Abstract
Due to the non-isoenergetic nature of discharge pulses in resistance-capacitance (RC) based micro electrical discharge machining (μEDM), the volume of produced micro-crater by each pulse varies significantly. This fact has driven the researchers in this work to propose an electrothermal principle–based analytical model to approximate dimensional accuracies of such micro-craters. A finite element (FE) simulation considering Gaussian heat flux distribution of single discharge μEDM has been performed at significant input parameters such as discharge energy, capacitance, and open-circuit voltage and compared with analytical simulation results. Upon validation of these simulated results with experimental results, nominal dimensional inaccuracies of 2–11% for a wide range of input parameters have been noticed. This effectively predicted crater dimension from the workpiece can be incorporated in the proposed thermal modeling–based real-time tool wear monitoring and compensation system through a unique strategy, which is discussed at the end.
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Abbreviations
- μEDM:
-
Micro electrical discharge machining
- CFD:
-
Computational fluid dynamics
- DAQ:
-
Data acquisition card
- EDS:
-
Energy dispersive spectroscopy
- FE:
-
Finite element
- FD:
-
Finite difference
- MRR:
-
Material removal rate
- PD:
-
Pulse discrimination
- SR:
-
Surface roughness
- SEM:
-
Scanning electron microscopy
- TWR:
-
Tool wear rate
- V MR :
-
Actual volume removal
- V target :
-
Target volume
- VRD:
-
Volume removal per discharge
- c p :
-
Average specific heat (Jkg−1K−1.)
- C :
-
Combination of fraction energy and a fraction of molten area (Dimensionless)
- erfc :
-
Complementary error function (Dimensionless)
- E P :
-
Energy of each pulse (μJ)
- E :
-
Complete elliptic integrals of the second kind (Dimensionless)
- h c :
-
Convective heat transfer coefficient (Wm−2K)
- I a :
-
Average current (A)
- J 0 :
-
Bessel function of the first kind of zero-order (Dimensionless)
- J 1 :
-
Bessel function of the first kind of first-order (Dimensionless)
- K t :
-
Thermal conductivity of the material (Wm−1K−1)
- K :
-
Complete elliptic integrals of the first kind (Dimensionless)
- L m :
-
Latent heat of melting (kJ/kg)
- L V :
-
Latent heat of vaporization (kJ/kg)
- N p :
-
Number of actual contributing pulses (Dimensionless)
- q :
-
Heat flux (Wm−2)
- R a :
-
Heat flux radius at anode (μm)
- r :
-
Radial coordinates (μm)
- R :
-
Heat flux radius (μm)
- t :
-
Time in seconds (s)
- T :
-
Temperature (K)
- T s :
-
Solidus temperature (K)
- T l :
-
Liquids temperature (K)
- T 0 :
-
Ambient temperature (K)
- t on :
-
Pulse on time (μs)
- u :
-
Dimensionless radius (Dimensionless)
- V a :
-
Average voltage (V)
- V 0 :
-
Open circuit voltage (V)
- α :
-
Thermal diffusivity of material (m2s−1)
- λ :
-
Dummy variables (Dimensionless)
- ρ :
-
Density of material (kgm−3)
- θ :
-
Ratio of anode erosion rate (Dimensionless)
- τ :
-
Dimensionless time (Dimensionless)
- w :
-
Dimensionless depth (Dimensionless)
- z :
-
Depth or axial coordinates (μm)
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Funding
The authors received financial support from the Department of Science and Technology (DST) Govt. of India (Grant No. ECR/DST/2017/000918)
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Nadda, R., Nirala, C.K. Thermal modeling of single discharge in prospect of tool wear compensation in μEDM. Int J Adv Manuf Technol 107, 4573–4595 (2020). https://doi.org/10.1007/s00170-020-05238-5
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DOI: https://doi.org/10.1007/s00170-020-05238-5