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comparative study for mrr on die-sinking edm using electrode ... - ijater

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Internati<strong>on</strong>al Journal of Advanced Technology & Engineering Research (IJATER)<br />

in <strong>on</strong>ly <strong>on</strong>e directi<strong>on</strong>, resulting in properties or “grain” similar<br />

to wood, that varied relative to the directi<strong>on</strong> of pressing.<br />

As an outgrowth of the space program, methods were developed<br />

to isostatically press graphite such that its properties<br />

became “isotropic”, that is the same in all directi<strong>on</strong>s. All<br />

high quality, high per<str<strong>on</strong>g>for</str<strong>on</strong>g>mance graphites are now manufactured<br />

this way. After compacting, the “green” compacted<br />

material undergoes a series of thermal treatments that c<strong>on</strong>vert<br />

the Carb<strong>on</strong> to graphite. Graphite has certain properties<br />

quite different than wrought metal based <strong>electrode</strong> materials:<br />

• Graphite has an extremely high melting point. Actually,<br />

graphite does not melt at all, but sublimes directly from a<br />

solid to a gas (just as the Carb<strong>on</strong> Dioxide in dry ice) at a<br />

temperature thousands of degrees higher than the melting<br />

point of Copper. This resistance to temperature makes graphite<br />

an ideal <strong>electrode</strong> material.<br />

• Graphite has significantly lower mechanical strength properties<br />

than metallic <strong>electrode</strong> materials. It is neither as hard,<br />

as str<strong>on</strong>g, nor as stiff as metallic <strong>electrode</strong> materials. However,<br />

since the EDM process is <strong>on</strong>e of relatively low macro<br />

mechanical <str<strong>on</strong>g>for</str<strong>on</strong>g>ces, these property differences are not often<br />

significant. Due to the significant differences between metallic<br />

<strong>electrode</strong>s and graphite, there are certain properties,<br />

unique to graphite that are comm<strong>on</strong>ly specified and c<strong>on</strong>trolled.<br />

Fig. 1 Die-Sinker EDM Set-up<br />

1.3 Characteristics of <strong>die</strong>-Sinker<br />

EDM<br />

The characteristics necessary <str<strong>on</strong>g>for</str<strong>on</strong>g> <strong>die</strong>-sinker EDM are given<br />

below in the table<br />

Table 1 Process Parameters of Die-Sinker EDM Process<br />

Mechanism of Processes C<strong>on</strong>trolled erosi<strong>on</strong> (melting<br />

Spark gap<br />

Spark frequency<br />

Peak voltage across the gap<br />

Metal removal rate (max.)<br />

Specific power c<strong>on</strong>sumpti<strong>on</strong><br />

Dielectric fluid<br />

Tool material<br />

Machine-able materials<br />

Shapes that can be produced<br />

Limitati<strong>on</strong>s<br />

and evaporati<strong>on</strong>)<br />

0.010 – 0.500 mm<br />

200 – 500 KHz<br />

30 – 250 V<br />

5000 mm3/min.<br />

2 – 10 W/mm3/min.<br />

EDM oil, Kerosene liquid,<br />

Silic<strong>on</strong> oil, Dei<strong>on</strong>ised water<br />

etc.<br />

Copper, Brass, Graphite, Ag-<br />

W alloy, Cu-W alloy<br />

All c<strong>on</strong>ducting metals and<br />

alloys<br />

Micro holes, Narrow slots<br />

High energy c<strong>on</strong>sumpti<strong>on</strong>,<br />

can’t machined n<strong>on</strong>c<strong>on</strong>ducting<br />

materials<br />

2. Literature Review<br />

In this paper few selected research paper related to Diesinker<br />

EDM with effect of metal MRR, surface roughness<br />

(SR), workpiece material<br />

2.1 Workpiece and tool material-<br />

Dhar and Purohit evaluates the effect of current (c), pulse<strong>on</strong><br />

time (p) and air gap voltage (v) <strong>on</strong> MRR, TWR, ROC of<br />

EDM with Al–4Cu–6Si alloy–10 wt. % SiCP composites.<br />

This experiment can be <strong>using</strong> the PS LEADER ZNC EDM<br />

machine and a cylindrical brass <strong>electrode</strong> of 30 mm diameter.<br />

And three factors, three levels full factorial design was<br />

<strong>using</strong> and analyzing the results. A sec<strong>on</strong>d order, n<strong>on</strong>-linear<br />

mathematical model has been developed <str<strong>on</strong>g>for</str<strong>on</strong>g> establishing the<br />

relati<strong>on</strong>ship am<strong>on</strong>g machining parameters. The significant of<br />

the models were checked <strong>using</strong> technique ANOVA and finding<br />

the MRR, TWR and ROC increase significant in a n<strong>on</strong>linear<br />

fashi<strong>on</strong> with increase in current.<br />

Karthikeyan et .al has presented the mathematical molding<br />

of EDM with aluminum-silic<strong>on</strong> carbide particulate composites.<br />

Mathematical equati<strong>on</strong> is Y=f(V, I, T). And the effect<br />

of MRR, TWR, SR with Process parameters taken in to<br />

c<strong>on</strong>siderati<strong>on</strong> were the current (I), the pulse durati<strong>on</strong> (T) and<br />

the percent volume fracti<strong>on</strong> of SiC (25 μ size). A three level<br />

full factorial design was choosing. Finally the significant of<br />

the models were checked <strong>using</strong> the ANOVA. The MRR was<br />

found to decrease with an increase in the percent volume of<br />

SiC, whereas the TWR and the surface roughness increase<br />

with an increase in the volume of Sic.<br />

B.Mohan and Satyanarayana evoluti<strong>on</strong> the of effect of the<br />

EDM Current, <strong>electrode</strong> marital polarity, pulse durati<strong>on</strong> and<br />

rotati<strong>on</strong> of <strong>electrode</strong> <strong>on</strong> metal removal rate, TWR, and SR,<br />

and the EDM of Al-Sic with 20-25 vol. % SiC, Polarity of<br />

the <strong>electrode</strong> and volume present of SiC, the MRR increased<br />

with increased in discharge current and specific current it<br />

decreased with increasing in pulse durati<strong>on</strong>. Increasing the<br />

ISSN NO: 2250-3536 VOLUME 2, ISSUE 2, MAY 2012 171

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