laser induced plasma micro machining
TRANSCRIPT
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LASER INDUCED PLASMA MICRO MACHIN
MOHAMMED A
P S
B120292ME
B BATCH
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INTRODUCTION
Micro Manufacturing – Products in range of μm
Products like micro shafts, micro slots , micro gears etc.
Applications in Automobiles, Health & Biotech , IT , Instrumentaetc.
Micro Te"turing – Micro channels, Micro dimples and geometrie
from μm to mm
#sed for surface friction control , Impro$e optical absorption , hdrophobicit.
Applications in Tribolog, Biomedical engineering , Metal cutting
%on$entional processes emploed – Micro 'M & (aser ablation
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MICRO EDM AND LASERABLATION
•
Micro 'M )Material remo$al b ablation $ia generation of plasmagenerated b an electric *eld
• (imitations ) (o+ M, inabilit to machine polmers & ceramics ,
amount of non producti$e cost in$ol$ed.
•
(aser ablation ) Ablation of material due to melting and $apori-atiofacilitated b short pulsed lasers +ith high freuenc.
• (imitations ) Inabilit to machine opticall transparent materials,
dependence of ablation on $arious control factors.
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LASER INDUCED PLASMA MICROMACHINING
•
It is a multi material , tool/less high precision micro manufacturing
• Able to machine materials like ceramics , glass and polmers.
• 0ork piece immersed in dielectric, plasma is generated b dielectric
breakdo+n using laser.
• The plasma absorbs energ and comes in contact +ith +ork piece
• Material remo$al is combined e1ect of mechanical erosion $ia shock
thermal $apori-ation of material due to contact +ith plasma.
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BA!I% !%HMATI% 23 (IPMM P2%!!
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PLASMA GENERATION
• The primar process is the generation of plasma. This is achie$ed +ith the
short high freuenc pulsed laser.
• These lasers ha$e high po+er due to small duration . 0hen focused in diele
high po+er densities.
• 0hen po+er densit e"ceeds threshold ioni-ation potential , results in plasm
generation due to optical breakdo+n.
• Plasma absorbs energ from laser and e"pands.
• The plasma is an opaue , highl locali-ed thermal -one +ith temperature a
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MATERIAL REMOVAL
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Plasma absorbs energ from laser/ plasma interaction.• Absorbed energ is partitioned into mechanical & thermal ener
• Thermal energ causes increase in temperature 894566 7:. Thiconducted to +ork piece through plasma/ +ork piece contact.
• Mechanical energ causes shock+a$es and ca$itation, +hich re
dielectric & appl pressure on +ork piece surface.
• This holds back molten metal, but +hen plasma collapses dieleback and ;ushes out the molten metal.
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MACHINING SETUP
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• 2? laser emitting laser pulses of @ ps duration at 4 nm +a$elength and fre
C6/466 kH- .
• The beam pro*le is Daussian and beam is linearl polari-ed.
• 0orkpiece immersed in dielectric is placed on *$e a"is positioning sstem) transl
rotational '23
• (aser beam is focused using a triplet lens +hich can be adEusted for precise focus.
• At super threshold $alue plasma generated near focal point and brought into conta
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•
'ielectric properties a1ect plasma generation and thus machin
• The desirable properties are)
(o+ absorption coeFcient
(o+ $ariation in absorption coeFcient +ith temperature
(o+ ioni-ation energ
(o+ $iscosit
!uFcientl high dielectric constant $alue
DIELECTRIC PROPERTIES
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LASER PERFORMANCE PARAMETE
• (aser performance parameters a1ect plasma generation and thmachining.
• Parameters that a1ect plasma generation are
C. Pulse repetition rate ) probabilit of formation of plasma depepeak po+er intensit +hich in turn depend of ratio of a$g.
and laser freuenc.
. Plasma discharge duration
. Polari-ation state
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• Micro channels are generated b o$erlapping of adEacent crater
• The degree of o$erlapping craters is determined b feed rate &
dimensions
• !ingle pass micro channels are basic blocks in micromachining
• ' features can be generated b lateral o$erlapping of multipa
channels.
MACHINING MICROCHANNELS
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• Able to machine opticall transparent and re;ecti$e surfaces
•
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CONCLUSIONS
• (IPMM is a tool less , multimaterial micromanufacturing proces