You probably find
that you are working inefficiently over some portion of you total working
envelope.
You are probably
seeing variations in cut quality as you progress from one end of your
nest to the other.
You are probably
having to readjust your focal position manually as your cut quality
deteriorates due to inacurate focal positioning.
You may even be
adjusting your laser parameters in an attempt to maintain acceptable
cut quality
Focal
Point Variation (as shown above) is a natural phenomenon occuring with
the variation in distance between a laser source and a focusing optic.
Focal
Point Variation with the Bystronic programmable Bypos system is completely
eliminated over the entire working envelope of the machine (as shown
above). As a bonus, refocusing between materials is handled automatically
by the programs...
From
thin mild steel sheets to thick stainless steel sheets
The Bystronic programmable Bypos system provides you with the easiest
and fastest refocusing system imaginable... Changing between different
materials types or just changing to a different thickness can be this
easy and requires no operator intervention.
Imagine
the benefits...
Rapid changeover between
thick and thin materials without additional setting up...
Change from mild steel
to stainless steel automatically...
Ensure the cut quality
is consistant across the entire working area of your machine...
Contact our sales
team to discuss this technology.
Laser Cutting Theory
In
order to understand what makes a laser suitable for cutting, one must
distinguish its unique features in comparison to ordinary light.
Conventional light produces waves, which radiate out in all
directions to fill up and illuminate a wide area. The energy intensity
rapidly decreases as waves moves away from the source, just as the sun's
intensity is diminished when it finally reaches the earth.
The laser on the other hand provides a stream of collimated,
coherent light waves which give it exceptional intensity and direction
ability. Lacking the dispersion of conventional light, a laser can be
easily projected as a beam over relatively long distances while maintaining
nearly all of its useful power output.
The use of lasers for cutting can be thought of in the same
way as that of focusing sunlight with a magnifying glass to produce a
concentrated source of heat energy. While this method only results in
a few burned holes in paper, it gives us an illustration that light is
indeed a source of energy with potential material processing capabilities.
A laser can be used for cutting by exposing material to the
intense heat energy developed by its beam. If that heat input to the material
is greater than that material's ability to reflect, conduct, or disperse
the added energy, it will cause a sudden rise in temperature of the material
at that point. If the temperature rise is substantial enough, the input
heat is capable of initialising a hole by vaporizing the material. The
linear movement of this intense heat energy with respect to the material
provides cutting action.
In most cases the "raw" (unfocused) beam of even high
power (multi-kilowatt) industrial lasers has inadequate energy to do much
more than slowly heat a surface. Therefore, the beam is directed through
a focusing lens. This allows the energy to be concentrated into a spot
of less than 0.25 mm thus producing power densities of over a million
watts per centimeter squared, capable of vaporizing many materials.
While intense heat is capable of vaporising material, the control
of that heat is essential in determining quality. The key performance
features of a laser are those beam characteristics that affect the resultant
power density as it is directed onto the workpiece.
Mode
A cross-section
of a laser's beam profile is commonly referred to as mode. Described in
terms of TEM (Transverse Electromagnetic Mode) mode relates to the beam's
ability to be focused. It is also comparable to the degree of sharpness
of a cutting tool. The lowest order or reference mode is TEM00, of which
the beam's profile simulates a Gaussian distribution curve. Modes that
approach this energy distribution can be focused down to the laser's theoretical
minimum spot size and give the sharpest energy density.
Higher order or multi-mode beam profiles are characterised by
a tendency to spread out the energy distribution away from the centre
of the beam. The resultant spot is large with this mode causing lower
energy concentration. Therefore, higher order mode lasers are considered
to be duller cutting tools than low order mode lasers of equivalent power
output.
Power Output
Lasers
are rated by their power output in terms of watts. Since laser cutting
is a thermal process, the amount of heat produced relates to its capabilities.
Whereas a 300 watt laser with a high quality output is more than adequate
for the cutting of paper products, it lacks the heat producing capabilities
to effectively couple into aluminium. Given all other considerations being
equal (eg power distribution, spot size, etc), increased power allows
for faster processing speeds and the ability to cut thicker sections of
materials.
Stability
Since
quality results are obtained by the application of consistent energy,
the stability of the laser's output is a key feature in cutting. This
includes maintaining unwavering output energy (power stability), consistent
beam quality (mode stability), and fixed energy concentration (pointing
stability). Should the power increase or decrease by more than a few percent
over the short term operation, the beam quality oscillate between a Gaussian
and multi-mode profile, or the location of the beams direction shift more
than a few tenths of a milliradian due to the outputs instability, there
will result a noticeable change in the available power density for cutting.
Polarisation
Particularly
evident in metal cutting and ceramic processing, studies have shown that
random occurrences of inconsistent edge quality, namely variations in
kerf, edge smoothness, and perpendicularly, are attributable to the effects
of polarisation. Uncontrolled or random polarisation is characteristic
of most standard material processing lasers. It can unpredictably affect
the relative degree of absorption of the beam's energy that is coupled
into the material at a given moment. To correct this inconsistency, lasers
can be equipped with optical packages that either fix the polarisation
to be aligned in the same direction of the cutting action or circularly
polarise the output to give equivalent coupling regardless of the direction
travel.
An important asset of laser cutting is the high level of control,
which is available over the variables affecting the process. The cut can
be tailored to meet the exact requirements of the job and the results
can be readily duplicated. The principle parameters are:
Speed
Laser
cutting feedrates have been found to fit empirical formulas based on the
available laser power density and the properties of the material to be
cut. Above a threshold amount, the feedrates are directly proportional
to available power density, which takes into account the laser's performance
features (eg power, mode) in addition to the focusing system's characteristics
(eg spot size). Cutting rates are likewise inversely proportional to the
materials density and thickness. Therefore, given all other parameters
are constant, feedrates will increase with:
·Additional power (1700 watts vs 3500 watts)
·Improved mode (TEMoo, vs multimode)
·Smaller focused spot size (2.5 vs 5" F.L lens)
·Lower required energy to initiate vaporisation (plastic vs steel)
·Lower material density (white pine vs hickory)
·Decreased thickness (1.25" vs.250")
Feedrates can be varied for a particular set of parameters in
order to obtain different edge quality results, particularly for metals,
the plot of cutting speed versus thickness for a material has two curves.
The upper curve reflects the top speed at which through cuts are achieved
while the lower curve shows the limit below which the material is self-burning.
The resultant window of acceptable cut speeds is usually wider at the
thinner range of a material.
Focusing Lens
Since
speed is a function of available power density, the choice of the focusing
lens has a great impact on the resulting cut quality. Imaging of lasers
beams is usually accomplished with transmissive lenses of focal lengths
ranging from 2.5 to 10 inches. Because the focused spot size is proportional
to the focal length, the power density that is produced is proportional
to the square of that length. Short focal length lenses give very high
energy densities, but are limited in their application due to a shallow
working depth. They are appropriate for use with thin materials and in
high-speed operations where the material can be held within the limited
depth of field. Longer focal length lenses have lower power densities
but are able to maintain those densities over a much broader range and
therefore can be used for thicker cross sections of materials given that
they have enough energy initially.
Focal Point Position
During
the laser cutting process, the focal point of the lens should be consistently
positioned in order to provide the best cutting results. In most cases,
the focal point is positioned at or slightly below the surface of the
material. Above or below this point the power density will taper off until
it is insufficient to produce an effective cut. Cutting systems that employ
short focal length lenses must ensure constant monitoring of the lens-to-work
piece distance.
Assist Gas
Recall
that assist gas is supplied coaxial with the focused beam to protect the
lens and aid in the material removal process. Generally, compressed air
or inert gas is used to purge melted and evaporated material from the
cut zone while minimising any excess burning. For most metal cutting applications,
a reactive gas assist can be employed to promote an exothermic reaction.
The enhanced energy intensity from the use of oxygen can improve cutting
speeds by 25% - 40% over the results obtained with use of air.
In addition to gas type, delivery pressure is an important consideration.
Typically, pressures of 45-60 psi (3-4 bar) developed in the gas jet nozzle
are used in cutting thin material at high speeds to help prevent the clinging
of slag or dross to the back edge of the cut. The pressure is reduced
as the material thickness increases or process speeds slow.
LASER CUTTING PROCESS
Laser
cutting systems combine the heat of the focused beam with assist gas,
which is introduced through a nozzle coaxial to the focused beam. The
high velocity gas jet serves to:
·Aid in material removal by blowing out excess material through
the backside of the work piece
·Protect the lens from spatter ejected from the cut zone
·Assist in the burning process.
The best example of the chemical effect of the assist gas is
the use of oxygen for the cutting of steels where performances are increased
by the exothermic reaction of combustion of iron in oxygen. Another example
is clean cutting stainless steel with high-pressure nitrogen. As the laser
beam cuts the stainless steel, the high-pressure nitrogen blows the melted
material away.
While carbon dioxide lasers are capable of generating tremendous
heat intensity, it is an incorrect assumption that they are capable of
vaporising and cutting all known materials. Rather, each material has
its own unique response, some of which are not suitable, to the effects
of CO 2 lasers. Therefore, the question of suitability of using
a laser for cutting that material hinges on how well it handles the added
energy input. That interaction is dependent upon three key factors of
the material.
Surface condition
- how well it initially absorbs the energy
Heat flow properties
- its coefficients of thermal diffusivity and conductivity
Heat phase-change
requirements - the amount of excess heat required to induce a change
as a function of the materials density, specific heat, and latent heat
of vaporisation.
The following information is intended to provide general inputs
on the major categories of materials, keeping in mind these factors.
NON-METALS
In
general, non-metallic materials are good absorbers of infrared energy
as produced by a CO 2 laser. Likewise,
they are generally poor conductors of heat and have relatively low boiling
temperatures. As such, the energy intensity of a focused beam is almost
totally transmitted into the material at the spot and will instantly vaporise
a hole.
Plastics (Polymers)
Lasers
have found their way into many plastic machining operations because of
their ability to cut complex geometrise, at high feedrates without contacting
the work piece. Since the laser is an intense heat source, it uses its
energy to vaporise the binder and quickly breaks down the material's polymer
chains.
Thermoplastics with relatively low melting temperatures typically
display clean cuts with fire-polished edges as a result of resolidified
melting. Process control can be exercised to minimise or eliminate bubbling
or the presence of small burrs on the backside of the cut.
As the tensile strength of the polymer increases, there is a
correlation to a marked increase of charring present along the cut edge.
Greater energy intensity per unit time is required to break the stronger
chains and therefore leads to a burning action. Reasonable results have
been obtained with polyester and polycarbonate while there is generally
a substantial layer of decomposed material along the edge of phenolic,
polyamides, and PVC.
As a caution, in the cutting of some polymers, specifically
lucite, and PVC, careful attention must be directed at the containment
and appropriate filtering of potentially hazardous and/or corrosive fumes
that are generated as the result of burning.
Composites
New
lightweight, fibre reinforced polymers are difficult to machine with conventional,
cutting tools. This has led many users to the non-contact cutting capabilities
of a laser. Prior to the curing of laminated stacks, thin prepreg sheets
in thicknesses up to 0.5mm can be trimmed or sized at speeds up to 40
metres per min without gumming up a cutting tool. The heat from the lasers
cutting action fuses the edges, thus preventing fraying of the fibres.
For thicker sections and fully cured composites, particularly
boron and carbon fibre material, there is a higher probability of charring,
and thermal damage along the cut edge, thus reducing the acceptability
of laser cutting for structural members. As with the cutting of polymers,
care should be exercised in the removal of fumes.
Rubber
Both
natural gum and synthetic rubber materials in thicknesses up to l9mm readily
vaporise from the heat of a focused laser beam. This allows precision
sizing of items such as gaskets.
Material with fibre or steel cord reinforcement can be cut with
a laser at considerably slower speeds due to the higher energy intensity
per unit time necessary to sever the cords.
The advantage of laser cutting is the simplicity of handling
without having to worry about stretching or distorting of the material
due to the impact of a cutting tool. Fresh cut samples tend to exhibit
slight stickiness along the edge so they require care in post-process
handling. Additionally, some rubber, particularly those containing carbon
black, may require a clean-up operation to wipe clean any edge charring.
Wood
The
laser offers a number of attractive advantages for the cutting of timber,
plywood, and particleboard. In particular, it provides narrow kerfs of
0.3-0.8mm, the absence of sawdust, the ability to contour cut in any direction
and no tool wear and noise. While the use of a laser likewise eliminates
rough, torn-out, and fuzzy edges as evident with conventional sawing techniques,
it is characterised by "burned" edges produced by the laser's
heat. Greater amounts of charring will result when the material thickness
is increased, thereby slowing the cutting feed-rates.
While lasers are routinely cutting slots in die boards for mounting
of steel rule dies their acceptance for other industrial applications
has been hampered by process limitations and relatively high initial cost.
Since practical power outputs are limited to a few kilowatts, lasers are
limited in their ability to cut up to 75mm thick for timber and 25mm for
particleboard and plywood.
Other Organics
Paper
products and leather, as well as natural and synthetic textiles, can easily
be cut with a laser. The lack of thickness; coupled with their high combustibility
minimises the power output requirements of a laser to no more than a few
hundred watts. The resultant edges are clean and free from fraying.
Quartz
Since
it has a relatively low co-efficient of thermal expansion, quartz responds
well to the cutting action of a laser. Though there is the presence of
a shallow heat affected zone adjacent to a cut, the resultant edges are
crack-free and have a smooth appearance thereby eliminating clean-up operations
required by saw cutting. Thicknesses up to10mm can be cut at speeds that
are a couple orders of magnitude greater than sawing and without imparting
force to the work piece.
Glass
As
opposed to quartz, most types of glass are prone to thermal shock and
are therefore generally not suitable candidates for laser cutting. The
instantaneous heat of the laser's beam provides cutting action by both
vaporisation and the blowing away of molten glass from the cut zone.
Some materials such as boro silicates have a low co-efficient
of expansion and, with adequate head cycling, can tolerate the heat input
from a laser. However, most other forms of glass including soda lime experience
thermal shock that results in crack propagation along the cut edge. Also,
based on the reflow characteristics of the particular glass, there will
be varying degrees of resolidified material that will adhere to the edges
and underside of the cut.
Stone & Rock
While
they tend to absorb the heat energy from a laser, granite, concrete, rock,
stone and various minerals are not suited for laser cutting. The explosiveness
from heating moisture within the materials can lead to undesirable cracking.
Aside from the lack of uniformity in their structures, stone and rock
are typically found in thicknesses greater than 25mm, far in excess of
the practical depth. of field of useable focussed laser energy.
Metals
Although
at room temperature, almost all metals are highly reflective of infrared
energy, the CO 2 laser with its 10.6-micron wavelength (far infrared)
is successfully employed on many metal cutting applications. The initial
absorptivity can range from only 10% to as little as 0.5% of the incident
energy. However, the focusing of a beam to provide power densities in
excess of 1 million watts per square cm can quickly (in a matter of microseconds)
initiate surface melting. The absorption characteristics of most metals
in their molten states increase dramatically, raising the absorptivity
of energy to as much as 60% - 80%.
Carbon Steel
Conventional
steels of up to 16 mm lend themselves reasonably well to oxygen assisted
laser mating. The kerfs are narrow (as little as 0. 1 mm for thin material)
and the resultant heat affected zones are negligible, particularly for
mild and low carbon steel. At the same time, the cut edges are smooth,
clean, and square.
It has been found that the presence of pockets of phosphorus
and sulphur within mild steel can cause burnout along the cut edge, as
such, the use of low impurity steels (eg cold rolled) will result in improved
edge quality over results obtained with hot-rolled material. A higher
carbon content within the steel does yield a slight improvement in edge
quality yet will make the material subject to an increased HAZ.
Stainless Steel
Lasers
have been shown to be viable cutting tools for the fabrication of sheet
metal components made from stainless. The controlled heat input of the
laser beam serves to minimise the HAZ along the cut edge, thereby helping
the material to maintain its corrosion resistance. Since stainless does
not react with an oxygen assist as efficiently as does mild steel, cutting
speeds for stainless are slightly slower than those for comparable thicknesses
of plain steel. At the expense of up to 50% of the speed for oxygen-assisted
cutting, an inert assist gas can be employed to obtain a "weld ready",
oxide-free cut edge.
As for the resultant cut quality, martensitic and ferritic (400
series) stainless provide clean smooth edges. The presence of nickel within
austenitic (300 series and precipitation hardened) stainless steels affects
the energy coupling and transfer within the material. Specifically, the
viscosity of molten nickel generated during the cutting action causes
it to migrate and adhere to the backside of the cut. While the use of
high velocity gas jets can effectively eliminate slag for material up
to 1.0 mm thick, slag deposits up to 0. 5mm are generally present on thicker
cross sections.
Alloy Steel
Since
care is taken to control the amount and distribution of additives to the
base iron, most alloy steels are considered ideal candidates for the laser
cutting process. High strength materials such as AISI-SAE 4130 (chrome
moly steel) and 4340 (chrome nickel moly steel) display exceptional laser
cut edges that are square and clean.
Tool Steel
Similar
in many ways to allow steels, most tool steels respond reasonably well
to the cutting action of a laser. The most notable exceptions are the
tungsten high speed (Group T) and tungsten hot work (part of Group H)
materials that retain heat in a molten state, thereby resulting in burned
out and slaggish cuts.
Aluminium Alloys
Due
to its high thermal conductivity and high reflectivity to a CO
2 laser's wavelength, aluminium requires considerably
higher laser energy intensity in order to initiate cutting compared to
steel. This means the need for a laser possessing exceptional beam quality
and capable of outputting at least 500 watts, in addition to precise focus
control. Due to the reduced coupling efficiency, even 1-2 kilowatt lasers
are limited to cutting of thicknesses under 3.8mm.
During the cutting process, the assist gas serves primarily
to blow the molten material from the cut zone. This helps to produce edge
quality that is generally superior to that produced by a bandsaw. However,
the melted material tends to flow along the edge and cling to the backside
of the cut. While this slag is easily removable, there are intergranular
cracks emanating from the cut surface on some alloys. Concern over the
presence of this micro cracking has prevented the use of lasers for manufacturing
structural components such as aircraft.
Copper Alloys
Copper
has less ability than aluminium to absorb energy from a CO
2 laser. Due to its high reflectance, copper
generally cannot be cut. Brass on the other hand can absorb some energy.
It essentially behaves like aluminium with slag adhering to the backside
of the cut.
Titanium
Pure
titanium responds well to the concentrated heat energy of a focused laser
beam. The use of an oxygen assist enhances the cutting speeds but tends
to promote a larger oxide layer along the cut edge. Aircraft alloys such
6AL-4V tend to exhibit some slag that adheres to the bottom side of the
cut but is relatively easy to remove.
Primary Considerations
This
section discusses the criteria that are important to successful cutting.
It is intended as a guide only, since there is no substitute for operator
experience.
These are the principal considerations with which the operator
must concern himself at all times. Note that it is the combined effect
of these adjustments that determines the result. The various items cannot
be considered independently.
Laser Power Setting
The
most important point regarding laser power is that maximum power is not
necessarily beneficial. Firstly, there is some trade-off between power
and mode - the mode (or quality of the beam, which determines the fineness
of the focus) is of significantly greater importance to cutting than the
power level. Secondly, limiting the power is frequently beneficial in
terms of reducing thermal input into the material - especially when cutting
thin material, or materials which can be adversely affected by excess
heat. It is simply wasteful to use more power than necessary.
Cutting Speed
The
actual feedrate in use for a job will directly affect the cutting results;
the feedrate is decidedly a function of the type of material and material
thickness to be used. In any particular case, there will be some feedrate
that is too high and the cut will simply fail to penetrate the material
fully; at the other extreme, excessive heat input is likely to damage
the material adjacent to the cut. In general, some feedrate closer to
the maximum limit will be optimum, but always the choice is made experimentally
on the basis of cutting results; the operator, with a little experience,
can make this determination quite readily, making use of the feedrate
override control.
Focal Height
Focus
assemblies provide support for the lens in order to image the beam. These
assemblies generally provide means to adjust the focal point in or at
the part. Height sensing devices can be incorporated to automatically
maintain the proper focal point position regardless of undulations in
the work piece surface. These devices measure the lens-to-work piece spacing
either through contact probes riding on the work piece surface or via
a comparison of non-contact optical, acoustic, or electrical (inductance
or capacitance measuring) signals bounced off the material. The feedback
can trigger compensation of the vertical axis position.
For best results, the focal point of the beam must impinge on
the surface of a work piece. This factor is of greater or lesser importance,
depending on the material; in general, materials that have a high intrinsic
reflectivity to the laser beam will be most critical of the focal height
setting (eg. mild steel 45% reflective; stainless steel 66%; aluminium
99%). The focal point on aluminium and stainless steel should be approximately
4/5 buried into the material. Thicker carbon steel will cut better when
the focal point is 1-2 mm above the material.
The operator may find that the focal point needs to be "tweaked"
occasionally during a job; the precise focal point can change slightly
owing to thermal effects in the lens.
Nozzle Lateral Adjustment (Spot)
Gas
jet nozzle assemblies are usually integrated with the focusing assembly
below the lens in order to develop the desired gas assist. A properly
designed nozzle tip is very important to the cutting process. It can promote
higher feedrates, and better quality with minimum gas consumption.
Nozzle adjustment is an important factor, ensuring that the
beam emanates centrally through the orifice. Misalignment of the nozzle
normally causes noticeable variations in cut quality with respect to the
direction of the cutting traverse. Severe misalignment results in the
laser beam hitting the inner walls of the nozzle, with consequent poor
cutting performance, and heating of the nozzle and surrounding assembly.
The nozzle adjustment must be made whenever a lens is changed,
or even if a lens is removed temporarily for cleaning. During a working
shift, the operator might "tweak" this adjustment a few times;
the slight changes in pointing angle of the beam (through the external
optical system) account for this requirement.
Secondary Considerations
These
are considerations with which an operator must become concerned when cutting
results are below expectations, and all primary considerations (listed
above) have been checked.
Choice of lens
As
a general rule, the shortest focal length lens (5") produces the
most sharply defined focal point. Thus, the 5" lens is used when
maximum intensity is important - that is, cutting materials with high
intrinsic reflectivity (metals). In practice, there is only a slight (but
usually noticeable) difference between a 5" lens and a 7.5 lens in
this respect.
The longer focal length is required, however, to achieve parallel-sided
cuts in some materials when the material is reasonably thick. For example,
to cut 1" thick acrylic, it is found virtually impossible to keep
the sides of the cut parallel with the 5" lens, whereas the 7.5"
lens makes this quite easy. Note that the choice of laser power, assist
gas pressure, and feedrate all combine to influence the cut quality in
this respect, apart from the lens itself.
Condition of the lens
Cleanliness
of the lens is of major importance, since any contaminants on its surfaces
will cause it to absorb energy and become warm. Thermal distortion in
the lens inevitably produces fuzziness in the focal point of the beam,
and consequent reduction in cutting performance. Eventually, if a lens
becomes excessively heated, thermal stress and gas pressure will cause
it to shatter.
The operator should inspect the lens regularly (and clean as
necessary). In fact, common sense is the rule here; the source of contamination
is virtually always airborne particles produced by the cutting. Therefore,
if material being cut produces contaminants (eg. sheet metal often has
oil on the surface; rubber produces black smog when cut; etc.), the lens
should be inspected as often as convenient. The assist gas greatly helps
in keeping contaminants away from the lens, but the operator must be aware
that this is by no means total protection. Lifting the focal height while
piercing will also help protect the lens.
Condition of the nozzle
The
copper nozzle may become damaged or blocked in time, usually as a result
of hot metal spatter thrown up from the work surface. The orifice can
be cleared by a conventional oxy tip-cleaner.
After some usage, the orifice may become "out of round";
this causes swirling or vortex action in the assist gas jet, which usually
produces highly directional effects in the cutting. Often, this can be
rectified by carefully drilling the orifice; if the orifice is of large
diameter then excessive assist gas will be consumed. Eventually, the nozzle
will need replacement.
External Optical Alignment
The
optical system (set of mirrors) external to the laser cavity (including
the mirror mounted at the top of the Beam Control Unit) should normally
be checked and adjusted on a routine basis (say, once per month). However,
if the integrity of the alignment is under suspicion in the meantime,
it can be checked by using the cross-wire method of allowing the raw beam
to pass through the system onto a target. The image produced by the cross-wire
(its shadow) will indicate whether the beam passes through the position
centrally.
Misalignment of the external beam will generally cause haphazard
cutting results, with highly noticeable directionality.
Assist Gas Pressure
Generally
oxygen is used for metal cutting, and air is used for non-metal cutting.
High-pressure nitrogen can be used to cut mild steel, stainless steel and
aluminium. Using nitrogen as an assist gas leaves the cut edges clean and
free of dross but is expensive because up to 25 bar is needed. The general
rule with assist gas is: there must be sufficient flow (pressure) in each
case, but an excessive amount is wasteful. Normally, high-pressure cutting
requires increased pressure with increased material thickness and cutting
with oxygen requires decreased pressure with increased thickness. Of course,
the type of material is also an influence; very low carbon steel, for example,
will be adversely affected by excessive oxygen flow since it is highly reactive.
In any particular case, the pressure used will be experimentally
determined, and is usually not highly critical. Note that no material can
be cut without any assist gas.