᣿ߢ߈ࠆ㧚ߔߥࠊߜ㧘ᐥ߹ߚߪጁ‛ߩᱷ⇐㔚⩄ ߇ੱ૕㔚૏ߦᓇ㗀ߒߡ޿ࠆߣ⠨߃ࠄࠇࠆ㧚ߘߎߢ㧘ߎߩࡕ࠺ ࡞ߦ࿑ 5 ߩ᷹ቯ⚿ᨐࠍᒰߡߪ߼㧘࿁〝ቯᢙ╬ࠍ᳞߼ࠆߣᰴߩ ࠃ߁ߦߥࠆ㧚 ࿑ 5 ߩੱ૕㔚૏ߪ᭎ߨ৻ቯ୯ߩ㔚࿶ߦẋㄭߒߡ޿ࠆߩߢ㧘 ੱ૕߆ࠄߩ㔚⩄ṳᵨ R0߇චಽᄢ߈ߊήⷞߢ߈ࠆߣ઒ቯߒߚ㧚 t=0 ߩߣ߈ߩ vvxߩೋᦼ୯ࠍߘࠇߙࠇV0㧘Vxߣߔࠆߣ㧘ੱ ૕㔚૏v0ߪᰴᑼߢ⴫ࠊߐࠇࠆ㧚 (1) ߎߎߢ㧘 (2) (3) ߎߎߢ㧘t ψ пߣߒߚߣ߈ߩ v0ߩ෼᧤୯ࠍVпߣߒ㧘ੱ૕ 㔚૏߇ᱜߩ႐วߣ⽶ߩ႐วࠍߘࠇߙࠇᷝሼ p ߣ m ߢ⴫ࠊߒߚ ᑼ(1)ߩㅪ┙ᣇ⒟ᑼࠍVxߣǩߦߟ޿ߡ⸃ߊߣ㧘 (4) (5) ߣߥࠆ㧚਄ᑼߦ࿑ 5 ߆ࠄ⺒ߺขߞߚ୯ࠍઍ౉ߔࠇ߫㧘Vxߣ ǩ߇᳞߹ࠆ㧚ߘߩ⚿ᨐࠍ⴫ 2 ߦ␜ߔ㧚 ߎߎߢ㧘ߐࠄߦ C0߇ਈ߃ࠄࠇࠇ߫ Cxߣ Rxࠍ᳞߼ࠆߎߣ߇ ߢ߈ࠆ㧚ᢧ⮮ߪ㧘⿷ߣᐥߩ㑆ߦ᜽ࠎߛ⛘✼‛ߩෘߺࠍᄌ߃ߡ ⴫ 2 ࿑ 5 ߦᑼ(4)㧘(5)ࠍᒰߡߪ߼ߡᓧࠄࠇߚ୯

Table 2 Variables in Equations (4) and (5) derived from Fig. 5.

V0p(V) Vп㨜(V) Ǽp(s) V0m(V) Vпm(V) Ǽm(s) Vx(V) ǩ 780 370 18 -675 -820 7.0 -1500 0.82 ) 1 )( ( ) ( 0 x 0 0 D W t e V V V t v     0m 0p m p m 0m p 0p p 0m m 0p x 1 V V V V V V V V V V V V V        f f f f f f D x 0 0 x x R ĮC IJ C C C Į  ࿑ 5 ⋥ᵹ㔚Ḯߢల㔚ᓟ㧘㕒ᱛ⁁ᘒߩੱ૕㔚૏ A㧦ᱜ㔚࿶ߢల㔚ߒߚ႐ว B㧦⽶㔚࿶ߢల㔚ߒߚ႐ว Fig. 5 Voltage decay curves of a human body initially charged

with a DC voltage with footwear No.9. A: Charged with a positive voltage. B: Charged with a negative voltage.

Human body Cx Rx C0 R0 Cx Rx C 0 R0 v0 vx ࿑ 6 ࿑ 5 ߩ㔚࿶ᄌൻ߆ࠄផቯߐࠇࠆੱ૕ߩ╬ଔ࿁〝 Fig. 6 Equivalent circuit of a charged human body

anticipated from the voltage decay curves in Fig. 5.

࿑ 4 ᱠⴕ஗ᱛࠍ➅ࠅ㄰ߒߚߣ߈ߩੱ૕㔚૏㧔ጁ‛ No.6㧕 Fig. 4 Human body voltage during repeated walking and

stopping with footwear No.6. A

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0 v0 v0 v2 v1 v0 v2 v1 v1 v2=0

(a) During a walk. (|v1|<|v0|) (b) During a walk. (|v1|>|v0|) (c) After stopping walking in (b). v1: v1L or v1R v2: v2L or v2R ࿑ 8 ᱠⴕ஗ᱛᓟߦ⽶㔚࿶߇⃻ࠊࠇࠆᯏ᭴ߩ⺑᣿࿑ Fig. 8 Conceptual diagram representing the appearance of

negative voltage after stopping. 㕒㔚ኈ㊂ࠍ᷹ቯߒ㧘ጁ‛ߣᐥߩᓇ㗀ࠍ㒰޿ߚੱ૕ߩ㕒㔚ኈ㊂ ߇⚂ 62pF ߢ޽ࠆߣߒߡ޿ࠆ3)㧚ዊ㊁ࠄ߽⿷ⵣ㧘⢵૕㧘⣨ߩ㕒 㔚ኈ㊂ࠍಽഀߒߡ᷹ቯߒ㧘ߎࠇߦㄭ޿⚿ᨐࠍᓧߡ޿ࠆ11)㧚ߘ ߎߢ㧘ᢧ⮮ߩ୯ߦ᷹ቯ♽ߩ㕒㔚ኈ㊂⚂ 30pF ࠍട߃ߚ 92pF ࠍ C0ߣߔࠆߣ Cxߪ 420pF ߣߥࠅ㧘ǼpߣǼmߦኻߔࠆ Rxߪߘࠇ ߙࠇ㧘2.4˜1011ǡ߅ࠃ߮ 9.3˜1010ǡߣߒߡ᳞߼ࠄࠇࠆ㧚 ࿑ 4 ߩᱠⴕ஗ᱛࠍ➅ࠅ㄰ߒߚߣ߈ߦߺࠄࠇߚ⽶ᣇะ߳ߩߕ ࠇ߽㧘࿑ 6 ߩ╬ଔ࿁〝ߦࠃߞߡ⺑᣿ߢ߈ࠆ㧚ߔߥࠊߜ㧘ᱠⴕ ਛߦ Cx߇⽶ߦల㔚ߐࠇ㧘ᱠⴕ஗ᱛࠍ➅ࠅ㄰ߔߏߣߦvxߩ⽶ 㔚࿶߇ᄢ߈ߊߥࠅ㧘ᦨ⚳⊛ߦ࿑ਛߩ⍫ශA ߦ␜ߔࠃ߁ߦੱ૕ 㔚૏߇⽶ߦߥߞߚߣ⠨߃ࠄࠇࠆ㧚߹ߚ㧘࿑ 4 ߩًශߢ␜ߒߚ ᤨὐߢੱ૕ࠍࠕ࡯ࠬߒߚߣ߈ߦੱ૕㔚૏߇ 0V ߦߥࠄߥ߆ߞ ߚߎߣ߽㧘Cxߩ㔚⩄߇ߔߴߡ᡼㔚ߒߥ߆ߞߚߣ⠨߃ࠇ߫⺑᣿ ߢ߈ࠆ㧚 એਅ㧘ߎࠇࠄߩ⚿ᨐࠍෳ⠨ߦߒߡ㧘ᱠⴕᤨߩੱ૕Ꮺ㔚ߩ╬ ଔ࿁〝ࠍᬌ⸛ߒߚ㧚 3. ੱ૕ߩᱠⴕᏪ㔚ߦ߅ߌࠆ࿁〝ࡕ࠺࡞ߩᬌ⸛ 3.1 ᱠⴕᤨߩᏪ㔚㔚૏ࠍᮨᡆߔࠆߚ߼ߩ╬ଔ࿁〝 ࿑ 6 ߩ╬ଔ࿁〝ߪ㕒ᱛਛߩੱ૕ߦߟ޿ߡ᳞߼ߚ߽ߩߢ޽ߞ ߚ㧚ߘߎߢ㧘ᱠⴕേ૞ߦ઻߁㔚⩄ߩ⊒↢ࠍ⴫ࠊߔߚ߼㧘࿑ 6 ߩ࿁〝ߦጁ‛ߣᐥߩ㑆ߩ㕒㔚ኈ㊂ C2R߹ߚߪ C2Lࠍㅊടߒߚ㧚 ߎࠇࠍ࿑ 7 ߦ␜ߔ㧚ߎߩ࿑ߪ㧘ฝ⿷ࠍ਄ߍߚߣ߈ߩ⁁ᘒࠍ⴫ ࠊߒߡ޿ࠆ㧚Ꮐ⿷ࠍ਄ߍߚߣ߈ߦߪ C2Rߩઍࠊࠅߦ C1Lߣ⋥ ೉ߦ C2L߇౉ࠅ㧘ᱠⴕਛߪਔ⿷߇หᤨߦ⌕࿾ߔࠆߎߣߥߊߎ ߩ⁁ᘒ߇੤੕ߦ➅ࠅ㄰ߐࠇ㧘ᱠⴕ஗ᱛᓟߪ C2Lߣ C2R߇ߥߊ ߥࠆߣ઒ቯߔࠆ㧚 ࿑ 7 ߩ࿁〝ߦࠃࠅ㧘ᱠⴕਛ߅ࠃ߮ᱠⴕ஗ᱛᓟߩੱ૕㔚૏ᄌ ൻߦߟ޿ߡ㧘᭎ߨએਅߩࠃ߁ߦ⺑᣿ߢ߈ࠆ㧚C0㧘C1L㧘C2L㧘 C1R㧘C2Rߩ㔚࿶ࠍߘࠇߙࠇv0㧘v1L㧘v2L㧘v1R㧘v2Rߣߒ㧘㔚࿶ ߩะ߈ߪੱ૕஥߇ᱜ㧘ᄢ࿾஥߇⽶ߢ޽ࠆߣߔࠆ㧚߹ߚ㧘઒ߦ㧘 ᐥߣጁ‛ߩ㑆ߦ⊒↢ߔࠆ㔚࿶v2Lߣv2Rߪචಽᄢ߈޿ᱜߩ㔚࿶ ߢ޽ࠅ㧘ੱ૕㔚૏v0ߩೋᦼ୯ߪ 0V ߢ޽ࠆߣߔࠆ㧚 ߚߣ߃߫㧘࿑ 7 ߩฝ⿷ࠍ਄ߍߚ⁁ᘒߢߪ㧘v0=v1R+v2Rߢ޽ ࠆ㧚v2R߇චಽᄢ߈޿ᱜߩ㔚࿶ߢ޽ࠆ߆ࠄ㧘࿑ 8(a)ߦ␜ߔࠃ߁ ߦ㧘C0ߩ㔚࿶v0߇ᱜ㧘C1Rߩ㔚࿶v1R߇⽶ߦߥࠆ㧚ߎߩᓟ㧘 ࿁〝ฦㇱߩ㔚࿶ߪㆊᷰ⊛ߦᷫ⴮ߔࠆ߇㧘ᰴߩ 1 ᱠߢ࿁〝ߩᏀ ฝ߇੤ᦧߒ㧘એਅห᭽ߩߎߣ߇➅ࠅ㄰ߐࠇࠆ㧚 ߎߩࠃ߁ߦv1R߹ߚߪv1L߇⽶ߦߥࠆ⚿ᨐ㧘C0߿ C1R㧘C1L ߩల᡼㔚ㅦᐲߩ⋧੕㑐ଥߦࠃߞߡߪ㧘v0߇⽶ߦߥࠆน⢻ᕈ߇ ޽ࠆޕߎࠇߪ㧘ᱠⴕਛ߽ᱠⴕ஗ᱛᓟ߽޿ߕࠇߩ႐ว߽⠨߃ࠄ ࠇࠆߎߣߢ޽ࠆޕߚߣ߃߫㧘࿑ 9(b)ߩࠃ߁ߦᱠⴕ஗ᱛ⋥೨ߩ v1Rߣv1L߇v0ࠃࠅ߽චಽᄢ߈޿ߣ㧘࿑ 9(c)ߩࠃ߁ߦᱠⴕ஗ᱛ ᓟߩੱ૕㔚૏ v0߇ᷫ⴮ߔࠆㆊ⒟ߢ⽶ߦᄌൻߔࠆน⢻ᕈ߇޽ ࠆ㧚ߎࠇ߇㧘࿑ 2 ߿࿑㧠ߢ⷗ࠄࠇߚੱ૕㔚૏ߩ╓ภ߇ᄌൻߔ ࠆᯏ᭴ߢ޽ࠆ㧚 3.2 ╬ଔ࿁〝ߩቯᢙ ⸘▚⚿ᨐࠍᲧセߒ߿ߔߊߔࠆߚ߼㧘R0ߣ R1ߩ޿ߕࠇ߆৻ ᣇࠍ৻ቯ୯ߦ࿕ቯߒ㧘ઁᣇࠍࡄ࡜ࡔ࡯࠲ߣߒߡᄌൻߐߖߚ㧚 ࿑ 2 ߢߪ㧘ੱ૕߇ CR ਗ೉࿁〝ߢ޽ࠆߣ઒ቯߒߡᱠⴕ஗ᱛᓟ ߩ✭๺ᤨ㑆߆ࠄ᭎▚ߢ᳞߼ߚᛶ᛫୯ R ߪ 1010㨪1011ǡߢ޽ߞ ߚ㧚ߘߎߢ㧘R0ߣ R1ߩ୯ߪ 1010ǡએ਄ߩ▸࿐ߢᄌൻߐߖߚ㧚 R1ߩ࿕ቯ୯ߪ㧘࿑ 6 ߩ╬ଔ࿁〝ߢ᳞߼ߚ R㨤ࠍෳ⠨ߦߒߡ 1011ǡߦ⸳ቯߒߚ㧚R0ߩ࿕ቯ୯ߪ㧘R㨤ࠍ᳞߼ߚߣ߈ߣห᭽㧘 R1ࠃࠅචಽᄢ߈޿ߣߺߥߖࠆ୯ߣߒߡ 1012ǡߦ⸳ቯߒߚ㧚 C0ߩ୯ߪ㧘ᑼ(2)ߩ⸘▚ߢߪ 92pF ߣߒߚ߇㧘ߎߎߢߪ᭎ᢙ ߢචಽߢ޽ࠆߚ߼ 100pF ߦ⸳ቯߒߚ㧚 C1ߩ୯ߪ㧘࿑ 6 ߩ╬ଔ࿁〝ߢ᳞߼ߚ Cxࠍෳ⠨ߦߒߚ㧚Cx ߩ୯ 400pF ߪਔ⿷߇ᐥߦ⌕࿾ߒߚ⁁ᘒߢ᳞߼ߚ߽ߩߢ޽ࠆ߆ ࠄ㧘C1ߪ ⿷ಽߣߒߡ 200pF ߦ⸳ቯߒߚ㧚 C3ߩ୯ߪ㧘Pirici ࠄߩੱ૕Ꮺ㔚ࡕ࠺࡞ߩ᭴▽ࠍෳ⠨ߦߒߡ ᰴᑼߢ⸘▚ߒߚ11㧕 ࿑ 7 ᱠⴕᤨߩੱ૕Ꮺ㔚㔚࿶ߩ⸘▚ߦ↪޿ߚ╬ଔ࿁〝 Fig.7 Equivalent circuit used for simulation of electrostatic

charging of a walking human body.

R1R R0 C0 C1R C1L R1L iL i0 iR v1L v1R v2R v0 㧗 㧙 㧗 㧙 㧗 㧙 㧗 㧙C2R Human body

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(6) ߎߎߢǭ0ߪ⌀ⓨߩ⺃㔚₸㧘ǭrߪ‛⾰ߦࠃߞߡ⇣ߥࠆᲧ⺃㔚 ₸ߢ޽ࠆ㧚ߎߩ႐ว㧘ⓨ᳇ਛߢ޽ࠆ߆ࠄǭrߪ 1 ߢ޽ࠆ㧚ᐩ㕙 Ⓧ S ࠍ 0.025m2㧘ᐥ߆ࠄߩ〒㔌 d ࠍ 0.05m ߣߒߡᑼ(6)ߢ⸘▚ ߒߚ⚿ᨐ߆ࠄ㧘C2ߪ 5pF ߦ⸳ቯߒߚ㧚 ߎߩࡕ࠺࡞ߢߪ㧘ጁ‛߇ᐥ߆ࠄ㔌ࠇߚߣ߈ C3ߦ⊒↢ߔࠆ㔚 ⩄㊂ࠍ઒ቯߔࠆᔅⷐ߇޽ࠆ㧚Pirici ࠄߪ㧘㒠ゞᤨߩੱ૕࡮ᐳᏨ 㑆㧔ធ⸅㕙Ⓧ 0.09m2㧕ߢ⊒↢ߔࠆ㔚⩄㊂ࠍ 2.5ǴC ߣߒߡ޿ ࠆ12)㧚ߎߩ୯ࠍන⚐ߦ㕙ⓍᲧߢ឵▚ߔࠆߣ㧘ጁ‛ߦ⊒↢ߔࠆ 㔚⩄㊂ߪ⚂ 0.7ǴC ߣߥࠆ㧚ߒ߆ߒ㧘ߎߩ୯ࠍ↪޿ߡ⸘▚ߔࠆ ߎߣߪታ㓙⊛ߢߪߥ޿㧚ߥߗߥࠄ㧘C2ߩ㔚࿶߇ 140kV ߣ⸘▚ ߐࠇࠆ߆ࠄߢ޽ࠆ㧚߽ߒ㧘ታ㓙ߦߘߩࠃ߁ߥ㔚⩄߇⊒↢ߒߚ ߣߒߡ߽㧘ጁ‛߇ᐥ߆ࠄ㔌ࠇࠆㆊ⒟ߢ㔚⩄ߩㅒᵹ 12㧕߇⿠ߎ ࠅ㧘㑆㓗ߩ⛘✼⠴ജࠍ⿥߃ࠆ㔚࿶߹ߢ㆐ߔࠆߎߣߪߥ޿ߢ޽ ࠈ߁㧚ߘߎߢ㧘C2ߩ㔚࿶ߩᅷᒰߥ୯ߣߒߡ 1 ᩴዊߐ޿ 10kV ࠍᗐቯߒ㧘⊒↢ߩ㔚⩄㊂ࠍ 0.05ǴC ߦ⸳ቯߒߚ㧚 3.3 ╬ଔ࿁〝ߦࠃࠆ⸘▚ᣇᴺ ࿑ 7 ߦ␜ߔࠃ߁ߦฦㇱߩ㔚࿶ߣ㔚ᵹࠍቯ߼ࠆߣ㧘ࠝ࡯ࡓߩ ᴺೣߣࠠ࡞ࡅࡎ࠶ࡈߩᴺೣ߆ࠄ㧘ᰴᑼ(7)ߩ㑐ଥ߇ᚑࠅ┙ߟ㧚 ߎߎߢ㧘v ߪ0 dv0 dtࠍ⴫ߔ߽ߩߣߔࠆ㧚߹ߚ㧘ฝ⿷஥ߣᏀ ⿷஥ߩ࿁〝ቯᢙߪ╬ߒ޿ߣ⠨߃㧘C1R=C1L=C1㧘C2R=C2L=C2㧘 R1R=R1L=R1㧘R2R㧩R2L㧩R2ߢ޽ࠆߣߔࠆ㧚 (7) ᑼ(7)߆ࠄ㔚ᵹߩᄌᢙࠍᶖ෰ߔࠆߣᰴᑼ߇ᓧࠄࠇࠆ㧚 (8) ߎߩㅪ┙ᓸಽᣇ⒟ᑼߩᢙ୯⸃ࠍ࡞ࡦࠥ࡮ࠢ࠶࠲࡯ᴺࠍ↪޿ ߡ⸘▚ߒ㧘ᱠⴕߦ઻߁ੱ૕㔚૏ v0ߩᤨ㑆ᄌൻࠍ᳞߼ߚ㧚⸘▚ ߩೞߺᤨ㑆ߪ 0.1s㧘ᱠⴕㅦᐲߪᲤ⑽ 2 ᱠߣߒߚ㧚߹ߚ㧘ᱠⴕ 㐿ᆎ೨ߩ᧦ઙߣߒߡ㧘㔚࿶ v0㧘v1L߅ࠃ߮ v1Rߩೋᦼ୯ߪ 0V ߣߒߚ㧚 Ꮐฝߩ⿷ࠍ੤੕ߦ㧝ᱠߕߟㅴ߼ࠆߚ߮ߦ㧘࿑ 7 ߩ࿁〝ߩᏀ ฝࠍ౉ࠇᦧ߃ࠆᔅⷐ߇޽ࠆ㧚ታ㓙ߩ⸘▚਄ߢߪ㧘ࡊࡠࠣ࡜ࡓ ߩਛߢ㔚࿶ v1Lߣ v1Rߩ୯ࠍ౉ࠇᦧ߃ࠆߎߣߦࠃߞߡᏀฝߩ౉ ࠇᦧ߃ࠍⴕߞߚ㧚৻ᱠߏߣߩ⸘▚඙㑆ߩೋᦼ୯ߣߒߡ㧘ጁ‛ ߣᐥ㑆ߩ㕒㔚ኈ㊂ C3ߦ 0.05ǴC ߩ㔚⩄ࠍਈ߃ߚ㧚ᱠⴕᤨ㑆ߪ 60s 㑆ߣߒ㧘ߘߩᓟߪᱠⴕ஗ᱛߔࠆߣߒߚ㧚 3.4 ╬ଔ࿁〝ߦࠃࠆ⸘▚⚿ᨐ ᑼ(7)㧘(8)ߦࠃࠆ⸘▚⚿ᨐߩ৻଀ࠍ࿑ 9(a)㨪(c)ߦ␜ߔ㧚࿑ 2 ߢߺࠄࠇߚࠃ߁ߥᱠⴕਛ޽ࠆ޿ߪᱠⴕ஗ᱛᓟߦੱ૕㔚૏ߩ ╓ภ߇ᄌࠊࠆߣ޿߁․ᓽ߇⃻ࠊࠇߚ㧚એਅ㧘⸘▚⚿ᨐߦߺࠄ ࠇࠆ․ᓽࠍ᜼ߍߡ⠨ኤߔࠆ㧚 3.4.1 R0ࠍᄌൻߐߖߚ႐ว ࿑ 9(a)ߪ R1ࠍ 1011ǡߢ࿕ቯߒߡ R0ࠍᄌൻߐߖߚ႐วߩ⸘ ▚⚿ᨐߢ޽ࠆ㧚R0߇ዊߐߊߥࠆߣ㧘ᱠⴕਛߩੱ૕㔚૏߇ૐߊ ߥߞߚ㧚R0߇ 1012ǡએਅߢߪ㧘ᱠⴕ஗ᱛᓟߩੱ૕㔚૏߇ᷫ⴮ ㆊ⒟ߢᱜ߆ࠄ⽶ߦᄌൻߔࠆ⁁ᴫ߇⃻ࠊࠇ㧘R0߇ 1011ǡߩߣ߈ ߦ⽶㔚࿶ߩ⛘ኻ୯߇ᦨ߽ᄢ߈ߊߥߞߚ㧚 ࿑ 2 ߩታ᷹଀ߦ߅޿ߡታ㛎ߏߣߦᄌൻߐߖߚ᧦ઙߪጁ‛ߩ ⒳㘃ߛߌߢ޽ࠆ㧚ߎߩታ㛎᧦ઙߩ㆑޿ߦࠃߞߡ㧘࿑ 7 ߩ╬ଔ ࿁〝ߢ޿߁ߣ R1߇ᄌൻߒߚߪߕߢ޽ࠆ㧚߽ߒ㧘R1ߛߌ߇ᄌ ൻߒߚߩߢ޽ࠇ߫㧘ታ᷹଀ߦߪ R0ߩᓇ㗀߇⃻ࠊࠇߥ޿ߎߣߦ ߥࠆ㧚ߒ߆ߒ㧘ጁ‛߿ᐥࠍㅢߒߡߩ㕒㔚᳇ߩṳᵨߪታ㓙ߦ⚻ 㛎ߔࠆߣߎࠈߢ޽ࠅ㧘ߎࠇߪ R0ߩᚑಽߣߒߡ⠨߃ࠆߴ߈߽ߩ ߢ޽ࠆ㧚ߔߥࠊߜ㧘ጁ‛ߩ⒳㘃ࠍᄌ߃ߚߎߣߦࠃߞߡታ᷹଀ ߩ㔚૏ᄌൻߦߪ R0ߣ R1ߩਔᣇߩᓇ㗀߇ᷙ࿷ߒߡ޿ࠆߣ⠨߃ ࠄࠇࠆߚ߼㧘⸘▚⚿ᨐߣන⚐ߦᲧセߔࠆߎߣ߇ߢ߈ߥ޿㧚ታ ᷹଀ߦ߅ߌࠆ R0ߣ R1ࠍಽ㔌ߔࠆߎߣ߇੹ᓟߩᬌ⸛ߦ߅ߌࠆ ⺖㗴ߢ޽ࠆ㧚 3.4.2 R1ࠍᄌൻߐߖߚ႐ว ࿑ 9(b)ߪ㧘R0ࠍ 1011ǡߢ࿕ቯߒߡ R1ࠍᄌൻߐߖߚ႐วߩ⸘ ▚⚿ᨐߢ޽ࠆ㧚R1߇ᄢ߈ߊߥࠆߦᓥߞߡੱ૕㔚૏ߩ਄᣹߇✭ ᘟߦߥߞߚ㧚ߘߩ⚿ᨐ㧘R1ߩ୯߇ 1012ǡએ਄ߢߪ㧘৻ቯߩᱠ ⴕᤨ㑆ౝߦ೔㆐ߒᓧࠆੱ૕㔚૏ߩᦨᄢ୯߇ૐߊߥߞߚ㧚 ࿑ 9(b)ߦ␜ߒߚC ߩ✭ᘟߥੱ૕㔚૏ᄌൻߩࡄ࠲࡯ࡦߪ㧘࿑ 2 ߩਛߢߪ㧘(j)ߩጁ‛ No.10 ߩታ᷹଀߇ᦨ߽㘃ૃߒߡ޿ࠆ㧚 ߎߩጁ‛ No.10 ߩ✭๺ᤨ㑆߆ࠄ᳞߼ߚ R ߩ୯ߪታ᷹଀ߩਛߢ ᦨ߽ᄢ߈ߊ㧘R1ߦ⋧ᒰߔࠆᛶ᛫߇ᄢ߈߆ߞߚߎߣࠍ␜ໂߒߡ ޿ࠆ㧚 ৻ᣇߢ㧘࿑ 2 ߩታ᷹଀ߩਛߢ R ߇ᦨ߽ዊߐ޿(a)㧘(e)㧘(g) ߩᄌൻࡄ࠲࡯ࡦߪ㧘޿ߕࠇ߽ 500V ೨ᓟߩૐ޿୯ߢផ⒖ߒߡ ߅ࠅ㧘࿑ 9(b)ߩD ߩࡄ࠲࡯ࡦߣ㘃ૃߒߡ޿ࠆ㧚 ߎࠇࠄߩߎߣ߆ࠄ㧘೨㗄ߢㅀߴߚ R0ߩᷙ࿷߇ήⷞߢ߈ߥ޿ ߽ߩߩ㧘࿑ 2 ߩታ᷹଀ߦߪ R1ߩᓇ㗀߇ᒝߊ⃻ࠊࠇߡ޿ࠆߣ⠨ ߃ࠄࠇࠆ㧚ߎࠇߪ㧘ታ᷹଀ߢጁ‛ߩ⒳㘃ࠍᄌ߃ߚߣ޿߁ߎߣ ߆ࠄ੍߽ᗐߢ߈ࠆ⚿ᨐߢ޽ࠆ㧚 ࿑ 9 ߦ␜ߔࠃ߁ߦ㧘R1ߩ୯߇ 1012ǡએ਄ߩߣ߈㧘ᱠⴕ஗ᱛ ᓟߩੱ૕㔚૏ߩ⸘▚୯߇⽶ߦᄌൻߒߚ㧚R1ߪጁ‛ߩᛶ᛫ࠍᗐ d S C H0Hr ° ° ¿ ° ° ¾ ½    1 R 2R 1R 1 L 1L 0 0 0 R 2R 2 1R 1 L 1L 1 R L 0 0 0 R R R C C C C i v v i v i v i v v i v i i i v

°° ° ° ¿ °° ° ° ¾ ½      R R R R R R L L R R L v v v v v v v v v v v v v v v v 2 1 1 1 2 0 1 1 2 2 2 1 0 1 1 1 1 1 0 1 1 1 1 2 1 1 1 1 0 0 1 1 0 1 0 0 R C R C R C R C R C 2R1 R C

(6)

ቯߒߚ߽ߩߢ޽ࠆ߆ࠄ㧘ᵻ㊁ߩ⸃⺑ 13㧕ࠍᒁ↪ߔࠆߣ㧘ߎߩ ߎߣߪᰴߩࠃ߁ߦ߽⺑᣿ߢ߈ࠆ㧚ߔߥࠊߜ㧘ጁ‛ߩᛶ᛫߇Ყ セ⊛ૐ޿႐ว㧔1012ǡએਅ㧕ߪ㧘⊒↢㔚⩄߇ੱ૕ో૕ߦᐢ߇ ߞߡੱ૕ߩ㔚૏ࠍ਄ߍࠆ߇㧘㜞޿႐วߦߪ㧘ጁ‛ߣ⿷ߩⵣ߇ 㔚᳇ੑ㊀ጀߣߥࠅ㧘ੱ૕㔚૏ߪጁ‛ߩ㔚૏ࠃࠅૐߊߥߞߚߣ ⠨߃ࠄࠇࠆ㧚 3.4.3 R0㧘R1ࠍหᤨߦᄌൻߐߖߚ႐ว ࿑ 9(c)ߪ㧘R0ߣ R1ߩਔᣇࠍหᤨߦᄌൻߒߚ႐วߩ⸘▚⚿ᨐ ߢ޽ࠆ㧚࿑ 9(b)ߩ႐วߣห᭽㧘R0ߣ R1ߩ୯߇ᄢ߈ߊߥࠆߣ ੱ૕㔚૏ߩ਄᣹߇✭ᘟߦߥࠅ㧘৻ቯߩᱠⴕᤨ㑆ౝߢᲧセߒߚ ႐วߩ೔㆐ߒᓧࠆੱ૕㔚૏ߩᦨᄢ୯߇ૐߊߥߞߚ㧚 R0ߣ R1߇ 10 10 ǡߩߣ߈ߩA ߩࡄ࠲࡯ࡦߢߪ㧘ᱠⴕਛߪੱ ૕㔚૏߇߶ߣࠎߤ 0V ߢ޽ࠆ߇㧘ᱠⴕ஗ᱛᓟߦ⽶ߩᣇะߦᄢ ߈ߊߥࠆߣ޿߁࿑ 2(i)㧘(k)ߩታ᷹଀ߦ㘃ૃߒߚ․ᓽ߇ߺࠄࠇ ߚ㧚ߚߛߒ㧘࿑ 2 ߩ✭๺ᤨ㑆߆ࠄ᳞߼ߚߎࠇࠄߩጁ‛ߩ R ߩ ୯ߪฦޘ0.8˜1010ǡߣ 1.5˜1011ǡߢ޽ࠅ㧘ᓟ⠪ߩ࿑ 2(k)ߩ႐ วߦߪᔅߕߒ߽ R0ߣ R1ߩਔᣇߩ୯߇ዊߐ޿ߣߪ⸒߃ߥ޿㧚 ߎߩ࿁〝ࡕ࠺࡞ߢߪ⴫ࠊߖߡ޿ߥ޿೎ߩⷐ⚛ࠍ⠨ᘦߔࠆᔅ ⷐ߇޽ࠆߣᕁࠊࠇࠆ㧚 4. ߹ߣ߼ ጁ‛ߩ⒳㘃ࠍᄌ߃ߡᱠⴕਛߩੱ૕Ꮺ㔚㔚૏ࠍ᷹ቯߒ㧘ᱠⴕ ஗ᱛᓟߩᷫ⴮ㆊ⒟ߢੱ૕㔚૏߇ᱜ߆ࠄ⽶ߦᄌൻߔࠆߣ޿߁ ታ᷹଀ࠍ␜ߒߚ㧚ߘߒߡ㧘ߎߩᏪ㔚㔚૏ߩ╓ภߩᄌൻߪ㧘ጁ ‛߿ᐥߩᓇ㗀ࠍട๧ߒߚ╬ଔ࿁〝ߦࠃߞߡ⺑᣿ߢ߈ࠆߎߣ ࠍ␜ߒߚ㧚ߐࠄߦ㧘ታ㛎⚿ᨐߦၮߠ޿ߡ࿁〝ቯᢙࠍ᳿ቯߒ㧘 ⸘▚ߦࠃࠆࠪࡒࡘ࡟࡯࡚ࠪࡦࠍⴕߞߚߣߎࠈ㧘ታ᷹଀ߦߺࠄ ࠇߚ⽶ߦᄌൻߔࠆ․ᓽߥߤ߇ౣ⃻ߐࠇߚ㧚 ߎߩ⎇ⓥߢߪ㧘ጁ‛߿ᐥߩᓇ㗀ࠍട๧ߒߚ◲නߥ╬ଔ࿁〝 ࠍ↪޿ߡ㧘ᱠⴕᤨߦߺࠄࠇࠆੱ૕㔚૏ߩ╓ภߩᄌൻߩ⺑᣿ࠍ ⹜ߺߚ߽ߩߢ޽ࠆ㧚ታ㓙ߩᱠⴕᏪ㔚ߪੱ૕ࠍขࠅᏎߊ๟࿐ߩ ‛૕߽฽߼ߚᄙ૕㑆ߩಽᏓቯᢙ⊛ขࠅᛒ޿ࠍᔅⷐߣߔࠆⶄ 㔀ߥ⃻⽎ߢ޽ࠆ㧚නߥࠆ╬ଔ࿁〝ߩⶄ㔀ൻߢߪߥߊ㧘ታ᷹୯ ߣߩኻᔕߦၮߠ޿ߚቯ㊂⊛ߥ੍᷹ߦ߽૶߃ࠆ⸘▚ࡕ࠺࡞ߦ ⊒ዷߐߖࠆߎߣ߇੹ᓟߩ⺖㗴ߢ޽ࠆ㧚  ෳ⠨ᢥ₂ 1) ዊᨋാੱ, ᧛㦮ᙗ㓶, ⮮ᨋብ৻, ᧻੗ḩ: 㕒㔚᳇ቇળ⻠Ṷ ⺰ᢥ㓸 '82, p.247, 㕒㔚᳇ቇળ (1982) 2) 㕒㔚᳇ቇળ: ᣂ 㕒㔚᳇ࡂࡦ࠼ࡉ࠶ࠢ, p.204-283, ࠝ࡯ ࡓ␠ (1998) 3) ᢧ⮮ᵗ: ᔕ↪‛ℂ, 32 (1963) 301 4) ↰⇗ᵏᐘ, ఽ₹ീ, ⫱ᳰᱜਯ੺, ਃ␹ᐘ↵: 㕒㔚᳇ቇળ⻠ Ṷ⺰ᢥ㓸 '86, p.367, 㕒㔚᳇ቇળ (1986) 5) ⪤ᧄ቟ᤘ, ᷰㆺᙗ㆏, ᧁਅൎඳ: 㕒㔚᳇ቇળ⻠Ṷ⺰ᢥ㓸 ' 93, p.407, 㕒㔚᳇ቇળ (1993) 6) ᧻የ⟵ノ, ↰⇗ᵏᐘ: 㕒㔚᳇ቇળ⻠Ṷ⺰ᢥ㓸 '87, p.239, 㕒㔚᳇ቇળ (1987) 7) ◉ፒ⮍, ᫪ᢅೣ: 㔚ሶᖱႎㅢାቇળᤐቄో࿖ᄢળ⻠Ṷ⺰ ᢥ㓸, p.1-280, 㔚ሶᖱႎㅢାቇળ (1988) 8) ੖๧ᒄ, Ⓑ⪲ੳ, ศ↰㓉♿, ጟ↰ቁᄦ: ╙ 7 ࿁ࠦࡦ࠲ࡒࡀ ࡯࡚ࠪࡦࠦࡦ࠻ࡠ࡯࡞⎇ⓥᄢળ੍Ⓜ㓸, p.215, ᣣᧄⓨ᳇ ᷡᵺදળ (1988) 9) ዊ㊁㓷ม: 㕒㔚᳇ቇળ⹹, 15 (1991) 19 10) JIS L 1021ᢝ‛⹜㛎ᣇᴺ (1979)

11) D. Pirici, J. Rivenc, T. Lebey, D. Malec, A, Agneray, M. Cheaib: Journal of Electrostatics, 62 (2004) 167

12) ᧛㦮ᙗ㓶: 㕒㔚᳇㓚ἴኂኻ╷ࡂࡦ࠼ࡉ࠶ࠢ(਄), p.11, ࡑ ࠣࡠ࠙ࡅ࡞ᅢቇ␠ (1977) 13) ᵻ㊁๺ବ: 㕒㔚᳇ቇળ⹹, 5 (1981) 428 C0 =100pF C1 =200pF R0 =1˜1012ǡ C0 =100pF C1 =200pF R1 =1˜1011ǡ A㧦R1 =1˜1010ǡ B㧦R1 =1˜1011ǡ C㧦R1 =1˜1012ǡ D㧦R1 =1˜1013ǡ A㧦R0 =1˜1010ǡ B㧦R0 =1˜1011ǡ C㧦R0 =1˜10 12ǡ D㧦R0 =1˜1013ǡ C0 =100pF C1 =200pF A㧦R0 =R1 =1˜10 10 ǡ B㧦R0 =R1 =1˜1011ǡ C㧦R0 =R1 =1˜1012ǡ D㧦R0 =R1 =1˜1013ǡ ࿑ 9 ⸘▚⚿ᨐߩ଀

Fig. 9 Typical computations results. (a) R1ࠍ࿕ቯߒߡ㧘R0ࠍᄌൻߐߖߚ႐ว

(a) R1is constant and R0 varies.

(b) R0ࠍ࿕ቯߒߡ㧘R1ࠍᄌൻߐߖߚ႐ว

(b) R0 is constant and R1 varies.

(c) R0ߣ R1ࠍหᤨߦᄌൻߐߖߚ႐ว

Fig. 1 Schematic of measurement apparatus.
Table 1  Footwear used for experiments.
Table 2  Variables in Equations (4) and (5) derived from Fig. 5.
Fig. 8  Conceptual diagram representing the appearance of negative voltage after stopping
+2

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Reynolds, “Sharp conditions for boundedness in linear discrete Volterra equations,” Journal of Difference Equations and Applications, vol.. Kolmanovskii, “Asymptotic properties of

Answering a question of de la Harpe and Bridson in the Kourovka Notebook, we build the explicit embeddings of the additive group of rational numbers Q in a finitely generated group

[25] Nahas, J.; Ponce, G.; On the persistence properties of solutions of nonlinear dispersive equa- tions in weighted Sobolev spaces, Harmonic analysis and nonlinear

Then it follows immediately from a suitable version of “Hensel’s Lemma” [cf., e.g., the argument of [4], Lemma 2.1] that S may be obtained, as the notation suggests, as the m A

Applications of msets in Logic Programming languages is found to over- come “computational inefficiency” inherent in otherwise situation, especially in solving a sweep of