View source for Electrospray

{{short description|Apparatus that employs electricity to disperse a liquid into fine aerosol}}
{{About|high voltage-induced sprays|mass spectrometry ion formation|electrospray ionization}}

The name '''electrospray''' is used for an apparatus that employs electricity to disperse a liquid or for the fine aerosol resulting from this process. High voltage is applied to a liquid supplied through an '''emitter''' (usually a glass or metallic capillary). Ideally the liquid reaching the emitter tip forms a [[Taylor cone]], which emits a liquid jet through its apex. [[Varicose wave]]s on the surface of the jet lead to the formation of small and highly charged liquid droplets, which are radially dispersed due to [[Coulomb's law|Coulomb]] repulsion.

==History==
{{see also|Electrospinning#History}}
In the late 16th century [[William Gilbert (astronomer)|William Gilbert]]<ref name=gilbert>Gilbert, W. (1628) De Magnete, Magneticisque Corporibus, et de Magno Magnete Tellure (On the Magnet and Magnetic Bodies, and on That Great Magnet the Earth), London, Peter Short</ref> set out to describe the behaviour of magnetic and electrostatic phenomena. He observed that, in the presence of a charged piece of amber, a drop of water deformed into a cone. This effect is clearly related to electrosprays, even though Gilbert did not record any observation related to liquid dispersion under the effect of the electric field.

In 1750 the French clergyman and physicist [[Jean-Antoine Nollet|Jean-Antoine (Abbé) Nollet]] noted water flowing from a vessel would aerosolize if the vessel was electrified and placed near electrical ground.<ref>{{cite thesis |type=Ph.D. |chapter= 2 |title= Fundamental Studies of the Mechanisms and Applications of Field-Induced Droplet Ionization Mass Spectrometry and Electrospray Mass Spectrometry |chapter-url= https://thesis.library.caltech.edu/3992/12/complete_thesis.pdf |last= Grimm |first= Ronald L. |year= 2006|publisher= Caltech Library |access-date= May 17, 2013}}</ref>

In 1882, [[John Strutt, 3rd Baron Rayleigh|Lord Rayleigh]] theoretically estimated the maximum amount of charge a liquid droplet could carry;<ref>{{cite journal| author=Rayleigh, L. |title = On the Equilibrium of Liquid Conducting Masses charged with Electricity | journal = [[Philosophical Magazine]] | year = 1882 | volume = 14 |issue = 1 | pages = 184–186 | doi=10.1080/14786448208628425| url = https://zenodo.org/record/1431159/files/article.pdf }}</ref> this is now known as the "Rayleigh limit". His prediction that a droplet reaching this limit would throw out fine jets of liquid was confirmed experimentally more than 100 years later.<ref>{{cite journal|author1=Gomez, A |author2=Tang, K |title = Charge and fission of droplets in electrostatic sprays. | journal = [[Physics of Fluids]] | year = 1994 | volume = 6 | issue=1 | pages = 404–414 | doi = 10.1063/1.868037|bibcode = 1994PhFl....6..404G }}</ref>

In 1914, [[John Zeleny]] published work on the behaviour of fluid droplets at the end of glass capillaries.<ref>{{cite journal| author=Zeleny, J. |title = The electrical discharge from liquid points, and a hydrostatic method of measuring the electric intensity at their surfaces. | journal = [[Physical Review]] | year = 1914 | volume = 3 | issue = 2 | page = 69 | doi = 10.1103/PhysRev.3.69 | bibcode=1914PhRv....3...69Z|url = https://zenodo.org/record/1517382 }}</ref> This report presents experimental evidence for several electrospray operating regimes (dripping, burst, pulsating, and cone-jet). A few years later, Zeleny captured the first time-lapse images of the dynamic liquid meniscus.<ref>{{cite journal| author=Zeleny, J. |title = Instability of electrified liquid surfaces. | journal = [[Physical Review]] | year = 1917 | volume = 10 | issue = 1 | pages = 1–6 | doi = 10.1103/PhysRev.10.1 | bibcode=1917PhRv...10....1Z}}</ref> 
 
Between 1964 and 1969 [[Geoffrey Ingram Taylor|Sir Geoffrey Ingram Taylor]] produced the theoretical underpinning of electrospraying.<ref name=Taylor1964>{{cite journal | author = Geoffrey Taylor | year = 1964 | title = Disintegration of Water Droplets in an Electric Field | journal = [[Proceedings of the Royal Society A]] | volume = 280 | issue = 1382 | pages = 383–397 | doi = 10.1098/rspa.1964.0151 | jstor=2415876 | bibcode=1964RSPSA.280..383T}}</ref><ref name=Taylor1965>{{cite journal|author=Taylor, G.|year=1965|title=The force exerted by an electric field on a long cylindrical conductor|journal=Proceedings of the Royal Society of London A: Mathematical, Physical and Engineering Sciences|volume=291|issue=1425|pages=145–158|doi=10.1098/rspa.1966.0085|bibcode=1966RSPSA.291..145T}}</ref><ref name=Taylor1969>{{cite journal|author=Geoffrey Ingram Taylor and M. D. Van Dyke|year=1969|title=Electrically Driven Jets|journal=Proceedings of the Royal Society of London A: Mathematical, Physical and Engineering Sciences|volume=313|issue=1515|pages=453–475|doi=10.1098/rspa.1969.0205|bibcode=1969RSPSA.313..453T}}</ref> Taylor modeled the shape of the cone formed by the fluid droplet under the effect of an electric field; this characteristic droplet shape is now known as the [[Taylor cone]]. He further worked with J. R. Melcher to develop the "leaky dielectric model" for conducting fluids.<ref name=MelcherTaylor>Melcher, J. R. & Taylor, G. (1969) Electrohydrodynamics: A Review of the Role of Interfacial Shear Stresses. Annual Review of Fluid Mechanics, 1, 111-146</ref>

The number of publications about electrospray started rising significantly around 1990 (as shown in the figure on the right) when [[John Fenn (chemist)|John Fenn]] (2002 Nobel Prize in Chemistry) and others discovered electrospray ionization for [[mass spectrometry]].

[[File:ElectroSpray-ByYear.png|thumb|log(N+1) number of publications about electrospray by year: patent families from Questel-Orbit, non-patents from Web of Science and from SciFinder-N.]]

==Mechanism==
[[File:Electrospray close-up.JPG|thumb|300 px|A close-up of an electrospray device, with emitter tip in foreground pointing to the right. The jet of ionised spray is visible within the image.]]
To simplify the discussion, the following paragraphs will address the case of a positive electrospray with the high voltage applied to a metallic emitter. A classical electrospray setup is considered, with the emitter situated at a distance <math>d\,</math> from a grounded counter-electrode. The liquid being sprayed is characterized by its viscosity <math>(\mu)\,</math>, surface tension <math>(\gamma)\,</math>, conductivity <math>(\kappa)\,</math>, and relative permittivity <math>(\epsilon_r)\,</math>.

===Effect of small electric fields on liquid menisci===
Under the effect of surface tension, the liquid meniscus assumes a semi-spherical shape at the tip of the emitter. Application of the positive voltage <math>V\,</math> will induce the electric field:<ref>{{cite journal |author1=L. B. Loeb |author2=A. F. Kip |author3=G. G. Hudson |author4=W. H. Bennett | year = 1941 | title = Pulses in negative point-to-plane corona | journal = [[Physical Review]] | volume = 60 | issue = 10 | pages = 714–722 | doi = 10.1103/PhysRev.60.714|bibcode = 1941PhRv...60..714L }}</ref>
:<math>E={2V \over r \ln(4d/r)}</math>
where <math>r\,</math> is the liquid radius of curvature. This field leads to liquid polarization: the negative/positive charge carriers migrate toward/away from the electrode where the voltage is applied. At voltages below a certain threshold, the liquid quickly reaches a new equilibrium geometry with a smaller radius of curvature.

===The Taylor cone===
Voltages above the threshold draw the liquid into a cone. Sir [[Geoffrey Ingram Taylor]] described the theoretical shape of this cone based on the assumptions that (1) the surface of the cone is an equipotential surface and (2) the cone exists in a steady state equilibrium.<ref name="Taylor1964"/> To meet both of these criteria the electric field must have [[azimuth]]al symmetry and have <math>R^{1/2}\,</math> dependence to balance the surface tension and produce the cone. The solution to this problem is:

:<math>V=V_0+AR^{1/2}P _{1/2} (\cos\theta _0)\,</math>

where <math>V=V_0\,</math> (equipotential surface) exists at a value of <math>\theta _0</math> (regardless of R) producing an equipotential cone.  The magic angle necessary for <math>V=V_0\,</math> for all R is a zero of the [[Legendre polynomial]] of order 1/2, <math>P _{1/2} (\cos\theta _0)\,</math>. There is only one zero between 0 and <math>\pi\,</math> at 130.7099°, which is the complement of the Taylor's now famous 49.3° angle.

===Singularity development===
The apex of the conical meniscus cannot become infinitely small. A singularity develops when the hydrodynamic [[relaxation time]] <math>\tau_H={\mu r \over \gamma}</math> becomes larger than the charge [[relaxation time]] <math>\tau_C={\epsilon_r\epsilon_0 \over \kappa}</math>.<ref>{{cite journal | author = Fernández de la Mora, J. |author2=Loscertales, I. G. |name-list-style=amp | title = The current emitted by highly conductive Taylor cones. | journal = [[Journal of Fluid Mechanics]] | year = 1994 | volume = 260 | pages = 155–184 | doi = 10.1017/S0022112094003472|bibcode = 1994JFM...260..155D }}</ref> The undefined symbols stand for characteristic length <math>(r)\,</math> and vacuum permittivity <math>(\epsilon_0)\,</math>. Due to intrinsic varicose instability, the charged liquid jet ejected through the cone apex breaks into small charged droplets, which are radially dispersed by the space-charge.

===Closing the electrical circuit===
The charged liquid is ejected through the cone apex and captured on the counter electrode as charged droplets or positive ions. To balance the charge loss, the excess negative charge is neutralized electrochemically at the emitter. Imbalances between the amount of charge generated electrochemically and the amount of charge lost at the cone apex can lead to several electrospray operating regimes. For cone-jet electrosprays, the potential at the metal/liquid interface self-regulates to generate the same amount of charge as that lost through the cone apex.<ref>{{cite journal |author1=Van Berkel, G. J. |author2=Zhou, F. M. | title = Characterization of an electrospray ion source as a controlled-current electrolytic cell | journal = [[Analytical Chemistry (journal)|Analytical Chemistry]] | year = 1995 | volume = 67 | issue = 17 | pages = 2916–2923 | doi = 10.1021/ac00113a028 }}</ref>

==Applications==

===Electrospray ionization===
{{main|Electrospray ionization}}
Electrospray became widely used as ionization source for mass spectrometry after the [[John Fenn (chemist)|Fenn]] group successfully demonstrated its use as ion source for the analysis of large biomolecules.<ref>{{cite journal |author1=Fenn, J. B. |author2=Mann, M. |author3=Meng, C. K. |author4=Wong, S. F. |author5=Whitehouse, C. M. |title=Electrospray ionization for mass spectrometry of large biomolecules. |journal=[[Science (journal)|Science]] |year=2007 |volume=246 |pages=64–71 |doi=10.1126/science.2675315 |pmid=2675315 |issue=4926 |bibcode=1989Sci...246...64F|citeseerx=10.1.1.522.9458 }}</ref>

===Liquid metal ion source===
A [[liquid metal ion source]] (LMIS) uses electrospray in conjunction with liquid metal to form [[ion]]s.<ref name="Swanson1983">{{cite journal|last1=Swanson|first1=L.W.|title=Liquid metal ion sources: Mechanism and applications|journal=Nuclear Instruments and Methods in Physics Research|volume=218|issue=1–3|year=1983|pages=347–353|issn=0167-5087|doi=10.1016/0167-5087(83)91005-0|bibcode = 1983NIMPR.218..347S }}</ref><ref name="Clampitt1981">{{cite journal|last1=Clampitt|first1=R.|title=Advances in molten metal field ion sources|journal=Nuclear Instruments and Methods in Physics Research|volume=189|issue=1|year=1981|pages=111–116|issn=0167-5087|doi=10.1016/0029-554X(81)90132-4|bibcode = 1981NIMPR.189..111C }}</ref> Ions are produced by field evaporation at tip of the Taylor cone. Ions from a LMIS are used in [[ion implantation]] and in [[focused ion beam]] instruments.

===Electrospinning===
{{main|Electrospinning}}
Similarly to the standard electrospray, the application of high voltage to a polymer solution can result in the formation of a cone-jet geometry. If the jet turns into very fine fibers instead of breaking into small droplets, the process is known as '''electrospinning''' .

===Colloid thrusters===
{{main|Colloid thruster}}
Electrospray techniques are used as low thrust [[Electrically powered spacecraft propulsion|electric propulsion]] [[rocket engine]]s to control [[satellite]]s, since the fine-controllable particle ejection allows precise and effective thrust.

===Deposition of particles for nanostructures===
Electrospray may be used in [[nanotechnology]],<ref>{{cite journal |author=Salata, O.V. |title=Tools of nanotechnology: Electrospray |journal=Current Nanoscience |year=2005 |volume=1 |issue=1 |pages=25–33 |doi=10.2174/1573413052953192 |bibcode=2005CNan....1...25S}}</ref> for example to deposit single particles on surfaces. This is done by spraying [[colloids]] on average containing only one particle per droplet.  The solvent evaporates, leaving an [[aerosol]] stream of single particles of the desired type.  The ionizing property of the process is not crucial for the application but may be used in [[Electrostatic precipitator|electrostatic precipitation]] of the particles.

===Deposition of ions as precursors for nanoparticles and nanostructures===
{{Unreferenced section|date=August 2014}}
Instead of depositing [[nanoparticle]]s, nanoparticles and nano structures can also fabricated in situ by depositing metal ions to desired locations. Electrochemical reduction of ions to atoms and in situ assembly was believed to be the mechanism of nano structure formation.

===Fabrication of drug carriers===
Electrospray has garnered attention in the field of drug delivery, and it has been used to fabricate drug carriers including polymer microparticles used in [[immunotherapy]]<ref>{{cite journal |author=Duong, A.D. |title=Electrospray Encapsulation of Toll-Like Receptor Agonist Resiquimod in Polymer Microparticles for the Treatment of Visceral Leishmaniasis |journal=Molecular Pharmaceutics |year=2013 |volume=10 |issue=3 |pages=1045–1055 |doi=10.1021/mp3005098|pmid=23320733 |pmc=3857017 }}</ref> as well as [[lipoplexes]] used for [[nucleic acid]] delivery.<ref>{{cite journal |author=Wu, Y. |title=Coaxial Electrohydrodynamic Spraying: A Novel One-Step Technique To Prepare Oligodeoxynucleotide Encapsulated Lipoplex Nanoparticles |journal=Molecular Pharmaceutics |year=2009 |volume=6 |issue=5 |pages=1371–1379 |doi=10.1021/mp9000348|pmid=19499922 }}</ref> The sub-micrometer-sized drug particles created by electrospray possess increased dissolution rates, thus increased bioavailability due to the increased surface area.<ref>{{cite journal |author1=Radacsi, N. |author2=Ambrus, R. |author3=Szunyogh, T. |author4=Szabó-Révész, P. |author5=Stankiewicz, A. |author6=van der Heijden, A. |author7=ter Horst, J. H. |name-list-style=amp |title=Electrospray Crystallization for Nanosized Pharmaceuticals with Improved Properties |journal=Crystal Growth & Design |year=2012 |volume=12 |issue=7 |pages=3514–3520 |doi=10.1021/cg300285w}}</ref> The side-effects of drugs can thus be reduced, as smaller dosage is enough for the same effect.

===Air purifiers===
Electrospray is used in some [[air purifier]]s. Particulate suspended in air can be charged by aerosol electrospray, manipulated by an electric field, and collected on a grounded electrode. This approach minimizes the production of [[ozone]] which is common to other types of air purifiers.

==See also==
*[[Flow focusing]]

==References==
{{reflist}}

[[Category:Electric and magnetic fields in matter]]
[[Category:Industrial equipment]]
[[Category:Aerosols]]