Abstract
In micro-electrical discharge machining (micro-EDM) using the non-hollow circular cross-section tool electrode with the side flushing technique, when the aspect ratio of machined micro-hole is expected to be further increased, the discharge debris expelling speed and the working fluid renewal efficiency are weakened, which hinders the improvement of machining efficiency and accuracy with increased machining depth. In order to reveal the flow behavior of the working fluid in the micro-EDM gap, so as to realize the high-precision and high-efficiency machining of micro-hole with high aspect ratio, a three-phase flow simulation model of fluid, bubble, and debris is established in Fluent under the ideal assumption that the spark discharges occur continuously to generate high-pressure bubbles. The simulation results show that when the boundary condition of the flushing pressure at the side gap entrance is set to 0, the pressure wave emitted when the high-pressure bubble expands, which is formed by the instantaneous gasification of the working fluid between electrodes under high temperature, is the source of pneumatic force that drives the working fluid flow at the micron scale. Affected by the gap flow channel structure and the viscous resistance from inner wall, the flow velocity direction of the fluid dragging the discharge debris to rise up and expel will change, forming a dynamic alternation process of flowing into and out of the side machining gap entry. As the machining depth increases, due to the energy attenuation of the pressure wave propagating from the bottom gap to the side gap entrance, the expelling speed of the discharge debris decreases exponentially at the side gap entrance, resulting in the reduced machining efficiency and accuracy. However, when the simulated bubble generation frequency is increased to the megahertz level, the expelling efficiency of debris has a step-like improvement. The continuous and high-frequency generation of high-pressure bubbles can maintain a high pressure gradient in the bottom gap, and the discharge debris is able to continuously move upward without falling back to accumulate in the bottom gap, which is beneficial to the stable and smooth machining process, realizing the high-precision and high-efficiency machining of micro-hole with high aspect ratio.
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Abbreviations
- A 0 :
-
Initial amplitude of pressure wave, m
- A l :
-
Amplitude of pressure wave after propagation distance l, m
- A S :
-
Flow area of side machining gap cross-section, μm2
- c :
-
Constant
- c 1 :
-
Sound velocity of liquid phase, m/s
- c wave :
-
Transmission velocity of pressure wave in liquid, m/s
- d 1 :
-
Diameter of tool electrode, μm
- d 2 :
-
Diameter of machined micro-hole, μm
- dp:
-
Change of fluid pressure, Pa
- dT:
-
Change of fluid temperature, K
- dv:
-
Change of fluid velocity, m/s
- dV:
-
Symbol of volume integral
- dρ:
-
Change of fluid density, kg/m3
- d p :
-
Diameter of debris, μm
- d e :
-
Equivalent diameter of side machining gap cross-section, μm
- E e :
-
Energy in the energy equation, J
- E wave :
-
Energy of pressure waves, J
- F buoy :
-
Buoyancy on bubbles, N
- F disjoin :
-
Disjoining pressure between bubble and contact wall, N
- F drag :
-
Drag force exerted on debris by surrounding fluid, N
- F pressure :
-
Pressure gradient force exerted on debris by surrounding fluid, N
- F saffman :
-
Saffman lift force exerted on debris by surrounding fluid, N
- F σ :
-
Surface tension of the fluid, N
- g :
-
Gravitational acceleration, m/s2
- h v :
-
Heat of vaporization, kJ/kg
- I(t):
-
Discharge current, A
- K qp :
-
Factor of phase transition intensity
- K eff :
-
Effective thermal conductivity coefficient in energy equation
- k G :
-
Gaussian heat coefficient
- L e :
-
Latent heat of vaporization, kJ/kg
- l :
-
Distance between any two points in machining gap, μm
- l c :
-
Capillary length of the dielectric fluid, m
- l d :
-
Machining depth of micro-holes, mm
- l f :
-
Liquid film thickness between bubbles and contact wall, nm
- l g :
-
Machining gap width, μm
- m p :
-
Mass of debris, kg
- \({\dot{\mathrm{m}}}_{\mathrm{pq}}\) :
-
Mass transfer velocity from liquid phase to gas phase, kg/s
- \({\dot{\mathrm{m}}}_{\mathrm{qp}}\) :
-
Mass transfer velocity from gas phase to liquid phase, kg/s
- N :
-
Number of initial generated bubbles
- n :
-
Number of particles released at one time
- n v :
-
Unit normal vector of fluid interface
- p :
-
Shared pressure of fluid phase, Pa
- p 0 :
-
Atmospheric pressure, Pa
- p flush :
-
Lateral flushing pressure, Pa
- p q :
-
Pressure of gas phase, Pa
- p sat :
-
Saturated vapor pressure, Pa
- q(r,t):
-
Gaussian heat, J
- Reb :
-
Fluid Reynolds number in bottom machining gap
- Res :
-
Fluid Reynolds number in side machining gap
- R(t):
-
Discharge channel radius, μm
- r :
-
Distance from discharge center, μm
- r b :
-
Bubble radius, μm
- r bi :
-
Initial bubble radius, μm
- \({\mathrm{S}}_{{\mathrm{a}}_{\mathrm{q}}}\) :
-
Source term in Continuity Equation, kg/m3-s
- S h :
-
Source term in Energy Equation, W/m3
- T e :
-
Temperature in Energy Equation, K
- T nuc :
-
Nucleation temperature, K
- T sat :
-
Saturated temperature, K
- t c :
-
Time of bubble collapse, μs
- t on :
-
Pulse width of the pulsed power supply, μs
- t total :
-
Total time of micro-hole machining, s
- U(t):
-
Discharge voltage, V
- V c :
-
Volume of single grid cell, μm3
- V crater :
-
Volume of single discharge crater, μm3
- V debris :
-
Volume of single debris, μm3
- \({\mathrm{V}}_{\mathrm{f}}^{\mathrm{n+1}}\) :
-
Volumetric flux on surface through normal velocity vector at n + 1 time step, m3/s
- V total :
-
Total volume of removed workpiece material, m3
- v :
-
Shared velocity of fluid phase, m/s
- v b :
-
Initial expansion velocity of bubbles, m/s
- v f :
-
Lateral flushing speed, m/s
- v p :
-
Movement velocity of debris, m/s
- v q :
-
Movement velocity of gas interface, m/s
- v s :
-
Fluid flow speed in side machining gap, m/s
- v up :
-
Rising speed of bubbles in narrow gap, nm/s
- α q :
-
Volume fraction of gas phase
- \({\alpha }_{\mathrm{q}}^{\mathrm{n}}\) :
-
Volume fraction of gas phase at n time step
- \({\alpha }_{\mathrm{q}}^{\mathrm{n+1}}\) :
-
Volume fraction of gas phase at n + 1 time step
- ΔP :
-
Pressure loss along the side gap channel, Pa
- Δt :
-
Unit of time, s
- ΔV :
-
Material removal volume per unit time, m3
- η :
-
Pressure wave energy attenuation coefficient
- η G :
-
Gaussian heat transfer coefficient
- κ :
-
Surface curvature, m−1
- λ :
-
Pressure loss coefficient along the side gap channel
- μ :
-
Dynamic viscosity of fluid, Pa·s
- ρ :
-
Shared density of fluid phase, kg/m3
- ρ p :
-
Density of debris, kg/m3
- ρ q :
-
Density of gas phase, kg/m3
- \({\rho }_{\mathrm{q}}^{\mathrm{n}}\) :
-
Gas-phase density at n time step, kg/m3
- \({\rho }_{\mathrm{q}}^{\mathrm{n+1}}\) :
-
Gas-phase density at n + 1 time step, kg/m3
- σ :
-
Surface tension coefficient of fluid, N/m
- τ :
-
Tangential stress, Pa
- υ :
-
Kinematic viscosity of fluid, m2/s
- χ :
-
Wet perimeter of side machining gap, μm
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Funding
This research was supported by the National Natural Science Foundation of China (grant No. 92060108) and Independent Research Project of State Key Laboratory of Tribology of China (grant No. SKLT2022B08).
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Cao, P., Tong, H., Li, Y. et al. Interelectrode gas–liquid-solid three-phase flow analysis and simulation for drilling holes with high aspect ratio by micro-EDM. Int J Adv Manuf Technol 128, 5261–5276 (2023). https://doi.org/10.1007/s00170-023-12220-4
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DOI: https://doi.org/10.1007/s00170-023-12220-4