5. Gas– Shielded Metal Arc Welding
2003
5. Gas-Shielded Metal Arc Welding
56
The difference between gas-shielded metal arc welding (GMA) and the gas tungsten arc welding process is the consumable electrode. Essentially the process is classified as metal inert gas welding (MIG) and metal active gas welding (MAG). Besides, there are gas-shielded arc welding (SG)
two more process
gas-shielded metal-arc welding (GMAW) metal inert gas welding (MIG) electrogas welding (MSGG) Narrow-gap gasshielded arc welding (MSGE)
variants, the elec-
tungsten gasshielded welding
trogas and the nar-
metal active gas welding
plasma gas metal arc welding
tungsten inert-gas welding
tungsten plasma welding
hydrogen tungsten arc welding
(MAG)
(MSGP)
(TIG)
(WP)
(WHG)
plasma jet welding
plasma arc welding
(WPS)
(WPL)
plasma jet plasma arc welding (WPSL)
gas mixture gas metalarc CO2 metal-arc welding welding (GMMA)
(MAGC)
consumable electrode
and also the gasshielded
plasma
metal arc welding, a combination of both plasma weld-
non consumable electrode
br-er5-01e.cdr
row gap welding
© ISF 2002
ing and MIG weld-
Classification of Gas-Shielded Arc Welding Processes
ing, Figure 5.1.
Figure 5.1 In contrast to TIG welding, where the electrode is normally negative in order to avoid the melting of the tungsten
wire feed unit
electrode, this effect is exploited in MIG welding, as the positive pole is
water cooling
strongly heated than the negative pole,
shielding gas control device
thus improving the melting characteris-
control switch cooling water control
tics of the feed wire. Figure 5.2 shows the principle of a
rectifier transformer
GMA welding installation. The welding power source is assembled using
welding power source
the following assembly groups: The transformer converts the mains voltage to low voltage which is subsebr-er5-02e.cdr
© ISF 2002
quently rectified. GMA Welding Installation
Figure 5.2
5. Gas-Shielded Metal Arc Welding
compact device
57 Apart from the torch cooling and the
universal device
shielding gas control, the process 5, 10 or 20m 3 to 5m 3 to 5m
control is the most important installation component. The process control ensures that once set welding data are adhered to.
mini-spool device
push-pull device
A selection of common welding installation variants is depicted in Figure 5.3, where the universal device
10, 20 or 30m
5 to 10m
with a separate wire feed housing is the most frequently
used variant in
the industry.
© ISF 2002
br-er5-03e.cdr
Types of Welding Installations
Figure 5.4 shows in detail a manually operated inert-gas shielded torch with the common swan-neck shape. A
Figure 5.3 machine torch has no handle and its shape is straight or swan-necked. The hose package contains the wire core and also supply lines for shielding gas, current and cooling water, the latter for contact tube cooling. The current is transferred to the wire electrode over the contact tube. The shielding gas
1 torch handle 2 torch neck 3 torch trigger 4 hose package 5 shielding gas nozzle 6 contact tube 7 contact tube fixture 8 insulator 9 wire core 10 wire guide tube 11 wire electrode 12 shielding gas supply 13 welding current supply
nozzle is shaped to ensure a steady gas flow in the arc space, thus protecting arc and molten pool against the atmosphere.
© ISF 2002
br-er5-04e.cdr
Manual Gas-Shielded Arc Welding Torch
Figure 5.4
5. Gas-Shielded Metal Arc Welding
58 A so-called “Two-Wire-Drive” wire
1 2
4
feed system is of the most simple de-
2
F
sign, as shown in Figure 5.5. The wire is pulled off a wire reel and fed into the hose package. The wire transport
4
4
3
roller, which shows different grooves depending on the used material, is driven by an electric motor. The counterpressure roller generates the frictional force which is needed for wire
5
feeding.
6
1 wire reel
3 wire transport roll
2 wire guide tube
4 counter pressure roll
More complicated but following the
5 wire feed roll with a V-groove for steel electrodes
same operation principle is the “Four-
6 wire feed roll with a rounded groove for aluminium br-er5-05e.cdr
© ISF 2002
Wire Feed System
Wire-Drive”, Figure 5.6. Here, the second pair of rollers guarantees higher feeding reliability by reducing
Figure 5.5 4-roller drive 4
3
the risk of wheel slip. Another design
1
3
among the wire feed drive systems is the planetary drive, where the wire is fed in axial direction by the motor. A rectilinear rotation-free wire feed motion is the outcome of the motor rota-
1
2
2
1 wire guide tube 2 drive rollers 3 counter pressure rollers 4 wire guide tube
tion and the angular offset of the drive rollers which are firmly connected to
planetary drive 3
the motor shaft. direction of rotation
Figure 5.7 depicts the metal transfer in the short arc range. During the burn-
3
ing phase of the arc, material is molten 1
and accumulates at the electrode end.
1 wire guide tube 2 roller holding device 3 drive rollers
2
br-er5-06e.cdr
The voltage drops slowly while the arc
© ISF 2002
Wire Drives
shortens. Electrode and workpiece Figure 5.6
5. Gas-Shielded Metal Arc Welding
59
make contact and a short-circuit occurs. In the short-circuit phase is the liquid electrode material drawn as result of surface tension into the molten pool. The narrowing liquid root and the welding voltage
rising current lead to a very high current time
density
that
welding current
causes a sudden evaporation of the remaining
time
1 ms 1 mm
root.
The arc is reignited. The shortarc
technique
is
particularly suitable
br-er5-07e.cdr
for
Short-Circuiting Arc Metal Transfer
and
Figure 5.7
out-of-position root
passes
welding.
The limitation of the rate of the current rise during the short-circuit phase with a choke leads to a pointed burn-off process which is smoother and clearly shows less spatter formation, Figures 5.8
In shielding gases welding current
welding current
with a high CO2 proportion a long arc is formed in the upper power range, Figure 5.9. Material time
time
transfer
is
unde-
fined and occurs as illustrated in Figlow
choke effect
br-er5-08e.cdr
medium
ures 5.13 and 5.14.
© ISF 2002
Short-circuits Choke Effect
Figure 5.8
with
very strong spatter formation
are
5. Gas-Shielded Metal Arc Welding
60
welding current
welding current
caused by the formation of very large droplets at the electrode end.
time
welding voltage
welding voltage
time
time
time br-er5-09e.cdr
© ISF 2002
br-er5-10e.cdr
© ISF 2002
Long Arc
Spray Arc
Figure 5.9
Figure 5.10
If the inert gas content of the shielding gas exceeds 80%, a spray arc forms in the upper power range, Figure 5.10. The spray arc is characterised by a non-shortcircuiting 35
C1 shielding gas composition: C1: CO2 M21: 82% Ar, 18% CO2 M23: 92% Ar, 8% O2
welding voltage
V
long arc
and
spray-like material
M21 M23
transfer. high
For
its
deposition
25
rate the spray arc 20
is used for welding mixed circuiting arc
15
short arc contact tube distance: approx. 15 mm 150 3,5 br-er5-11e.cdr
4,5
filler
spray arc
contact tube distance: approx. 19 mm
Figure 5.11
cover
passes in the flat position.
200 welding current
250
A
300
5,5 7,0 wire feed
8,0
m/min
10,5
Welding Parameters in Dependence on the Shielding Gas Mixture (SG 2, Ø1,2 mm)
and
© ISF 2002
Connections tween
be-
welding
5. Gas-Shielded Metal Arc Welding
61 parameters, shielding gas and arc type are shown in Figure 5.11. When the shielding gas M23 is used, the
thermal conductivity
helium
spray arc may already be produced hydrogen
with an amperage of 260 A. With the decreasing argon proportion the am-
CO2
perage has to be increased in order to
nitrogen
remain in the spray arc range. When pure carbon dioxide is applied, the
argon
spray arc cannot be produced. Figure
temperature
5.11 shows, moreover, that with the argon 82%Ar+18%CO2
CO2
increasing CO2 content the welding
helium
voltage must also be increased in order to achieve the same deposition br-er2-12e.cdr
© ISF 2002
rate.
The different thermal conductivity of Figure 5.12 current-carrying arc core
the shielding gases has a considerable influence on the arc configuration and
by the low thermal conductivity of the argon the arc core becomes very hot –
temperature
weld geometry, Figure 5.12. Caused
this results in a deep penetration in the
r
r
argon
weld centre, the so-called “argon finger-type penetration”. Weld reinforce-
carbon dioxide
Fa
F
ment is strongly pronounced. ApplicaFr
tion of CO2 and helium leads, due to
Fr
the better thermal conductivity of these F
shielding gases, to a wide and deep
Fa
penetration. argon br-er5-13e.cdr
A recombination (endothermic break of the linkage in the arc space – exoFigure 5.13
carbon dioxide © ISF 2002
5. Gas-Shielded Metal Arc Welding
62 thermal reaction 2CO + O2 ->2CO2 in the workpiece proximity) intensifies
wire elektrodes
this effect when CO2 is used. In argon, the current-carrying arc core
current-carrying arc core
is wider and envelops the wire electrode end, Figure 5.13. This generates electromagnetic forces which
argon
bring about the detachment of the
carbon dioxide
liquid electrode material. This socalled “pinch effect” causes a metal transfer in small drops, Figure 5.14.
The pointed shape of the arc attachbr-er5-14e.cdr
© ISF 2002
ment in carbon dioxide produces a reverse-direction
force
component,
i.e., the molten metal is pushed up Figure 5.14
until gravity has overcome that force component and material transfer in the form of very coarse drops appear.
acceleration due to gravity wire electrode
electromagnetic force FL (pinch effect)
Besides the pinch effect, the inertia and
the
gravitational
force,
other
forces, shown in Figure 5.15, are ac-
viscosity surface tension S
droplets necking down
tive inside the arc space; however these forces are of less importance.
backlash forces fr of the evaporating material
inertia electrostatic forces
suction forces, plasma flow induced work piece br-er5-15e.cdr
© ISF 2002
Forces in Arc Space
Figure 5.15
5. Gas-Shielded Metal Arc Welding
63
If the welding voltage and the wire feed speed are further increased, a rotating arc occurs after an undefined transition zone, Figure 5.16. High-efficiency MAG welding has been applied since the beginning of the nineties; the deposition rate, when this process is used, is twice the size as, in comparison, to spray arc welding. Apart from a multicomponent gas with a helium
proportion,
also a high-rating power source and a precisely controlled wire feed system for high
wire
feed
speeds are necessary.
br-er5-16e.cdr
© ISF 2002
Rotating Arc
Figure 5.16
Figure 5.17 depicts the deposition rates over the wire feed speed, as achievable with modern high-efficiency MAG welding processes.
During Ø 1,2 mm
kg/h
deposition rate
transi-
tion from the short
25
to the spray arc the
high performance GMA welding
20
Ø 1,0 mm
15
drop frequency rate increases erratically
10
Ø 0,8 mm
conventional GMA
while the drop volume
5
the 0
the
0
5
10
15
20
25
30
35
40
45 m/min
wire feed speed br-er5-17e.cdr
decreases same
degree.
With an increasing CO2-content,
this
© ISF 2002
“critical Deposition Rate
Figure 5.17
at
current
range” moves up to higher power ranges
5. Gas-Shielded Metal Arc Welding
64
and is, with inert gas constituents of lower than 80%, hardly achievable thereafter. This effect facilitates the pulsed-arc welding technique, Figure 5.18. 300
300
200
100
100
V arc voltage
200 critical current range
UEff
3
10 cm
drop volume
number of droplets
35 -4
1/s
25 20 Um
15 10 5
0
500
0 0
A
400
tP
200
600
A 400 welding current
Ikrit
Im
- background current IG - pulse voltage UP - impulse time tP - background time tG or frequency f with f = 1 / ( tG + tP), resp. - wire feed speed vD
time
IG
tG
Setting parameters:
350 300 IEff
250 200
Im
150 100 50 0 5
0
br-er5-18e.cdr
© ISF 2002
10
15 time
20
ms
br-er5-19e.cdr
30 © ISF 2002
Pulsed Arc
Figure 5.18
Figure 5.19
In pulsed-arc welding, a change-over occurs between a low, subcritical background current and a high, supercritical pulsed current. During the background phase which
welding current
corresponds with the pulsed current intensity
short arc range, the
Non-short-circuiting metal tranfer range
arc length is ionised and
backround current intensity
wire
electrode
and work surface are preheated. During the time
pulsed material
phase is
the
molten
and, as in spray arc welding,
superseded
© isf 2002
br-er5-20e.cdr
by
the
magnetic
Pulsed Metal Transfer
forces. Figure 5.20. Figure 5.20
5. Gas-Shielded Metal Arc Welding
65
Figure 5.19 shows an example of pulsed arc real current path and voltage time curve. The formula for mean current is:
Im =
1T idt T ∫0
for energy per unit length of weld is:
1T 2 i dt T ∫0
Ieff =
By a sensible se-
50 working range welding current / arc voltage
lection of welding
45
parameters,
40 optimal setting lower limit upper limit
35 voltage [v]
spray arc
GMA
the
welding
technique allows a
30 transition arc
selection of differ-
25 short arc shielding gas: 82%Ar, 18%CO2 wire diameter: 1,2 mm wire type: SG 2
20 15 10 50
75
100
125
150
175 200 225 250 welding current
275
300
325
350
375
are
distinguished
by
their
metal
400
transfer way. Fig-
© ISF 2002
br-er5-21e.cdr
ent arc types which
ure 5.21 shows the
Parameter Setting Range in GMA Welding
setting range for a
Figure 5.21
good
welding
process in the field filler metal: SG2 -1,2 mm shielding gas: Ar/He/CO2/O2-65/26,5/8/0,5
conventional
GMA welding.
transition zones spray arc
V
voltage
of
rotating arc
50
Figure 5.22 shows
30 high-efficiency spray arc
the extended set-
20
ting range for the
high-efficiency short arc
10
short arc
high-efficiency MAGM
100 br-er5-22e.cdr
200
300 welding current
400
A Quelle: Linde, ISF2002
Setting Range or Welding Parameters in Dependence on Arc Type
Figure 5.22
welding
600
process
with
rotating arc.
a
5. Gas-Shielded Metal Arc Welding
66 Some typical ap-
arc types welding methods MAGC MAGM MIG seam type, positions workpiece thickness
applications
spray arc
short arc
long arc
-
aluminium copper steel unalloyed, lowalloy, high-alloy
fillet welds or inner passes and cover passes of butt welds at medium-thick or thick components in position PA, PB
aluminium copper
different arc types
steel unalloyed, low-alloy
steel unalloyed, low-alloy, steel low-alloy, high-alloy high-alloy
steel unalloyed, low-alloy
steel unalloyed, low-alloy
fillet welds or inner passes and cover passes of butt welds at medium-thick or thick components in position PA, PB
fillet welds or butt welds fillet welds or inner at thin sheets, all positions passes and cover passes of thin and root layers of butt welds medium-thick at medium-thick or thick components, all components, all positions positions
welding of root layers in position PA
plications of the
pulsed arc
aluminium (s < 1,5 mm)
are depicted in Fig-
-
inner passes and cover passes of fillet or butt welds in position PC, PD, PE, PF, PG (out-of-position)
ure
5.23.
The
rotating arc, (not mentioned in the figure), is applied
root layer welds only conditionally possible
in just the same way as the spray
br-er5-23e.cdr
© ISF 2002
arc, however, it is
Applications of Different Arc Types
not used for the Figure 5.23
welding of copper and aluminium.
The arc length within the working range is linearly dependent on the set
U
welding voltage, Figure 5.24. The AL
weld seam shape is considerably in-
AM
AK
arc length: long medium short
fluenced by the arc length. A long arc produces a wide flat weld seam and, in the case of fillet welds, generally undercuts. A short arc produces a narrow, banked weld bead.
On the other hand, the arc length is inversely proportional to the wire
vD, I
operating point: wire feed speed: arc length: welding current: deposition efficiency:
AL
AM
AK
low long low low
medium medium medium medium
high short high high
weld appearance:
feed speed, Figure 5.25. This has influence on the current over the internal adjustment with a slightly dropping power
source
characteristic.
br-er5-24e.cdr
This
Wire Feed Speed
again is of considerable importance for the deposition rate, i.e., a low wire feed speed leads to a low deposition
© ISF 2002
Figure 5.24
5. Gas-Shielded Metal Arc Welding
67 rate, the result is flat penetration and
arc length: long medium short
U AL AM AK
low base metal fusion. At a constant weld speed and a high wire feed speed a deep penetration can be obtained.
vD, I
operating point: welding voltage: arc length:
AL
AM
high long
medium medium
AK low short
At equal arc lengths, the current intensity is dependent on the contact tube distance, Figure 5.26. With a large contact tube distance, the wire
weld appearance butt weld
stickout is longer and is therefore characterised by a higher ohmic resisweld appearance fillet weld
tance which leads to a decreased current intensity. For the adjustment of
br-er5-25e.cdr
© ISF 2002
Welding Voltage
the contact tube distance, as a thumb rule, ten to twelve times the size of
Figure 5.25 the wire diameter should be considered. lk1
lk2
lk3
influence on weld formation and welding process, Figure 5.27. When welding with the torch pointed in forward direction of the weld, a part of the weld pool is moved in front of the arc. This results in process instability.
contact tube-to-work distance lk
The torch position has considerable 3
30 mm
2
20
lk = 10 to 12 dD 1
10
0 200
250
However, it ha s the advantage of a flat smooth weld surface with good gap bridging. When welding with the torch pointed in reversing direction of
operating rule:
300 A
350
current wire electrode:
1,2 mm diameter
shielding gas:
82% Ar + 18% CO2
arc voltage:
29 V
wire feed speed:
8,8 m/min
welding speed:
58 cm/min
br-er5-26e.cdr
the weld, the weld process is more
© ISF 2002
Contact Tube-to-Work Distance
stable and the penetration deeper, as Figure 5.26
5. Gas-Shielded Metal Arc Welding
68 base metal fusion by the arc is better,
advance direction
although the weld bead surface is irregular and banked.
Figure 5.28 shows a selection of different application areas for the GMA technique and the appropriate shieldpenetration:
shallow
average
deep
gap bridging:
good
average
bad
arc stability:
bad
average
good
spatter formation: strong
average
low
weld width:
average
narrow
average
rippled
ing gases.
The welding current may be produced by different welding power sources. In d.c. welding the transformer must be wide
equipped with downstream rectifier weld appearance: smooth
br-er5-27e.cdr
assemblies, Figure 5.29. An additional
© ISF 2002
ripple-filter choke suppresses the residual ripple of the rectified current
Torch Position
and has also a process-stabilising Figure 5.27
effect.
power
sources
became
possible,
Figure
92% Ar + 8% CO2 forming gas (N2-H2-mixture)
88% Ar + 12% O2 82% Ar + 18% CO2
application examples autoclaves, vessels, mixers, cylinders panelling, window frames, gates, grids stainless steel pipes, flanges, bends spherical holders, bridges, vehicles, dump bodies reactors, fuel rods, control devices rocket, launch platforms, satellites valves, sliders, control systems stator packages, transformer boxes passenger cars, trucks radiators, shock absorbers, exhausts cranes, conveyor roads, excavators (crawlers) shelves (chains), switch boxes braces, railings, stock boxes mud guards, side parts, tops, engine bonnets attachments to flame nozzles, blast pipes, rollers vessels, tanks, containers, pipe lines stanchions, stands, frames, cages beams, bracings, craneways harvester-threshers, tractors, narrows, ploughs waggons, locomotives, lorries
5.29. The operating principle of a transistor
80% Ar + 5% O2 + 15% CO2 92% Ar + 8% O2
industrial sections
analogue
83% Ar + 15% He + 2% CO2 90% Ar + 5% O2 + 5% CO2
sign of transistor
99% Ar + 1% O2 or 97% Ar + 3% O2 97,5% Ar + 2,5% CO2
transistors the de-
Argon 4.8 Helium 4.6
efficient Argon 4.6
of
shielding gases
ment
Ar/He-mixture Ar + 5% H2 or 7,5% H2
With the develop-
analogue br-er5-28e.cdr
power source fol-
Fields of Application of Different Shielding Gases
lows the principle of an audio frequency
© ISF 2002
Figure 5.28
amplifier which amplifies a low-level to a high level input signal, possibly distortion-free. The transistor power source is, as conventional power sources, also equipped with a three-phase
5. Gas-Shielded Metal Arc Welding
69
transformer, with generally only one secondary tap. The secondary voltage is rectified by silicon diodes into full wave operation, smoothed by capacitors and fed to the arc through a transistor cascade. The welding voltage is steplessly adjustable until no-load voltage is reached. The difference between source voltage and welding voltage reduces at the transistor cascade and produces a comparatively high stray power which, in general, makes water-cooling necessary. The efficiency factor is between 50 and 75%. This disadvantage is, however, accepted as those power sources are characterised by very short reaction times (30 to 50 µs). Along with the development of transistor analogue power sources, the consequent separation of the power section (transformer and rectifier) and electronic control took place. The analogue or digital control sets the reference values and also controls the welding process. The power section operates exclusively as an amplifier for the signals coming from the control.
The output stage may also be carried out by clocked cycle. A secondary clocked transistor power source features just as the analogue power sources, a transformer and a rectifier, Figure 5.30. The transistor unit functions as an on-off switch. By varying the on-off period, i.e., of the pulse duty factor, the average voltage at the output of the transistor stage may be varied. The arc voltage achieves small ripples, which are of a limited amplitude, in the switching frequency of, in general, 20 kHz; whereas the welding current shows to be strongly smoothed during the high pulse frequencies caused by inductivities. As the transistor unit has only a switching function, the stray power is lower than that three-phase transformer
fully-controlled three-phase bridge rectifier
energy store
of
analogue
sources. The effi-
transistor power section
mains supply
welding current
ciency factor is approx. 75 – 95%. The reaction times of
uist u1 . . un
reference input values
iist
signal processor (analog-to-digital)
these
clocked
units are within of current pickup
300
–
500
µs
clearly longer than © isf 2002
br-er5-29e.cdr
GMA Welding Power Source, Electronically Controlled, Analogue
Figure 5.29
those of analogue power sources.
5. Gas-Shielded Metal Arc Welding
70
Series regulator power sources, the so-called “inverter power sources”, differ widely from the afore-mentioned welding machines, Figure 5.31. The alternating voltage coming from the mains (50 Hz) is initially rectified, smoothed and converted into a medium frequency alternating voltage (approx. 25-50 kHz) with the help of controllable transistor and thyristor switches. The alternating voltage is then transformer reduced to welding voltage levels and fed into the welding process through a secondary rectifier, where the alternating voltage also shows switching frequency related ripples. The advantage of inverter power sources is their low weight. A transformer that
transforms
voltage
with
fre-
quency of 20 kHz, has, compared with a
50
former,
Hz
3-phase transformer
3-phase bridge rectifier
energy store
transistor switch
protective reactor welding current
mains supply
trans-
considera-
bly lower magnetic
Uist U1 . . Un
losses, that is to
reference input values
say, its size may accordingly
be
smaller
its
Iist
signal processor (analog-to-digital)
br-er5-30e.cdr
and
© ISF 2002
GMA Welding Power Source, Electronically Controlled, Secondary Chopped
weight is just 10% of that of a 50 Hz
current pickup
Figure 5.30
transformer.
Reaction time and efficiency
factor
are comparable to the
filter
3-phase bridge rectifier
energy storage
transistor inverter
medium frequency transformer
rectifier welding current
mains supply
corresponding
values of switchingUist
type power sources.
U1 . . Un
reference input values
br-er5-31e.cdr
Iist
signal processor (analog-to-digital)
current pickup
© ISF 2002
GMA Welding Power Source, Electronically Controlled, Primary Chopped, Inverter
Figure 5.31
5. Gas-Shielded Metal Arc Welding
71
All welding power sources are fitted with a rating plate, Figure 5.32. Here the performance capability and the properties of the power source are listed. The S in capital letter (former K) in manufacturer insulations class
rotary current welding rectifier
~
_
protective IP21 system
VDE 0542 production number
type welding MIG/MAG
U0 15 - 38 V
F
cooling type
the middle shows F
that
DIN 40 050
input 3~50Hz 6,6 kVA (DB) cosj 0,72
power
source is suitable
switchgear number
S
the
35A/13V - 220A/25V
power range
X 60% ED 100% ED 170 A I2 220 A 23 V U2 25 V
power capacity in dependence of current flow
17 A 10 A
U1 220 V
I1 26 A
U1 380 V
I1
15 A
U1
V
I1
A
A
U1
V
I1
A
A
power supply
for welding operations
under
ardous
haz-
situations,
i.e., the secondary no-load voltage is lower than 48 Volt
min. and max. no-load voltage © ISF 2002
br-er5-32e.cdr
and therefore not Rating Plate
dangerous to the welder.
Figure 5.32
Besides the familiar solid wires also filler wires are used for
gas-shielded
metal arc welding. They consist of a a
seamless flux-cored wire electrode
b
c
metallic tube and a flux
form-enclosed flux-cored wire electrode
core
Figure 5.33 depicts common
br-er5-33e.cdr
cross-
© ISF 2002
Cross-Sections of Flux-Cored Wire Electrodes
Figure 5.33
filling.
sectional shapes.
5. Gas-Shielded Metal Arc Welding
72
Filler wires contain arc stabilisators, slag-forming and also alloying elements which support a stable welding process, help to protect the solidifying weld from the atmosphere and, more often than not, guarantee very good mechanical properties. An important distinctive criteria is the type of the filling. The influence of the filling is symbol R
slag characteristics rutile base, slowly soldifying slag rutile base, rapidly soldifying slag basic filling: metal powder
P B M V W
rutile- or fluoride-basic fluoride basic, slowly soldifying slag fluoride basic, slowly soldifying slag other types
Y S
customary application* S and M
very similar to that shielding gas ** C and M2
S and M
C and M2
S and M S and M S S and M
C and M2 C and M2 without without
S and M
without
Figure 5.34
electrode
covering in manual electrode (see
welding
chapter
2).
Figure 5.34 shows a list of the differ-
wire. © ISF 2002
Type Symbols of Flux-Cored Wire Electrodes According to DIN EN 12535
the
ent types of filler
*) S: single pass welding - M: multi pass welding **) C: CO2 - M2: mixed gas M2 according to DIN EN 439 br-er5-34e.cdr
of