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E. Baake: 12-05-2016
EPM Academy
Webinar May 12, 2016
1
Physical and technical basics of
induction melting processes
Egbert Baake
Institute of Electrotechnology
Leibniz University of Hannover
Hannover / Germany
E. Baake: 12-05-2016
2
Outline
 Introduction
 Physical principles of induction melting
 Electromagnetic shaping and stirring
 Process simulation
 Power balance and efficiency
 Classical applications
 New developments
 Conclusions
E. Baake: 12-05-2016
3
Induction Melting:
Multifunctional Applications
E. Baake: 12-05-2016
4
Industrial process requirements for
melting in induction furnaces
 Mixing and homogenisation
of the entire melt
 Homogenisation of the
temperature, avoiding of
local overheating, but realizing of
sufficient superheating of the
entire melt
 Intensive stirring at the melt
surface (melting of small-sized
scrap)
 Avoiding of erosion and clogging
of the ceramic lining
 Avoiding of melt instabilities,
splashing or pinching
 Intensive stirring for cleaning or
degassing of the melt
E. Baake: 12-05-2016
5
Why induction technologies for
melting processing solutions?
Heat can be generated within the material
High energy density and fast processing if required
High temperature
if required
Homogeneous temperature distribution in the melt
High efficiency
Low specific energy consumption
High reliability
Low thermal inertia Less environmental impact
Clean melting in any atmosphere
Electromagnetic stirring
High level of automation
Reproducible process
conditions
Good integration in
the production line
Electromagnetic processing
High reliability
Electromagnetic shaping
E. Baake: 12-05-2016
electro-
magnetic field
velocity field temperature field
free surface shape
liquid-solid
interface
Physical correlations in induction
melting processes processes
alloy composition
non-linear
material properties
6
E. Baake: 12-05-2016
7
Principle of induction heating Example: Induction heating of a tube
Source: RWE-Information
Induktive Erwärmung
Principle of induction heating
Eddy currents
E. Baake: 12-05-2016
J: Stromdichte
J
8
Current density distribution in a
cylindrical workpiece (approximation)
Electromagnetic penetration depth
Source: RWE-Information Induktive Erwärmung
Current density distribution and skin effect
With: ρ = spec. electrical resistance
μ = permeability
f = frequency
J: current density
E. Baake: 12-05-2016
melt
steel-
construction
concrete-ring
meniscus
melt flow
crucible
induction
coil
magnetic
yoke
9
Induction furnaces for melting
Induction crucible furnace Induction channel furnace
 Used mainly for melting
 Medium high efficiency
 Operating frequency: 50 ... 1000 Hz
 Used mainly for holding and pouring
 High efficiency
 Operating frequency: 50 Hz, 60 Hz
Source: RWE-Information Prozesstechnik
thermal
isolation
magnetic
yoke
inductor
channel
furnace
vessel
refractory
melt
induction
coil
E. Baake: 12-05-2016
10
Scheme of an induction crucible furnace
melt
steel-
Construction
meniscus
melt flow
crucible
induction coil
magnetic yoke
E. Baake: 12-05-2016
11
Example of medium frequency induction crucible
furnace: 12 t/9,3 MW/250 Hz
source: ABB Industrietechnik AG
E. Baake: 12-05-2016
12
Meniscus shape and melt flow of the
crucible induction furnace
E. Baake: 12-05-2016
13
Meniscus shape and melt flow of the
crucible induction furnace
Inductor current: J1
E. Baake: 12-05-2016
14
Meniscus shape and melt flow of the
crucible induction furnace
Magnetic field: B
Inductor current: J1
E. Baake: 12-05-2016
15
Meniscus shape and melt flow of the
crucible induction furnace
Magnetic field: B
Inductor current: J1
Induced current
density in the melt:J2
E. Baake: 12-05-2016
16
Meniscus shape and melt flow of the
crucible induction furnace
Magnetic field: B
Inductor current: J1
Induced current
density in the melt:J2
Electromagnetic
force density:
F = J2 x B
E. Baake: 12-05-2016
17
Meniscus shape and melt flow of the
crucible induction furnace
Magnetic field: B
Inductor current: J1
Induced current
density in the melt:J2
Electromagnetic
force density:
F = J2 x B
Melt flow
pattern
E. Baake: 12-05-2016
18
Spec. kinetic energy of turbulence:
k = ½ (v´x1
2 + v´x2
2 + v´x3
2)
local melt flow velocity in
dependence on time
Shared in:
1. Time averaged flow velocity
 convective heat and mass
transfer
2. Instationary fluctuations
and oscillations
 turbulent heat and mass
transfer
Characteristics of turbulent flow in
induction furnaces
Vmax ≈ 20 cm/s
E. Baake: 12-05-2016
19
Influence of power and frequency on the melt
movement
melt
steel-
construction
concrete-ring
meniscus
melt flow
crucible
induction coil
magnetic
yoke
Velocity v of the melt flow is
proportional to the inductor
current I:
v ~ I for const. frequency f
and therefore proportional to
the square root of the spec.
power in the melt PS:
for const. frequency fSPv~
The height of the meniscus:
fPKh SÜ ⋅=
Melt flow velocity v is
proportional to:
0,4
S f1Pv ⋅~
E. Baake: 12-05-2016
20
Meniscus shape and melt flow in dependence on the filling level
filling level 80% filling level 100% filling level 120%
filling level: height of the melt when power is switched off relating to the upper end of active coil
E. Baake: 12-05-2016
Numerical simulation
approach
r << λEM
Harmonic
EM field
Alloy shape
Alloy HD
movement
Secondary
EM field
Steady part of EM force is
calculated for fixed free surface
shape
Volume of Fluid
numerical technique
for calculation of
two-phase fluid
hydrodynamics.
VF = 0 – phase #1 (air);
VF = 1 – phase #2 (melt);
0 < VF < 1 – free surface
intersects mesh element.
Unsteady Reynolds
Averaged Navier Stokes
equation for
incompressible fluid
with k – ω SST isotropic
turbulence description and
0
( )
0
ef ef
ROT
B B
f
µ
⋅∇ ⋅
=
 

2
2
HD
v
p ρ=
0 0Rem r vσµ=
0
2
EMδ
µ σω
=
2
0
04
EM
B
p
µ
=

qvol = 0
FEM –
Ansys Classic
FVM –
FLUENT and CFXReciprocal interaction
Rem << ω
˄
21
E. Baake: 12-05-2016
RANS (k-ε model)
• Whole energy spectrum is modelled
• Relatively low mesh resolution
requirements
• Steady-state simulations
Direct Numerical Simulation (DNS)
• All scales are resolved directly
• Very high requirements for
computational resources
• Simulations of industrial installations
are impossible
Large Eddy Simulation (LES)
• Large scales are resolved directly while only small
scales are modelled
• Relatively high mesh resolution requirements
• Transient 3D simulations
CFD problem
Re ≥ 104
Numerical simulation of CFD problems
Mesh
22
E. Baake: 12-05-2016
23
Time-averaged flow pattern [m/s] (3D-transient LES)
P = 4 540 KW
Hind = 1.33 m
Rcr = 0.49 m
3D hydrodynamic model of an industrial
induction crucible furnace melting cast iron
E. Baake: 12-05-2016
24
Cross-section of the transient
melt flow [m/s]
3D transient simulation of the melt flow of an industrial
induction crucible furnace using LES model
Length-section of the transient
melt flow [m/s]
E. Baake: 12-05-2016
25
Inductor efficiency of a cylindrical arrangement of inductor and workpiece
as function of workpiece diameter to penetration depth ratio
Source: RWE-Information
Induktive Erwärmung
Electrical efficiency of induction crucible
furnace
steel 20°C, μr=100, ρ=0.13
steel 400°C, μr=30, ρ=0.45
graphite 200…1000°C, ρ=10
steel 1000°C, μr=1, ρ=1.2
stainless steel 900°C, μr=1, ρ=1.2
stainless steel 20°C, μr=1, ρ=0.8
aluminium 100°C, ρ=0.038
copper 100°C, ρ=0.022
workpiece diameter / penetration depth
E. Baake: 12-05-2016
26
75%
4700 kW
390 kWh/t
1%
60 kW
15%
940 kW
1,5%
95 kW
3%
190 kW
1,5%
95 kW
100%
6270 kW
520 kWh/t
3%
190 kW
Trans-
former
Converter
Capacitor
bus bars
Induction
coil
Furnace
Construction
Heat
Losses
Energy balance for a medium frequency (MF) induction
crucible furnace for melting of grey cast iron (example)
E. Baake: 12-05-2016
27
Induction channel furnace: main features
 Joule heat and Lorentz forces
are generated in the melt of
the inductor channel
 heat transport from the inductor
channel to the furnace vessel is
important
thermal
isolation
magnetic
yoke
inductor
channel
furnace
vessel
refractory
melt
induction
coil
Primary and secondary current
E. Baake: 12-05-2016
28
3D electromagnetic and fluid-dynamic model for ICF
(examples)
~ 0.8 m
throat
Iron yoke
induction
coil
channel
cooling
shield
electromagnetic model
fluiddynamic model
channel
vessel inductor
throat
E. Baake: 12-05-2016
Distribution of the electromagnetic force density and melt flow in
the cross section of the channel
29
EM-force density Time averaged melt flow distribution
E. Baake: 12-05-2016
30
Kraftdichteverteilung Melt flow (Simulation)Melt flow (Measurement)
Distribution of the electromagnetic force density and melt
flow in the cross section of the channel
E. Baake: 12-05-2016
31
3D-simulation of the melt flow velocity in the
induction channel furnace
E. Baake: 12-05-2016
Channel of a double loop induction channel furnace for
melting of copper after solidification of the melt
32
„Solidified“
flow eddies structure
Complete channel
Part of the channel
E. Baake: 12-05-2016
3D transient result of the temperature distribution
33
Original design with symmetrical
channel: power: 240 kW Overheating ΔT: 50 K
E. Baake: 12-05-2016
34
melt with
meniscus
shape
crucible
segment
inductor
bottom
slit
skull
current
melt flow
EM-forces
heat conduction
radiation
(water cooled)
(water cooled)
(water cooled)
Features of the Induction Furnace
with Cold Crucible
 slitted crucible to realize
efficient electromagnetic
transparency
 free melt surface and
intensive melt stirring,
based on electromagnetic
forces
 water cooled bottom and
crucible segments leads to
solid layer (skull)
 heat losses by radiation
and conduction depending
on the meniscus shape
E. Baake: 12-05-2016
35
Melting in the Induction Furnace with Cold Crucible (IFCC)
 High reactive and high
purity materials, e.g. TiAl
 Melting, alloying, over-
heating and casting
in one process
 Good homogenization
of the melt caused by
electromagnetic stirring
 Overheating temperature
is the key-parameter of the
process
E. Baake: 12-05-2016
36
Principle of induction skull melting technology
Intensive cooling of inductor
and bottom
 formation of a skull
 skull protects against impurities
layer of
initial material
water-cooled inductor
skull
melt
water-cooled bottom
magnetic field
Advantages of induction
skull melting
High process temperatures
High power density
High purity of the melt
and the final product
High efficiency
Process can be realized
in different gas atmospheres
or in vacuum
Compact melting equipment
E. Baake: 12-05-2016
37
Electromagnetic levitation melting (ELM)
Features:
• contactless melting process
• no reaction with crucible
• high purity of the molten material
• high temperature of the melt
• high efficiency
• mixing and homogenization of the melt
• defined fast solidification due to maximal
under cooling of the melt is possible
Applications:
• precision casting of special alloys
• medicine and dental applications, e.g. implantats
• aeronautics, e.g. precision casting components
• investigation of new material compositions
• determination of material properties
• investigations of under-cooled melts
E. Baake: 12-05-2016
New setup for EM-levitation melting
Ief = 1.1 kA, f1 = 30 kHz, f2 = 40 kHz
Yoke: μr = 5000, Bef < 250 mT
Horizontal magnetic fields generated by
two pairs of induction coils with different
frequencies
Magnetic flux guiding system
500 g
38
E. Baake: 12-05-2016
39
Time-averaged flow
v, m/s
Supporting Lorentz force forms a single
torroidal vortex with an upward directed
flow on the z-axis
E. Baake: 12-05-2016
EM levitation melting of aluminum sample
m = 500 g
40
E. Baake: 12-05-2016
41
Induction melting processes – Summary
 melt homogenisation due to melt stirring
 small material losses because no local overheating
 exact adjustment of the alloy composition
 exact temperature control
 easy automatic process control
 high quality of the melt
 high throughput due to fast heating up speed
 high furnaces efficiency
 relatively simple handling
 good energy control
 friendly working conditions
 environmental friendly (small emission of dust, no exhaustion gas)
 new future oriented technologies, like skull melting and levitation melting
E. Baake: 12-05-2016
42
Thank you very much
for your attention!

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Physical and technical basics of induction melting processes

  • 1. E. Baake: 12-05-2016 EPM Academy Webinar May 12, 2016 1 Physical and technical basics of induction melting processes Egbert Baake Institute of Electrotechnology Leibniz University of Hannover Hannover / Germany
  • 2. E. Baake: 12-05-2016 2 Outline  Introduction  Physical principles of induction melting  Electromagnetic shaping and stirring  Process simulation  Power balance and efficiency  Classical applications  New developments  Conclusions
  • 3. E. Baake: 12-05-2016 3 Induction Melting: Multifunctional Applications
  • 4. E. Baake: 12-05-2016 4 Industrial process requirements for melting in induction furnaces  Mixing and homogenisation of the entire melt  Homogenisation of the temperature, avoiding of local overheating, but realizing of sufficient superheating of the entire melt  Intensive stirring at the melt surface (melting of small-sized scrap)  Avoiding of erosion and clogging of the ceramic lining  Avoiding of melt instabilities, splashing or pinching  Intensive stirring for cleaning or degassing of the melt
  • 5. E. Baake: 12-05-2016 5 Why induction technologies for melting processing solutions? Heat can be generated within the material High energy density and fast processing if required High temperature if required Homogeneous temperature distribution in the melt High efficiency Low specific energy consumption High reliability Low thermal inertia Less environmental impact Clean melting in any atmosphere Electromagnetic stirring High level of automation Reproducible process conditions Good integration in the production line Electromagnetic processing High reliability Electromagnetic shaping
  • 6. E. Baake: 12-05-2016 electro- magnetic field velocity field temperature field free surface shape liquid-solid interface Physical correlations in induction melting processes processes alloy composition non-linear material properties 6
  • 7. E. Baake: 12-05-2016 7 Principle of induction heating Example: Induction heating of a tube Source: RWE-Information Induktive Erwärmung Principle of induction heating Eddy currents
  • 8. E. Baake: 12-05-2016 J: Stromdichte J 8 Current density distribution in a cylindrical workpiece (approximation) Electromagnetic penetration depth Source: RWE-Information Induktive Erwärmung Current density distribution and skin effect With: ρ = spec. electrical resistance μ = permeability f = frequency J: current density
  • 9. E. Baake: 12-05-2016 melt steel- construction concrete-ring meniscus melt flow crucible induction coil magnetic yoke 9 Induction furnaces for melting Induction crucible furnace Induction channel furnace  Used mainly for melting  Medium high efficiency  Operating frequency: 50 ... 1000 Hz  Used mainly for holding and pouring  High efficiency  Operating frequency: 50 Hz, 60 Hz Source: RWE-Information Prozesstechnik thermal isolation magnetic yoke inductor channel furnace vessel refractory melt induction coil
  • 10. E. Baake: 12-05-2016 10 Scheme of an induction crucible furnace melt steel- Construction meniscus melt flow crucible induction coil magnetic yoke
  • 11. E. Baake: 12-05-2016 11 Example of medium frequency induction crucible furnace: 12 t/9,3 MW/250 Hz source: ABB Industrietechnik AG
  • 12. E. Baake: 12-05-2016 12 Meniscus shape and melt flow of the crucible induction furnace
  • 13. E. Baake: 12-05-2016 13 Meniscus shape and melt flow of the crucible induction furnace Inductor current: J1
  • 14. E. Baake: 12-05-2016 14 Meniscus shape and melt flow of the crucible induction furnace Magnetic field: B Inductor current: J1
  • 15. E. Baake: 12-05-2016 15 Meniscus shape and melt flow of the crucible induction furnace Magnetic field: B Inductor current: J1 Induced current density in the melt:J2
  • 16. E. Baake: 12-05-2016 16 Meniscus shape and melt flow of the crucible induction furnace Magnetic field: B Inductor current: J1 Induced current density in the melt:J2 Electromagnetic force density: F = J2 x B
  • 17. E. Baake: 12-05-2016 17 Meniscus shape and melt flow of the crucible induction furnace Magnetic field: B Inductor current: J1 Induced current density in the melt:J2 Electromagnetic force density: F = J2 x B Melt flow pattern
  • 18. E. Baake: 12-05-2016 18 Spec. kinetic energy of turbulence: k = ½ (v´x1 2 + v´x2 2 + v´x3 2) local melt flow velocity in dependence on time Shared in: 1. Time averaged flow velocity  convective heat and mass transfer 2. Instationary fluctuations and oscillations  turbulent heat and mass transfer Characteristics of turbulent flow in induction furnaces Vmax ≈ 20 cm/s
  • 19. E. Baake: 12-05-2016 19 Influence of power and frequency on the melt movement melt steel- construction concrete-ring meniscus melt flow crucible induction coil magnetic yoke Velocity v of the melt flow is proportional to the inductor current I: v ~ I for const. frequency f and therefore proportional to the square root of the spec. power in the melt PS: for const. frequency fSPv~ The height of the meniscus: fPKh SÜ ⋅= Melt flow velocity v is proportional to: 0,4 S f1Pv ⋅~
  • 20. E. Baake: 12-05-2016 20 Meniscus shape and melt flow in dependence on the filling level filling level 80% filling level 100% filling level 120% filling level: height of the melt when power is switched off relating to the upper end of active coil
  • 21. E. Baake: 12-05-2016 Numerical simulation approach r << λEM Harmonic EM field Alloy shape Alloy HD movement Secondary EM field Steady part of EM force is calculated for fixed free surface shape Volume of Fluid numerical technique for calculation of two-phase fluid hydrodynamics. VF = 0 – phase #1 (air); VF = 1 – phase #2 (melt); 0 < VF < 1 – free surface intersects mesh element. Unsteady Reynolds Averaged Navier Stokes equation for incompressible fluid with k – ω SST isotropic turbulence description and 0 ( ) 0 ef ef ROT B B f µ ⋅∇ ⋅ =    2 2 HD v p ρ= 0 0Rem r vσµ= 0 2 EMδ µ σω = 2 0 04 EM B p µ =  qvol = 0 FEM – Ansys Classic FVM – FLUENT and CFXReciprocal interaction Rem << ω ˄ 21
  • 22. E. Baake: 12-05-2016 RANS (k-ε model) • Whole energy spectrum is modelled • Relatively low mesh resolution requirements • Steady-state simulations Direct Numerical Simulation (DNS) • All scales are resolved directly • Very high requirements for computational resources • Simulations of industrial installations are impossible Large Eddy Simulation (LES) • Large scales are resolved directly while only small scales are modelled • Relatively high mesh resolution requirements • Transient 3D simulations CFD problem Re ≥ 104 Numerical simulation of CFD problems Mesh 22
  • 23. E. Baake: 12-05-2016 23 Time-averaged flow pattern [m/s] (3D-transient LES) P = 4 540 KW Hind = 1.33 m Rcr = 0.49 m 3D hydrodynamic model of an industrial induction crucible furnace melting cast iron
  • 24. E. Baake: 12-05-2016 24 Cross-section of the transient melt flow [m/s] 3D transient simulation of the melt flow of an industrial induction crucible furnace using LES model Length-section of the transient melt flow [m/s]
  • 25. E. Baake: 12-05-2016 25 Inductor efficiency of a cylindrical arrangement of inductor and workpiece as function of workpiece diameter to penetration depth ratio Source: RWE-Information Induktive Erwärmung Electrical efficiency of induction crucible furnace steel 20°C, μr=100, ρ=0.13 steel 400°C, μr=30, ρ=0.45 graphite 200…1000°C, ρ=10 steel 1000°C, μr=1, ρ=1.2 stainless steel 900°C, μr=1, ρ=1.2 stainless steel 20°C, μr=1, ρ=0.8 aluminium 100°C, ρ=0.038 copper 100°C, ρ=0.022 workpiece diameter / penetration depth
  • 26. E. Baake: 12-05-2016 26 75% 4700 kW 390 kWh/t 1% 60 kW 15% 940 kW 1,5% 95 kW 3% 190 kW 1,5% 95 kW 100% 6270 kW 520 kWh/t 3% 190 kW Trans- former Converter Capacitor bus bars Induction coil Furnace Construction Heat Losses Energy balance for a medium frequency (MF) induction crucible furnace for melting of grey cast iron (example)
  • 27. E. Baake: 12-05-2016 27 Induction channel furnace: main features  Joule heat and Lorentz forces are generated in the melt of the inductor channel  heat transport from the inductor channel to the furnace vessel is important thermal isolation magnetic yoke inductor channel furnace vessel refractory melt induction coil Primary and secondary current
  • 28. E. Baake: 12-05-2016 28 3D electromagnetic and fluid-dynamic model for ICF (examples) ~ 0.8 m throat Iron yoke induction coil channel cooling shield electromagnetic model fluiddynamic model channel vessel inductor throat
  • 29. E. Baake: 12-05-2016 Distribution of the electromagnetic force density and melt flow in the cross section of the channel 29 EM-force density Time averaged melt flow distribution
  • 30. E. Baake: 12-05-2016 30 Kraftdichteverteilung Melt flow (Simulation)Melt flow (Measurement) Distribution of the electromagnetic force density and melt flow in the cross section of the channel
  • 31. E. Baake: 12-05-2016 31 3D-simulation of the melt flow velocity in the induction channel furnace
  • 32. E. Baake: 12-05-2016 Channel of a double loop induction channel furnace for melting of copper after solidification of the melt 32 „Solidified“ flow eddies structure Complete channel Part of the channel
  • 33. E. Baake: 12-05-2016 3D transient result of the temperature distribution 33 Original design with symmetrical channel: power: 240 kW Overheating ΔT: 50 K
  • 34. E. Baake: 12-05-2016 34 melt with meniscus shape crucible segment inductor bottom slit skull current melt flow EM-forces heat conduction radiation (water cooled) (water cooled) (water cooled) Features of the Induction Furnace with Cold Crucible  slitted crucible to realize efficient electromagnetic transparency  free melt surface and intensive melt stirring, based on electromagnetic forces  water cooled bottom and crucible segments leads to solid layer (skull)  heat losses by radiation and conduction depending on the meniscus shape
  • 35. E. Baake: 12-05-2016 35 Melting in the Induction Furnace with Cold Crucible (IFCC)  High reactive and high purity materials, e.g. TiAl  Melting, alloying, over- heating and casting in one process  Good homogenization of the melt caused by electromagnetic stirring  Overheating temperature is the key-parameter of the process
  • 36. E. Baake: 12-05-2016 36 Principle of induction skull melting technology Intensive cooling of inductor and bottom  formation of a skull  skull protects against impurities layer of initial material water-cooled inductor skull melt water-cooled bottom magnetic field Advantages of induction skull melting High process temperatures High power density High purity of the melt and the final product High efficiency Process can be realized in different gas atmospheres or in vacuum Compact melting equipment
  • 37. E. Baake: 12-05-2016 37 Electromagnetic levitation melting (ELM) Features: • contactless melting process • no reaction with crucible • high purity of the molten material • high temperature of the melt • high efficiency • mixing and homogenization of the melt • defined fast solidification due to maximal under cooling of the melt is possible Applications: • precision casting of special alloys • medicine and dental applications, e.g. implantats • aeronautics, e.g. precision casting components • investigation of new material compositions • determination of material properties • investigations of under-cooled melts
  • 38. E. Baake: 12-05-2016 New setup for EM-levitation melting Ief = 1.1 kA, f1 = 30 kHz, f2 = 40 kHz Yoke: μr = 5000, Bef < 250 mT Horizontal magnetic fields generated by two pairs of induction coils with different frequencies Magnetic flux guiding system 500 g 38
  • 39. E. Baake: 12-05-2016 39 Time-averaged flow v, m/s Supporting Lorentz force forms a single torroidal vortex with an upward directed flow on the z-axis
  • 40. E. Baake: 12-05-2016 EM levitation melting of aluminum sample m = 500 g 40
  • 41. E. Baake: 12-05-2016 41 Induction melting processes – Summary  melt homogenisation due to melt stirring  small material losses because no local overheating  exact adjustment of the alloy composition  exact temperature control  easy automatic process control  high quality of the melt  high throughput due to fast heating up speed  high furnaces efficiency  relatively simple handling  good energy control  friendly working conditions  environmental friendly (small emission of dust, no exhaustion gas)  new future oriented technologies, like skull melting and levitation melting
  • 42. E. Baake: 12-05-2016 42 Thank you very much for your attention!