Ferrofluid

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Ferrofluid on glass, with a magnet underneath.
Steve Papell invented ferrofluid for NASA in 1963

A ferrofluid (portmanteau of ferromagnetic and fluid) is a liquid that becomes strongly magnetized in the presence of a magnetic field. Ferrofluid was invented in 1963 by NASA's Steve Papell as a liquid rocket fuel that could be drawn toward a pump inlet in a weightless environment by applying a magnetic field.[1]

Ferrofluids are colloidal liquids made of nanoscale ferromagnetic, or ferrimagnetic, particles suspended in a carrier fluid (usually an organic solvent or water). Each tiny particle is thoroughly coated with a surfactant to inhibit clumping. Large ferromagnetic particles can be ripped out of the homogeneous colloidal mixture, forming a separate clump of magnetic dust when exposed to strong magnetic fields. The magnetic attraction of nanoparticles is weak enough that the surfactant's Van der Waals force is sufficient to prevent magnetic clumping or agglomeration. Ferrofluids usually[2] do not retain magnetization in the absence of an externally applied field and thus are often classified as "superparamagnets" rather than ferromagnets.[3]

The difference between ferrofluids and magnetorheological fluids (MR fluids) is the size of the particles. The particles in a ferrofluid primarily consist of nanoparticles which are suspended by Brownian motion and generally will not settle under normal conditions. MR fluid particles primarily consist of micrometre-scale particles which are too heavy for Brownian motion to keep them suspended, and thus will settle over time because of the inherent density difference between the particle and its carrier fluid. These two fluids have very different applications as a result.

Description[edit]

Ferrofluid is the oily substance collecting at the poles of the magnet which is underneath the white dish.

Ferrofluids are composed of nanoscale particles (diameter usually 10 nanometers or less) of magnetite, hematite or some other compound containing iron, and a liquid. This is small enough for thermal agitation to disperse them evenly within a carrier fluid, and for them to contribute to the overall magnetic response of the fluid. This is similar to the way that the ions in an aqueous paramagnetic salt solution (such as an aqueous solution of copper(II) sulfate or manganese(II) chloride) make the solution paramagnetic. The composition of a typical ferrofluid is about 5% magnetic solids, 10% surfactant and 85% carrier, by volume.[4]

Particles in ferrofluids are dispersed in a liquid, often using a surfactant, and thus ferrofluids are colloidal suspensions – materials with properties of more than one state of matter. In this case, the two states of matter are the solid metal and liquid it is in.[5] This ability to change phases with the application of a magnetic field allows them to be used as seals, lubricants, and may open up further applications in future nanoelectromechanical systems.

True ferrofluids are stable. This means that the solid particles do not agglomerate or phase separate even in extremely strong magnetic fields. However, the surfactant tends to break down over time (a few years), and eventually the nano-particles will agglomerate, and they will separate out and no longer contribute to the fluid's magnetic response.

The term magnetorheological fluid (MRF) refers to liquids similar to ferrofluids (FF) that solidify in the presence of a magnetic field. Magnetorheological fluids have micrometre scale magnetic particles that are one to three orders of magnitude larger than those of ferrofluids.

However, ferrofluids lose their magnetic properties at sufficiently high temperatures, known as the Curie temperature.

Normal-field instability[edit]

When a paramagnetic fluid is subjected to a strong vertical magnetic field, the surface forms a regular pattern of peaks and valleys. This effect is known as the normal-field instability. The instability is driven by the magnetic field; it can be explained by considering which shape of the fluid minimizes the total energy of the system.[6]

From the point of view of magnetic energy, peaks and valleys are energetically favorable. In the corrugated configuration, the magnetic field is concentrated in the peaks; since the fluid is more easily magnetized than the air, this lowers the magnetic energy. In consequence the spikes of fluid ride the field lines out into space until there is a balance of the forces involved.[7]

At the same time the formation of peaks and valleys is resisted by gravity and surface tension. It requires energy both to move fluid out of the valleys and up into the spikes, and to increase the surface area of the fluid. In summary, the formation of the corrugations increases the surface free energy and the gravitational energy of the liquid, but reduces the magnetic energy. The corrugations will only form above a critical magnetic field strength, when the reduction in magnetic energy outweighs the increase in surface and gravitation energy terms.[8]

Ferrofluids have an exceptionally high magnetic susceptibility and the critical magnetic field for the onset of the corrugations can be realised by a small bar magnet.

Macrophotograph of ferrofluid influenced by a magnet.

Common ferrofluid surfactants[edit]

The surfactants used to coat the nanoparticles include, but are not limited to:

These surfactants prevent the nanoparticles from clumping together, ensuring that the particles do not form aggregates that become too heavy to be held in suspension by Brownian motion. The magnetic particles in an ideal ferrofluid do not settle out, even when exposed to a strong magnetic, or gravitational field. A surfactant has a polar head and non-polar tail (or vice versa), one of which adsorbs to a nanoparticle, while the non-polar tail (or polar head) sticks out into the carrier medium, forming an inverse or regular micelle, respectively, around the particle. Electrostatic repulsion then prevents agglomeration of the particles.

While surfactants are useful in prolonging the settling rate in ferrofluids, they also prove detrimental to the fluid's magnetic properties (specifically, the fluid's magnetic saturation). The addition of surfactants (or any other foreign particles) decreases the packing density of the ferroparticles while in its activated state, thus decreasing the fluid's on-state viscosity, resulting in a "softer" activated fluid. While the on-state viscosity (the "hardness" of the activated fluid) is less of a concern for some ferrofluid applications, it is a primary fluid property for the majority of their commercial and industrial applications and therefore a compromise must be met when considering on-state viscosity versus the settling rate of a ferrofluid.

A ferrofluid in a magnetic field showing normal-field instability caused by a neodymium magnet beneath the dish

Applications[edit]

Actual[edit]

Electronic devices[edit]

Main article: Ferrofluidic seal

Ferrofluids are used to form liquid seals around the spinning drive shafts in hard disks. The rotating shaft is surrounded by magnets. A small amount of ferrofluid, placed in the gap between the magnet and the shaft, will be held in place by its attraction to the magnet. The fluid of magnetic particles forms a barrier which prevents debris from entering the interior of the hard drive. According to engineers at Ferrotec, ferrofluid seals on rotating shafts typically withstand 3 to 4 psi;[citation needed] additional seals can be stacked to form assemblies capable of higher pressures.

Mechanical engineering[edit]

Ferrofluids have friction-reducing capabilities. If applied to the surface of a strong enough magnet, such as one made of neodymium, it can cause the magnet to glide across smooth surfaces with minimal resistance.

Ferrofluids can also be used in semi-active dampers in mechanical and aerospace applications. While passive dampers are generally bulkier and designed for a particular vibration source in mind, active dampers consume more power. Ferrofluid based dampers solve both of these issues and are becoming popular in the helicopter community, which has to deal with large inertial and aerodynamic vibrations.

Materials science research[edit]

Ferrofluids can be used to image magnetic domain structures on the surface of ferromagnetic materials using a technique developed by Francis Bitter.[9]

Loudspeakers[edit]

Ferrofluids are commonly used in loudspeakers to remove heat from the voice coil, and to passively damp the movement of the cone. They reside in what would normally be the air gap around the voice coil, held in place by the speaker's magnet. Since ferrofluids are paramagnetic, they obey Curie's law and thus become less magnetic at higher temperatures. A strong magnet placed near the voice coil (which produces heat) will attract cold ferrofluid more than hot ferrofluid thus forcing the heated ferrofluid away from the electric voice coil and toward a heat sink. This is a relatively efficient cooling method which requires no additional energy input.[10]

Art[edit]

Some art and science museums have special devices on display that use magnets to make ferrofluids move around specially shaped surfaces in a fountain show-like fashion to entertain guests. Sachiko Kodama is known for her ferrofluid art.

The Australian electronic rock band Pendulum used ferrofluid for the music video for the track, Watercolour. The design house Krafted London was responsible for the ferrofluid FX in the video. The post-metal band Isis also uses a ferrofluid in the music-video for 20 Minutes/40 Years.

Martin Frey, a German designer and technologist, built the pixel-based ferrofluid display SnOil in 2005. The device consists of a 12×12 matrix of electromagnets, allowing the apparatus to display text and run simple games.[11]

Former[edit]

Medical applications[edit]

Several ferrofluids were marketed for use as contrast agents in magnetic resonance imaging, which depend on the difference in magnetic relaxation times of different tissues to provide contrast.[12][13] Several agents were introduced and then withdrawn from the market, including Feridex I.V. (also known as Endorem and ferumoxides, discontinued in 2008;[14] resovist (also known as Cliavist (2001 to 2009);[15] Sinerem (also known as Combidex, withdrawn in 2007;[16] Lumirem (also known as Gastromark (1996[17] to 2012;[18][19] Clariscan (also known as PEG-fero, Feruglose, and NC100150), development of which was discontinued due to safety concerns.[20]

Proposed[edit]

Spacecraft propulsion[edit]

Ferrofluids can be made to self-assemble nanometer-scale needle-like sharp tips under the influence of a magnetic field. When they reach a critical thinness, the needles begin emitting jets that might be used in the future as a thruster mechanism to propel small satellites such as CubeSats.[21]

Analytical instrumentation[edit]

Ferrofluids have numerous optical applications because of their refractive properties; that is, each grain, a micromagnet, reflects light. These applications include measuring specific viscosity of a liquid placed between a polarizer and an analyzer, illuminated by a helium–neon laser.[citation needed]

Medical applications[edit]

Ferrofluids have been proposed for magnetic drug targeting. In this process the drugs would be attached to or enclosed within a ferrofluid and could be targeted and selectively released using magnetic fields.[22]

It has also been proposed for targeted magnetic hyperthermia to convert electromagnetic energy into heat.[23]

It has also been proposed in a form of nanosurgery to separate one tissue from another—for example a tumor from the tissue in which it has grown.[12]

Heat transfer[edit]

An external magnetic field imposed on a ferrofluid with varying susceptibility (e.g., because of a temperature gradient) results in a nonuniform magnetic body force, which leads to a form of heat transfer called thermomagnetic convection. This form of heat transfer can be useful when conventional convection heat transfer is inadequate; e.g., in miniature microscale devices or under reduced gravity conditions.

Ferrofluids of suitable composition can exhibit extremely large enhancement in thermal conductivity (k; ~300% of the base fluid thermal conductivity). The large enhancement in k is due to the efficient transport of heat through percolating nanoparticle paths. Special magnetic nanofluids with tunable thermal conductivity to viscosity ratio can be used as multifunctional ‘smart materials’ that can remove heat and also arrest vibrations (damper). Such fluids may find applications in microfluidic devices and microelectromechanical systems (MEMS).[24]

Optics[edit]

Research is under way to create an adaptive optics shape-shifting magnetic mirror from ferrofluid for Earth-based astronomical telescopes.[25]

Optical filters are used to select different wavelengths of light. The replacement of filters is cumbersome, especially when the wavelength is changed continuously with tunable-type lasers. Optical filters tunable for different wavelengths by varying the magnetic field can be built using ferrofluid emulsion.[26]

Energy harvesting[edit]

Ferrofluids enable an interesting opportunity to harvest vibration energy from the environment. Existing methods of harvesting low frequency (<100 Hz) vibrations require the use of solid resonant structures. With ferrofluids, energy harvester designs no longer need solid structure. One example of ferrofluid based energy harvesting is discussed in the journal article, Electromagnetic ferrofluid-based energy harvester. First a ferrofluid is placed inside a container that is wrapped with a coil of wire. The ferrofluid is then externally magnetized using a permanent magnet. When external vibrations cause the ferrofluid to slosh around in the container, there is a change in magnetic flux fields with respect to the coil of wire. Through Faraday's law of electromagnetic induction, voltage is induced in the coil of wire due to change in magnetic flux.[27]

See also[edit]

References[edit]

  1. ^ US Patent # 3215572 filed Oct 9, 1963 https://www.google.com/patents/US3215572
  2. ^ Albrecht, T.; Bührer, C.; Fähnle, M.; Maier, K.; Platzek, D.; Reske, J. (1997). "First observation of ferromagnetism and ferromagnetic domains in a liquid metal". Applied Physics A: Materials Science & Processing. 65 (2): 215. Bibcode:1997ApPhA..65..215A. doi:10.1007/s003390050569. 
  3. ^ Voit, Kim and Zapka. "Magnetic behavior of coated superparamagnetic iron oxide nanoparticles in ferrofluids". NCBI. Pubmed. Retrieved 2 July 2014. 
  4. ^ Helmenstine, Anne Marie. How to Make Liquid Magnets . chemistry.about.com
  5. ^ Vocabulary List. Education.jlab.org. Retrieved on 2011-11-23.
  6. ^ Andelman & Rosensweig, pp. 20–21.
  7. ^ Andelman & Rosensweig pp. 21, 23; Fig. 11
  8. ^ Andelman & Rosensweig p. 21
  9. ^ Mee, C. D. (1950). The Mechanism of Colloid Agglomeration in the Formation of Bitter Patterns. Proceedings of the Physical Society. Section A, 63(8), 922. doi:10.1088/0370-1298/63/8/122[permanent dead link]
  10. ^ Rlums, Elmars (1995). "New Applications of Heat and Mass Transfer Processes in Temperature Sensitive Magnetic Fluids" (PDF). Brazilian Journal of Physics. 25 (2). 
  11. ^ SnOil - A Physical Display Based on Ferrofluid. freymartin.de
  12. ^ a b Scherer, C.; Figueiredo Neto, A. M. (2005). "Ferrofluids: Properties and Applications" (PDF). Brazilian Journal of Physics. 35 (3A): 718–727. Bibcode:2005BrJPh..35..718S. doi:10.1590/S0103-97332005000400018. 
  13. ^ Wang, YX (December 2011). "Superparamagnetic iron oxide based MRI contrast agents: Current status of clinical application.". Quantitative imaging in medicine and surgery. 1 (1): 35–40. PMC 3496483Freely accessible. PMID 23256052. 
  14. ^ "Feridex - Products - AMAG Pharmaceuticals". Amagpharma.com. Retrieved 2012-06-20. 
  15. ^ Softways. "Magnetic Resonance TIP - MRI Database : Resovist". Mr-tip.com. Retrieved 2012-06-20. 
  16. ^ "AMAG Pharmaceuticals, Inc. Announces Update on Sinerem(TM) in Europe. - Free Online Library". Thefreelibrary.com. 2007-12-13. Retrieved 2012-06-20. 
  17. ^ "Newly Approved Drug Therapies (105) GastroMARK, Advanced Magnetics". CenterWatch. Retrieved 2012-06-20. 
  18. ^ "AMAG Form 10-K For the Fiscal Year Ended December 31, 2013". SEC Edgar. 
  19. ^ "NDA 020410 for GastroMark". FDA. Retrieved 12 February 2017. 
  20. ^ Wang, Yi-Xiang J. (2011). "Superparamagnetic iron oxide based MRI contrast agents: Current status of clinical application". Quantitative Imaging in Medicine and Surgery. 1 (1): 35–40. doi:10.3978/j.issn.2223-4292.2011.08.03. PMC 3496483Freely accessible. PMID 23256052. 
  21. ^ Raval, Siddharth (2013). Novel Thrusters Being Developed for Nanosats. Space Safety Magazine. Available: http://www.spacesafetymagazine.com/2013/10/17/novel-thrusters-developed-nanosats/ Accessed: 10/17/2013.
  22. ^ Kumar, CS; Mohammad, F (14 August 2011). "Magnetic nanomaterials for hyperthermia-based therapy and controlled drug delivery.". Advanced drug delivery reviews. 63 (9): 789–808. PMC 3138885Freely accessible. PMID 21447363. 
  23. ^ Kafrouni, L; Savadogo, O (December 2016). "Recent progress on magnetic nanoparticles for magnetic hyperthermia.". Progress in biomaterials. 5 (3-4): 147–160. doi:10.1007/s40204-016-0054-6. PMID 27995583. 
  24. ^ Shima, P. D.; Philip, John (2011). "Tuning of Thermal Conductivity and Rheology of Nanofluids Using an External Stimulus". The Journal of Physical Chemistry C. 115 (41): 20097. doi:10.1021/jp204827q. 
  25. ^ Hecht, Jeff (7 November 2008). "Morphing mirror could clear the skies for astronomers". New Scientist. 
  26. ^ Philip, John; Jaykumar, T; Kalyanasundaram, P; Raj, Baldev (2003). "A tunable optical filter". Measurement Science and Technology. 14 (8): 1289. Bibcode:2003MeScT..14.1289P. doi:10.1088/0957-0233/14/8/314. 
  27. ^ Bibo, A.; Masana, R.; King, A.; Li, G.; Daqaq, M.F. (June 2012). "Electromagnetic ferrofluid-based energy harvester". Physics Letters A. 376 (32): 2163–2166. doi:10.1016/j.physleta.2012.05.033. 

Bibliography[edit]

  • Andelman, David; Rosensweig, Ronald E. (2009). "The Phenomenology of Modulated Phases: From Magnetic Solids and Fluids to Organic Films and Polymers". In Tsori, Yoav; Steiner, Ullrich. Polymers, liquids and colloids in electric fields: interfacial instabilities, orientation and phase transitions. World Scientific. pp. 1–56. ISBN 978-981-4271-68-4. 
  • Berger, Patricia; Nicholas B. Adelman; Katie J. Beckman; Dean J. Campbell; Ellis, Arthur B.; Lisensky, George C. (1999). "Preparation and properties of an aqueous ferrofluid". Journal of Chemical Education. 76 (7): 943–948. doi:10.1021/ed076p943. ISSN 0021-9584. 

External links[edit]