Subscribe to our newsletter to receive the latest news and events from TWI:

Subscribe >
Skip to content

Cutting processes - plasma arc cutting - process and equipment considerations


Photo courtesy: Goodwin Plasma
Photo courtesy: Goodwin Plasma

The plasma arc process has always been seen as an alternative to the oxy-fuel process. In this part of the series the process fundamentals are described with emphasis being placed on the operating features and the advantages of the many process variants.


 Click here to see our latest technical engineering podcasts on YouTube.


Process fundamentals

The plasma arc cutting process is illustrated in Fig. 1. The basic principle is that the arc formed between the electrode and the workpiece is constricted by a fine bore, copper nozzle. This increases the temperature and velocity of the plasma emanating from the nozzle. The temperature of the plasma is in excess of 20 000°C and the velocity can approach the speed of sound. When used for cutting, the plasma gas flow is increased so that the deeply penetrating plasma jet cuts through the material and molten material is removed in the efflux plasma.


Fig.1. The plasma arc cutting process
Fig.1. The plasma arc cutting process

The process differs from the oxy-fuel process in that the plasma process operates by using the arc to melt the metal whereas in the oxy-fuel process, the oxygen oxidises the metal and the heat from the exothermic reaction melts the metal. Thus, unlike the oxy-fuel process, the plasma process can be applied to cutting metals which form refractory oxides such as stainless steel, aluminium, cast iron and non-ferrous alloys.

Power source

The power source required for the plasma arc process must have a drooping characteristic and a high voltage. Although the operating voltage to sustain the plasma is typically 50 to 60V, the open circuit voltage needed to initiate the arc can be up to 400V DC.

On initiation, the pilot arc is formed within the body of the torch between the electrode and the nozzle. For cutting, the arc must be transferred to the workpiece in the so-called 'transferred' arc mode. The electrode has a negative polarity and the workpiece a positive polarity so that the majority of the arc energy (approximately two thirds) is used for cutting.

Gas composition

In the conventional system using a tungsten electrode, the plasma is inert, formed using either argon, argon-H2 or nitrogen. However, as described in Process variants, oxidising gases, such as air or oxygen, can be used but the electrode must be copper with hafnium.

The plasma gas flow is critical and must be set according to the current level and the nozzle bore diameter. If the gas flow is too low for the current level, or the current level too high for the nozzle bore diameter, the arc will break down forming two arcs in series, electrode to nozzle and nozzle to workpiece. The effect of 'double arcing' is usually catastrophic with the nozzle melting.

Cut quality

The quality of the plasma cut edge is similar to that achieved with the oxy-fuel process. However, as the plasma process cuts by melting, a characteristic feature is the greater degree of melting towards the top of the metal resulting in top edge rounding, poor edge squareness or a bevel on the cut edge. As these limitations are associated with the degree of constriction of the arc, several torch designs are available to improve arc constriction to produce more uniform heating at the top and bottom of the cut.

Process variants

The process variants, Figs. 2a to 2e, have principally been designed to improve cut quality and arc stability, reduce the noise and fume or to increase cutting speed.

Dual gas

Fig.2a. dual gas
Fig.2a. dual gas

The process operates basically in the same manner as the conventional system but a secondary gas shield is introduced around the nozzle, Fig. 2a. The beneficial effects of the secondary gas are increased arc constriction and more effective 'blowing away' of the dross. The plasma forming gas is normally argon, argon-H2 or nitrogen and the secondary gas is selected according to the metal being cut.


air, oxygen, nitrogen

Stainless steel

nitrogen, argon-H2, CO2


argon-H2, nitrogen / CO2

The advantages compared with conventional plasma are:

  • Reduced risk of 'double arcing'
  • Higher cutting speeds
  • Reduction in top edge rounding

Water injection

Fig.2b. water injection
Fig.2b. water injection

Nitrogen is normally used as the plasma gas. Water is injected radially into the plasma arc, Fig. 2b, to induce a greater degree of constriction. The temperature is also considerably increased, to as high as 30,000°C.

The advantages compared with conventional plasma are:

  • Improvement in cut quality and squareness of cut
  • Increased cutting speeds
  • Less risk of 'double arcing'
  • Reduction in nozzle erosion

Water shroud

Fig.2c. water shrouded
Fig.2c. water shrouded

The plasma can be operated either with a water shroud, Fig. 2c, or even with the workpiece submerged some 50 to 75mm below the surface of the water. Compared with conventional plasma, the water acts as a barrier to provide the following advantages:

  • Fume reduction

  • Reduction in noise levels
  • Improved nozzle life

In a typical example of noise levels at high current levels of 115dB for conventional plasma, a water shroud was effective in reducing the noise level to about 96dB and cutting under water down to 52 to 85dB.

As the water shroud does not increase the degree of constriction, squareness of the cut edge and the cutting speed are not noticeably improved.

Air plasma

Fig.2d. air plasma
Fig.2d. air plasma

The inert or unreactive plasma forming gas (argon or nitrogen) can be replaced with air but this requires a special electrode of hafnium or zirconium mounted in a copper holder, Fig. 2d. The air can also replace water for cooling the torch. The advantage of an air plasma torch is that it uses air instead of expensive gases.

It should be noted that although the electrode and nozzle are the only consumables, hafnium tipped electrodes can be expensive compared with tungsten electrodes.

High tolerance plasma

Fig.2e. high tolerance
Fig.2e. high tolerance

In an attempt to improve cut quality and to compete with the superior cut quality of laser systems, High Tolerance Plasma Arc cutting (HTPAC) systems are available which operate with a highly constricted plasma. Focusing of the plasma is effected by forcing the oxygen generated plasma to swirl as it enters the plasma orifice and a secondary flow of gas is injected downstream of the plasma nozzle, Fig. 2e. Some systems have a separate magnetic field surrounding the arc. This stabilises the plasma jet by maintaining the rotation induced by the swirling gas. The advantages of HTPAC systems are:

  • Cut quality lies between a conventional plasma arc cut and laser beam cut
  • Narrow kerf width
  • Less distortion due to smaller heat affected zone

HTPAC is a mechanised technique requiring precision, high-speed equipment. The main disadvantages are that the maximum thickness is limited to about 6mm and the cutting speed is generally lower than conventional plasma processes and approximately 60 to 80% the speed of laser cutting. 

This article was prepared by Bill Lucas in collaboration with Derrick Hilton, BOC

For more information please email: