Inductively Coupled Plasma
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Inductively Coupled Plasma
Fig. 1. Picture of an analytical ICP torch

An inductively coupled plasma (ICP) or transformer coupled plasma (TCP)[1] is a type of plasma source in which the energy is supplied by electric currents which are produced by electromagnetic induction, that is, by time-varying magnetic fields.[2]

## Operation

Fig. 2. The construction of Inductively Coupled Plasma torch.[3] A: cooling gas tangential flow to the outer quartz tube B: discharge gas flow (usually Ar) C: flow of carrier gas with sample D: induction coil which forms the strong magnetic field inside the torch E: force vectors of the magnetic field F: the plasma torch (the discharge).

There are three types of ICP geometries: planar (Fig. 3 (a)), cylindrical [4] (Fig. 3 (b)), and half-toroidal (Fig. 3 (c)).[5]

Fig. 3. Conventional Plasma Inductors

In planar geometry, the electrode is a length of flat metal wound like a spiral (or coil). In cylindrical geometry, it is like a helical spring. In half-toroidal geometry, it is toroidal solenoid cut along its main diameter to two equal halves.

When a time-varying electric current is passed through the coil, it creates a time-varying magnetic field around it, with flux

${\displaystyle \Phi =\pi r^{2}H=\pi r^{2}H_{0}\cos \omega t}$,

where r is the distance to the center of coil (and of the quartz tube).

According to the Faraday-Lenz's law of induction, this creates azimuthal electromotive force in the rarefied gas:

${\displaystyle U=-{\frac {d\Phi }{dt}}}$,

which corresponds to electric field strengths of

${\displaystyle E={\frac {U}{2\pi r}}={\frac {\omega rH_{0}}{2}}\sin \omega t}$,[6]

leading to the formation of the figure-8 electron trajectories[5] providing a plasma generation. The dependence on r suggests that the gas ion motion is most intense in the outer region of the flame, where the temperature is the greatest. In the real torch, the flame is cooled from the outside by the cooling gas, so the hottest outer part is at thermal equilibrium. There temperature reaches 5 000-6 000 K.[7] For more rigorous description, see Hamilton-Jacobi equation in electromagnetic fields.

The frequency of alternating current used in the RLC circuit which contains the coil usually 27-41 MHz. To induce plasma, a spark is produced at the electrodes at the gas outlet. Argon is one example of a commonly used rarefied gas. The high temperature of the plasma allows the determination of many elements, and in addition, for about 60 elements degree of ionization in the torch exceeds 90%. The ICP torch consumes ca. 1250-1550 W of power, but this depends on the elemental composition of the sample (due to different ionization energies).[7]

The ICPs have two operation modes, called capacitive (E) mode with low plasma density and inductive (H) mode with high plasma density, and E to H heating mode transition occurs with external inputs.[8]

## Applications

Plasma electron temperatures can range between ~6,000 K and ~10,000 K (~6 eV - ~100 eV),[5] and are usually several orders of magnitude greater than the temperature of the neutral species. Argon ICP plasma discharge temperatures are typically ~5,500 to 6,500 K[9] and are therefore comparable to that reached at the surface (photosphere) of the sun (~4,500 K to ~6,000 K). ICP discharges are of relatively high electron density, on the order of 1015 cm-3. As a result, ICP discharges have wide applications where a high-density plasma (HDP) is needed.

Another benefit of ICP discharges is that they are relatively free of contamination, because the electrodes are completely outside the reaction chamber. By contrast, in a capacitively coupled plasma (CCP), the electrodes are often placed inside the reactor and are thus exposed to the plasma and subsequent reactive chemical species.

## References

1. ^ High density fluorocarbon etching of silicon in an inductively coupled plasma: Mechanism of etching through a thick steady state fluorocarbon layer Archived 2016-02-07 at the Wayback Machine T. E. F. M. Standaert, M. Schaepkens, N. R. Rueger, P. G. M. Sebel, and G. S. Oehrleinc
2. ^ A. Montaser and D. W. Golightly, eds. (1992). Inductively Coupled Plasmas in Analytical Atomic Spectrometry. VCH Publishers, Inc., New York.CS1 maint: extra text: authors list (link)
3. ^ Lajunen, L. H. J.; Perämäki, P. (2004). Spectrochemical Analysis by Atomic Absorption and Emission (2 ed.). Cambridge: RSC Publishing. p. 205. ISBN 978-0-85404-624-9.
4. ^ Pascal Chambert and Nicholas Braithwaite (2011). Physics of Radio-Frequency Plasmas. Cambridge University Press, Cambridge. pp. 219-259. ISBN 978-0521-76300-4.
5. ^ a b c Shun'ko, Evgeny V.; Stevenson, David E.; Belkin, Veniamin S. (2014). "Inductively Coupling Plasma Reactor With Plasma Electron Energy Controllable in the Range From ~6 to ~100 eV". IEEE Transactions on Plasma Science. 42 (3): 774-785. Bibcode:2014ITPS...42..774S. doi:10.1109/TPS.2014.2299954. ISSN 0093-3813. S2CID 34765246.
6. ^ , ?. ?.; ?, ?. ?.; ?, ?. ?.; , ?. ?.; , ?. ?.; , ?. ?. (1962). " ". In , ?. ?. (ed.). ? ?. : . p. 58.
7. ^ a b Dunnivant, F. M.; Ginsbach, J. W. (2017). Flame Atomic Absorbance and Emission Spectrometry and Inductively Coupled Plasma -- Mass Spectrometry. Whitman College. Retrieved 2018.
8. ^ Hyo-Chang Lee (2018) Review of inductively coupled plasmas: Nano-applications and bistable hysteresis physics 5 011108 https://doi.org/10.1063/1.5012001
9. ^ Cornelis, RITA; Nordberg, MONICA (2007). "CHAPTER 2 - General Chemistry, Sampling, Analytical Methods, and Speciation**Partly based on Chapter 2: General chemistry of metals by V. Vouk and Chapter 3: Sampling and analytical methods by T. J. Kneip and L. Friberg in Friberg et al. (1986).". Handbook on the Toxicology of Metals (Third ed.). Academic Press. pp. 11-38. doi:10.1016/B978-012369413-3/50057-4. ISBN 9780123694133.