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Showing posts with label Chemistry. Show all posts
Showing posts with label Chemistry. Show all posts

28 May 2010

Vitamin C Determination by Iodine Titration


Vitamin C (ascorbic acid) is an antioxidant that is essential for human nutrition. Vitamin C deficiency can lead to a disease called scurvy, which is characterized by abnormalities in the bones and teeth. Many fruits and vegetables contain vitamin C, but cooking destroys the vitamin, so raw citrus fruits and their juices are the main source of ascorbic acid for most people.
One way to determine the amount of vitamin C in food is to use a redox titration. The redox reaction is better than an acid-base titration since there are additional acids in a juice, but few of them interfere with the oxidation of ascorbic acid by iodine.
Iodine is relatively insoluble, but this can be improved by complexing the iodine with iodide to form triiodide:
I2 + I- <--> I3-
Triiodide oxidizes vitamin C to form dehydroascorbic acid:
C6H8O6 + I3- + H2O --> C6H6O6 + 3I- + 2H+
As long as vitamin C is present in the solution, the triiodide is converted to the iodide ion very quickly. Howevever, when the all the vitamin C is oxidized, iodine and triiodide will be present, which react with starch to form a blue-black complex. The blue-black color is the endpoint of the titration.
This titration procedure is appropriate for testing the amount of vitamin C in vitamin C tablets, juices, and fresh, frozen, or packaged fruits and vegetables. The titration can be performed using just iodine solution and not iodate, but the iodate solution is more stable and gives a more accurate result.

26 May 2010

How to Make a Smoke Bomb

by Anne Marie Helmenstine
 
Smoke bombs are the easiest and safest do-it-yourself firework project. You only need two inexpensive, non-toxic ingredients and it only takes minutes to make. Watch and learn how you can cook up a smoke bomb at home.

Smoke bombs are easy and fun to make and light. There are several types of smoke bombs you can make, plus you can use the smoke bomb recipe as a starting point for other types of pyrotechnic devices. Try these recipes for making your own smoke bombs.

Classic Smoke Bomb - Video Tutorial

This 
homemade smoke bomb is easy to make and only requires two ingredients.Anne Helmenstine
Smoke bombs are the easiest and safest do-it-yourself firework project. You only need two inexpensive, non-toxic ingredients and it only takes minutes to make up a batch of smoke bombs. Watch and learn how you can cook up a smoke bomb at home.

31 March 2010

Using "corrosion" to make ceramics

Form a metal precursor into a complex, shape, oxidize it, and get a ceramic with the same shape and dimensions.
Sometimes all it takes to solve a problem is to look at it from a completely different angle. For years, ceramists have been limited by their inability to form stable, complex shapes out of brittle metal oxides. Metallurgists, on the other hand, do everything they can to avoid forming metal oxides in the first place (they call them “corrosion products”). They can make any shapes they want out of malleable, ductile metals, but the resulting products don’t have the insulating and structural properties that ceramics have. When ceramic engineer Ken Sandhage joined a group of metallurgists, he didn’t see metal oxides as a problem, but as the beginning of a solution.
When Sandhage was earning his Ph.D. in ceramic engineering at the Massachusetts Institute of Technology in the early 1980s, he selected a metallurgist, Greg Yurek, as his adviser. Although he was the only ceramist in Yurek’s group at the time, this turned out to be an advantage—he gained more exposure than most ceramists to the theory of metal oxidation.
“Most work in this area has been done by metallurgists and electrochemists,” points out Sandhage, “so few ceramists know much about it, even though high-temperature metal oxidation is basically a ceramic process.”
Because metals are consumed by oxidation, metallurgists consider oxidation to be a type of corrosion that they would, of course, like to prevent. On the other hand, Sandhage realized that metal alloys that oxidize rapidly would be great as ceramic precursors or as nonfugitive binders. “This is using oxidation of metals from an opposite perspective. Instead of treating oxidation as metallic corrosion, oxidation can be considered to be an attractive processing route to ceramics or metal–ceramic composites,” Sandhage says. This idea became the basis for the development of the volume-identical metal oxidation (VIMOX) process and similar processes.
Laying the groundwork
But this would come later. First Sandhage had to earn his Ph.D., which involved studying the high-temperature corrosion of alumina in multi-silicate melts (slags) containing magnesia. Sandhage wanted to understand the corrosion of ceramic refractories used in coal gasifiers. Such refractories often contain Al2O3 that can react with the MgO in the slag to form spinel, MgAl2O4. He initially attempted to apply the Turkdogan–Wagner model for the active oxidation of volatile metals (1, 2) to describe the rate of this ceramic corrosion reaction, but he eventually realized a different model was needed.
He observed that in this ceramic reaction, Al2O3 dissolved incongruently in the corrosive slags; the Al2O3 dissolved by first forming a continuous, adherant layer of spinel that then, in turn, dissolved. Under steady-state conditions, the spinel formed and dissolved at equal rates, so that the spinel layer achieved a constant thickness on the Al2O3. Sandhage was able to describe this incongruent dissolution process with the use of the Tedmon model for the oxidation of chromium, which involves the simultaneous formation and volatilization of a continuous oxide layer with a constant thickness (3). As a result of his research, Sandhage realized that his knowledge of metal oxidation could be used effectively in modeling and understanding ceramic reactions and in developing new ceramic processes.
After working in the field of fiber optics for a few years, Sandhage joined his adviser at a start-up company called American Superconductor. Here, Yurek and his colleagues made oxide composite superconductors by selectively oxidizing yttrium, barium, and copper from alloys containing these elements and silver, resulting in a YBa2Cu3O7–Ag composite.
After 3½ years at American Superconductor, Sandhage decided to pursue oxidation-based research and develop other types of ceramics and ceramic composites in an academic setting. In 1991, he became a professor in materials science and engineering at Ohio State University, where he had to come up with a novel area of research. With his background in oxidation and a seed grant from the university, Sandhage started research in the oxidation of alloys containing alkaline and alkaline earth metals.
Sandhage went back to work done in the 1920s, when Pilling and Bedworth were looking at why oxidation rates differ in metals (4). Pilling and Bedworth considered the volume of oxide produced divided by the volume of metal consumed (now known as the Pilling–Bedworth ratio or PBR) to be an important parameter, and they evaluated this ratio for several metals. Most metals have a PBR > 1, whereas alkali and alkaline earth metals tend to have a PBR < 1 (Table 1).
Sandhage believed that if he could combine the right types of metals to form a precursor, so that the net volume change upon oxidation of the precursor was small or zero, he could convert complex-shaped metal-bearing precursors by oxidation into near net-shaped ceramic materials. (A net-shaped material has the same shape and size before and after processing. Most ceramics contain pores that cause them to shrink or deform when they are fired.) Metals tend to be ductile and relatively easy to form into complex shapes. On the other hand, ceramics traditionally have been difficult to make into complex parts without using expensive diamond machining to achieve the desired dimensions. By starting with easily formed metal precursors, then oxidizing the precursors to yield ceramics that retain the precursor shape and dimensions, near net-shaped ceramics can be produced without the need for ceramic machining. The VIMOX process is based on oxidizing different metals in a precursor (some of which expand, some of which contract upon oxidation) to limit the volume change upon conversion into a ceramic compound.
The VIMOX process
Sandhage and his students toiled for several years to demonstrate that the VIMOX process could be used to produce a number of technically useful ceramics and composites in near net shapes, such as those shown in Table 2 (6). During this time, Sandhage received support from several federal and state agencies for such research. In 1995, he was granted a patent for the VIMOX process (7).
The VIMOX process comprises several steps (Figure 1). First, precursors are prepared by mechanically alloying powders of metals and oxides to obtain a uniformly dispersed mixture with the proper phase content (for minimal volume change upon oxidation) and overall composition (for the desired final ceramic or ceramic composite). Next, the mixed powders are compacted and shaped by one or more of several metallurgical processes (e.g., pressing, rolling, drawing, machining). The amount of ductile metal in the precursor determines the type of fabrication process that is used. Approximately 30 vol% of ductile metal is used for pressing and about twice that for rolling and drawing.
Once the preforms are made into desired shapes, they are oxidized and converted into the final ceramic or ceramic composite using several heat treatments. These heat treatments can effect oxidation, compound formation, microstructural tailoring, or other desired processes. By carefully controlling the phase content of the precursor and the heat treatments, near net-shaped ceramics and composites can be produced without costly post-oxidation machining steps. Furthermore, because modest temperatures (300–500 °C) can be used to oxidize alkaline earth metals, the grain size of the resulting oxide can be quite small, so that subsequent sintering also can be done at modest temperatures. (Dense BaTiO3 has been produced at 1080 °C, several hundred degrees lower than normal, without a sintering aid.)
A casting process can also be used to prepare the precursors (Figure 2). A block of solid alkaline earth metal is placed in contact with a porous preform in the desired shape. The metal is melted under an inert atmosphere, causing it to infiltrate the pores of the preform. Heating the preform under oxygen produces a ceramic in the shape of the original preform that contains the alkaline earth metal.
One advantage of precursors containing alkaline earth metals is that they are ductile at room temperature, which makes them easy to machine and form into shapes. They are also easy to cast into shapes because of their low melting temperatures. Thus, the VIMOX process using these materials can make ceramics that retain shape, volume, and dimensions after oxidation, usually to within 1%.
In contrast, conventional ceramic processes require the use of organic binders that must be burned off the ceramic preform, producing high internal porosity. Such porosity produces significant distortions and shrinkage upon sintering, 20% or more, depending on the amount of binder used to form the ceramic preform (more for rolling, less for pressing). Since 1991, Sandhage’s group has produced a variety of functional ceramics by the VIMOX process, including biocompatible phosphates, ionically conducting cerates, dielectric titanates, superconducting cuprates, magnetic ferrites, and refractory aluminates and aluminosilicates for biomedical, sensor, electronic, magnetic, optical, chemical, and high-temperature applications.
Displacive compensation of porosity
One limitation of the VIMOX process is the thickness of parts produced. Parts thicker than several centimeters can take relatively long times (tens of hours) to oxidize completely. This limitation has recently been overcome with another oxidation-based process developed by Sandhage’s group, known as the DCP (displacive compensation of porosity) process. In 1998, graduate student Pragati Kumar was preparing preforms to spinel by infiltrating molten magnesium into porous Al2O3 and then solidifying the magnesium. He noticed that the Al2O3 had oxidized some of the magnesium to MgO during infiltration. After realizing that an oxidation–reduction reaction was occurring during infiltration, Sandhage and Kumar calculated the change in ceramic volume for this reaction:
3{Mg} + Al2O3 → 3MgO + 2{Al}
where {Mg} and {Al} refer to magnesium and aluminum dissolved in molten metal. To their surprise, more ceramic volume was generated than was consumed. They then decided to let this reaction run to completion during infiltration (reactive infiltration). They found that porous alumina preforms could be converted completely into dense, high MgO-bearing components with little change in shape or dimensions.
In other words, the increase in volume caused by the displacement reaction could be used to compensate for the porosity in the starting preform; hence, the term DCP. Because the oxygen source for such a displacement reaction is the solid oxide that is distributed throughout the preform, long-range diffusion of oxygen from outside of the preform is not required to complete this reaction. Once the molten metal fully infiltrates the preform (which occurs rapidly), the time required for complete reaction does not depend on the size of the preform. Sandhage’s group has since identified a variety of other volume-increasing displacement reactions that can be used to make components with a high ceramic content (Table 3).
The DCP process consists of two steps: infiltration of a molten metal into a porous, shaped ceramic preform and an in situ reaction of the molten metal with the ceramic preform (Figure 3). Because the volume of solid ceramic produced is larger than the original volume in the preform, dense composites with relatively high ceramic contents can be synthesized. If the metallic product of the reaction is solid at the reaction temperature, dense ceramic–metal composites are produced. If the metallic product is molten, the metallic liquid is squeezed out of the preform as the pores become filled with ceramic, and the composite contains a very high ceramic content. This latter process is called “pressureless reversible infiltration of molten alloys by the displacive compensation of porosity” (PRIMA-DCP).
A range of compositions and phase contents can be produced by varying the melt composition, the preform porosity, and the preform phase content. (The metal reinforcements in the composites can be continuous or discontinuous.) For example, composites of MgO/Mg–Al with MgO contents ranging from 70 to 86 vol% can be produced by varying the preform porosity from 47 to 29% (17). Composites with >80 vol% MgO were found to be electrically insulating; sufficient molten metal was extruded from the preform during reaction that only discontinuous particles of metal remained in the composite upon cooling to room temperature.
The DCP process also has been used to produce co-continuous MgAl2O4/Fe–Ni–Al composites by pressureless reactive casting of Mg–Al liquids at 900 °C into porous Fe/NiAl2O4 preforms with the net reaction:
4/3{Mg0.75Al0.25} + xFe(s) + NiAl2O4 → MgAl2O4 + y[Fex/yNi1/yAl1/(3y)]
where y = x + 4/3; 4 ≤ x ≤ 8; and the brackets {} and [] refer to liquid and solid alloys, respectively.
Composites with a variety of oxide and metal alloy compositions can be produced directly by DCP or PRIMA-DCP processes for use in electrical, refractory, insulating, or engine applications.
Nonoxide ceramic composites
The DCP process can also be used to make composites containing nonoxide ceramics. Sandhage recently worked with several senior undergraduate students to fabricate ZrC–W composites by the reactive casting of a Zr2Cu liquid into porous WC preforms (18). The net displacement reaction in this case is
0.5{Zr2Cu} + WC → ZrC + W + 0.5{Cu}
The residual molten copper does not form stable compounds with ZrC or tungsten and has minimal effect on the high-temperature resistance of the final material. Copper also has the advantage of lowering the reactive infiltration temperature and can be extruded out of the preform as the pores are filled. Dense, near net-shaped composites were produced within 2 h at 1200 °C and 1 h at 1300 °C.
Such composites are attractive for high-temperature applications where excellent resistance to creep, erosion, or thermal cycling is required, for example, throat inserts of rocket exhaust nozzles. Current nozzle liners are based on carbon or tungsten. Although tungsten exhibits minimal oxidation in solid-fuel rocket nozzles, and it has a very high melting point and good toughness, it is heavy (19.3 g/cm3) and relatively difficult to form into specific shapes at room temperature. Combining tungsten with ZrC is an alternative because ZrC is relatively lightweight (6.63 g/cm3) and chemically compatible with tungsten. This combination has better strength and toughness than ZrC alone.
However, the ZrC–W composites prepared by conventional methods are difficult to sinter, requiring hot pressing at 2000 °C and 20 MPa. They are also expensive to machine. Sandhage and his students have shown that the DCP process can produce ZrC–W composites in the desired shapes without machining at 1200 °C and ambient pressure. Furthermore, functionally graded ZrC–W composites can be produced by carefully tailoring the distribution of tungsten and WC in the starting preforms (19).
Sandhage has purchased a larger furnace for scaling up the DCP process. This furnace will be capable of making rocket nozzles that can be tested in rocket burner rigs at Edwards Air Force Base, CA (in collaboration with Wesley Hoffman of Edwards AFB).
Sandhage has also submitted a proposal to the U.S. Army to evaluate the use of the DCP process for making custom-tailored body armor. In this case, a plaster of Paris mold the exact shape of the torso is produced first. A slurry of silicon carbide is then cast into the mold. After drying, this porous preform is then infiltrated and reacted with a boron-bearing liquid to convert the porous SiC preform into lightweight, hard B4C–SiC composite armor that retains the preform shape and dimensions:
4{B} + (1+x)SiC → B4C + xSiC + {Si}
where {B} and {Si} refer to boron and silicon dissolved in a liquid solution. By tailoring the starting porosity and SiC particle size in the cast preform, Sandhage expects that near net-shaped B4C–SiC composites with tailored phase contents can be produced.
Although DCP is somewhat of an offshoot of VIMOX and can also produce net shapes at lower temperatures than conventional processes, there are major differences between the two approaches (Table 4).
Joint efforts expand applications
Sandhage is working with other Ohio State researchers to develop new applications for the VIMOX process. He has teamed up with Alan Litsky, a professor of orthopedics, to develop graded oxide coatings for metal hip implants. The pure oxide coatings of hydroxyapatite currently used do not adhere well to the underlying metal stem for long periods. A new graded hydroxyapatite coating concept has been demonstrated with the VIMOX process; the next step will be to make implants for animal studies after additional funding is obtained.
Sheik Akbar, a colleague in the materials science and engineering department, and Sandhage are investigating making TiO2-doped MgCr2O4 humidity sensors that can be reused after exposure to high temperatures. The VIMOX process produces near net-shaped sensors that can be positioned close to the ceramic ware to allow for local measurement of the drying rate. Placed on kiln cars, these humidity sensors could determine the drying rates of ceramic ware to allow for energy- and time-efficient rate-controlled drying.
One novel application of DCP takes advantage of marine biology, namely a type of green algae called diatoms. These single-celled creatures form microshells with intricate shapes and with submicrometer features. While on sabbatical in 1991 as a Humboldt Fellow in Germany, Sandhage met Australian marine biologist Monica Schoenwaelder, an expert on diatoms. After discussing her work, Sandhage came up with the idea of using diatoms as templates to make near net-shaped microdevices.
One application would be drug delivery biocapsules. Capsule-shaped diatoms, made of amorphous silica, have been reacted with magnesium to form MgO capsules that retain the diatom capsule shape. Because MgO is more biocompatible than SiO2,drugs could be easily and safely administered in MgO capsules. Capsule-shaped diatoms could also be converted into CaO, adding the benefit of dietary calcium to those who need it.
Eventually, Sandhage believes, genetic engineering can be used to tailor the diatom shape, and he has coined the term “genetically engineered microdevices” or GEMs. DCP would be used to tailor the composition and convert the silica into other ceramics or ceramic composites. Sandhage has applied for a patent (20) and expects to obtain seed money for further development.
“In addition to their size and shape advantages,” adds Sandhage, “diatoms have an extremely high replication rate of 3–8 times per day. This means you could theoretically make 1 billion similar microdevices in just 10 days. Genetically engineered diatoms could be used as biofactories to mass-produce large numbers of micro templates with similar tailored 3-D shapes that could then be converted by reaction into microdevices with tailored compositions for microsensors, micromotors, microrobots, etc.”
Bringing the products to market
After spending a decade conducting several millions of dollars worth of oxidation-based research and obtaining seven patents in metal oxidation technology, Sandhage is now actively working to commercialize the VIMOX and DCP processes. Orton Ceramic Foundation (Westerville, OH) is continuing development of the MgCr2O4 humidity sensors.
Sandhage believes that the VIMOX and DCP processes have great potential for commercially manufacturing ceramic and ceramic composite components with complex shapes. He warns, however, that “it is not easy to insert new processes into traditional ceramic manufacturing companies, especially since these companies are often not familiar with powder metallurgy or casting metallurgy-based processes. This requires a significant change in mindset.” Sandhage is thinking about starting his own company that will act as an intermediary to manufacture and test components.
Acknowledgments
Ken Sandhage has received research funding from the National Science Foundation, the U.S. Department of Energy, the U.S. Air Force Office of Scientific Research, and the Edison Materials Technology Center (Dayton, OH).

Back to the basics
The basic kinetic mechanism or mechanisms by which oxides undergo incongruent reduction with molten metals (DCP reactions) are not well understood. Sandhage and colleague Robert Snyder at Ohio State recently were awarded a National Science Foundation grant to study these reactions. The main objective of this research is to develop a fundamental understanding of the rate-limiting steps and microstructural evolution by which a solid oxide undergoes incongruent reduction with a reactive metallic liquid. A better knowledge of such reaction mechanisms will help predict how changes in processing conditions will affect reaction times, composite microstructure, and, consequently, the composite properties. In situ X-ray diffraction (XRD) will be used to track, in real time, the formation of spinel (MgAl2O4) on Al2O3 surfaces immersed under molten Mg–Al layers. This is possible because the absorption of MoKα X-rays by Mg–Al liquids is relatively low. This is the first time that dynamic X-ray analysis will be used to study liquid metal–solid ceramic displacement reactions underneath molten metal (Figure 4).
The in situ XRD method requires making novel graphite heating cells that are transparent to X-rays. With these heating cells, the entire preform and surrounding melt can be equilibrated thermally, avoiding the steep thermal gradients normally seen when heating strips are used. Dynamic in situ thermogravimetric analyses will also be used to determine the steady-state rate of incongruent reduction under well- controlled conditions.
References
  1. Turkdogan, E. T.; Grieveson, P.; Darken, L. S. J. Phys. Chem. 1963, 67, 1647–1654.
  2. Wagner, C. Corros. Sci. 1965, 5, 751–764.
  3. Tedmon, C. S., Jr. J. Electrochem. Soc. 1966, 113, 766–768.
  4. Pilling, N. B.; Bedworth, R. E. J. Inst. Metals 1923, 29, 530–591.
  5. Encyclopedia of Materials: Science and Technology; Buschow, K.H.J., Ed.; Elsevier: New York, 2001.
  6. Sandhage, K. H.; Allameh, S. M.; Kumar, P.; Schmutzler, H. J.; Viers, D.; Zhang, X.-D. Mater. Manuf. Processes 2000, 15, 1–28.
  7. Sandhage, K. H. U.S. Patent 5,447,291, 1995.
  8. Kumar, P.; Sandhage, K. H. J. Mater. Res. 1998, 13, 3423–3435.
  9. Viers, D. S.; Sandhage, K. H. J. Am. Ceram. Soc. 1999, 82, 249–252.
  10. Schmutzler, H. J.; Antony, M. M.; Sandhage, K. H. J. Am. Ceram. Soc. 1994, 77, 721–729.
  11. Ward, G. A.; Sandhage, K. H. J. Am. Ceram. Soc. 1997, 80, 1508–1516.
  12. Saw, E.; Sandhage, K. H.; Gallagher, P. K.; Litsky, A. S. Mater. Manuf. Processes 2000, 15, 29–45.
  13. Schmutzler, H. J.; Sandhage, K. H.; Nava J. C. J. Am. Ceram. Soc. 1996, 79, 1575–1584.
  14. Citak, R.; Rogers, K. A.; Sandhage, K. H. J. Am. Ceram. Soc. 1999, 82, 237–240.
  15. Jain, A.; Sandhage, K. H. In Innovative Processing and Synthesis of Ceramics, Glasses, and Composites IV; Bandal, N. P., Singh, J. P., Eds.; American Ceramic Society: Westerville, OH, 2000; pp 15–23.
  16. The Powder Diffraction File [CD-ROM], International Centre for Diffraction Data: Newtown Square, PA (2001 update).
  17. Kumar, P.; Sandhage, K. H. J. Mater. Sci. 1999, 34, 5757–5769.
  18. Dickerson, M. B.; Unocic, R. R.; Guerra, K. T.; Timberlake, M. J.; Sandhage, K. H. In Innovative Processing and Synthesis of Ceramics, Glasses, and Composites IV; Bandal, N. P., Singh, J. P., Eds.; American Ceramic Society: Westerville, OH, 2000; pp 25–31.
  19. Dickerson, M. B.; Snyder, R. L.; Sandhage, K. H., Presented at the 25th Annual Cocoa Beach Conference and Exposition, Cocoa Beach, FL, Jan 2001. Submitted for publication.
  20. Sandhage, K. H. U.S. Patent application pending.

Laurel M. Sheppard is a freelance writer based in Hilliard, OH (lashpubs@infinet.com). She has a B.S. in ceramic engineering from Ohio State University, Columbus.

A simple process for removing chloroform from water

Chloroform in water is a byproduct of the chlorination process (1). Bathing or showering in chlorinated tap water exposes individuals to chloroform by ingestion, inhalation, or dermal contact. Some epidemiological studies have suggested that exposure to chlorinated water causes bladder cancer (2, 3) and is associated with rectal cancer (3) and potential birth defects (4). Several studies, including some based on exhaled breath analysis, suggest that significant dermal exposure to chloroform occurs while showering, and the dose is roughly comparable to that resulting from inhalation (5, 6). (Breath analysis measures the time elapsed between first skin contact and when the chloroform is first observed in the exhaled breath.) Other studies have extended this work to swimming in indoor pools (7, 8). Most of these investigations have used breath measurements to determine total exposure.
We have proposed a process to remove chloroform from water. The process was tested and found to be adequate by public health standards for water that contains a concentration of chloroform up to 6.7 g/L.

Figure 1
Figure 1. A two-step process removes chloroform from water. Contaminated water is fed into a convection tank, where it passes through a “curtain” of compressed air. The air removes the chloroform from the water, and a charcoal bed removes the chloroform from the air. The purified air is released to the atmosphere.
We use an air curtain convection tank (Figure 1) coupled with a carbon bed system located at the air exit (9–11). This process provides rapid, efficient mass transfer of the chloroform from the liquid phase to the gas phase (11). The location of the air curtain and the flow rate of the compressed air have been optimized with respect to mass transfer and good mixing. Compressed air is injected into the convection tank through series of 16 equally spaced perforations (1.6 mm diam) in a single row along a transverse tube to create fluid circulation with an air curtain. The tube is placed centrally across the width of the bottom of the tank.
Saka and Doi (10) found that carbonized woody materials effectively adsorb chloroform from water and benzene from the atmosphere. Using their technique, we fed the air exiting the aerated tank into a charcoal-packed bed. This air contains chloroform and a small amount of water. The packed bed consists of a Perspex U tube (2 cm diam, 10 cm high) filled with granulated charcoal 0.5 mm in diameter. This shape was the most effective for reducing the concentration of chloroform in air.
We started with 5 L of water containing 18.25 g of chloroform. Air at 5 L/min aerated the water via the perforated pipe. The air exited the water tank, then passed through the carbon bed. The exhaust from the carbon bed was vented to the atmosphere.
(Figure 2) shows the change in the concentration of chloroform in water when air was blown into the contaminated water for 90 min. Gas chromatography was used to analyze for chloroform in the water. After 90 min, the concentration of chloroform in water went almost to zero. The chloroform was then removed from the air exiting the tank using the U-shaped charcoal bed. The air exiting the carbon bed was assumed to be free of chloroform (10).
This simple, novel process is very effective in eliminating chloroform from water. We believe that this method will be useful in protecting our environment from such a harmful pollutant.

References

  1. International Agency for Research on Cancer. Chlorinated Drinking Water; Chlorinated By-Products; Some Other Halogenated Compounds; Cobalt and Cobalt Compounds. IARC Monographs on the Evaluation of Carcinogenic Risk to Humans, Vol. 52; IARC: Lyon, France, 1991.
  2. Cantor, K. P., et al. J. Natl. Cancer Inst. 1987, 79, 1269–1279.
  3. Morris, R. D.; Audet, A. M.; Angelillo, I. F.; Chalmers, T. C.; Mosteller, F. Am. J. Public Health 1992, 82, 955–963.
  4. Bove, F.; Fulcomer, M. C.; Savrin, J. E. Am. J. Epidemiol. 1995, 141, 850–862.
  5. Jo, W. K.; Weisel, C. P.; Lioy, P. J. Risk Anal. 1990, 10, 575–580.
  6. Wester, R. C.; Maibach, H. I. Environ. Sci. Pollut. Control Ser. 1994, 9, 149–165.
  7. Wallace, L. A.; Nelson, W. C.; Pellizzari, E. D.; Raymer, J. H. J. Expo. Anal. Environ. Epidemiol. 1997, 7, 141–163.
  8. Lindstrom, A. B.; Pleil, J. D.; Berkoff, D. C. Environ. Health. Perspect. 1997, 105, 636–642.
  9. Fenelon, J. M.; Moore, R. C. Occurrence of Volatile Organic Compounds in Ground Water in the White River Basin, Indiana, 1994–1995; U.S Geological Survey Fact Sheet 138-96, U.S. Government Printing Office: Washington, DC, 1996.
  10. Saka, S.; Doi, M. Mater. Sci. Res. Int. 1998, 4, 249–253.
  11. Pleil, J. D.; Lindstrom, A. B. Clin. Chem. 1997, 43, 723–730.


Omar Chaalal is an associate professor of chemical engineering in the University General Requirements Unit at United Arab Emirates University (PO Box 17720, Al-Ain Abu Dhabi, U.A.E.; ochaalal@uaeu.ac.ae).
Ali Dowaidar is a research assistant in the chemical engineering department at United Arab Emirates University.

11 February 2010

Colored Flowers

Easy and Fun Color Science Project

By , About.com Guide

Blue is not a usual daisy color, but you can make a blue daisy using chemistry!

Blue is not a usual daisy color, but you can make a blue daisy using chemistry!

Frances Twitty, Getty Images
It's easy to make your own colored flowers, especially carnations and daisies, but there are a couple of tricks that help ensure great results. Here's how you do it.

Colored Flower Materials

  • fresh flowers, preferably white - don't use wilted flowers since they might not be able to absorb water well. Good choices include daisies and carnations.
  • food coloring
  • warm water

Make Colored Flowers

  • Trim the stems of your flowers so they aren't excessively long.

  • Make a slanted cut at the base of the stem under water. The cut is slanted so that the stem won't sit flat on the bottom of the container. A flat cut can prevent the flower from taking in water. Make the cut underwater to prevent air bubbles from forming in the tiny tubes at base of the stem, which would prevent water/color from being drawn up.

  • Add food coloring to a glass. You're looking at about 20-30 drops of food coloring per half cup of warm water. Warm water will be taken more readily than cold water.

  • Set the damp stem of the flower in the colored water. The petals should become colored after a few hours. It may take as long as 24 hours, however, depending on the flower.

  • You can set the colored flowers in plain water or flower preservative, but they will continue to drink water, changing the pattern of the color over time.

Getting Fancy

You can slit the stem up the middle and put each side in a different color to get bi-colored flowers. What do you think you will get if you put half of the stem in blue dye and half in yellow dye? What do you think will happen if you take a colored flower and put its stem in dye of a different color?

How It Works

A few different processes are involved in plant 'drinking' or transpiration. As water evaporates from flowers and leaves, the attractive force between water molecules called cohesion pulls more water along. Water is pulled up through tiny tubes (xylem) that run up a plant's stem. Although gravity might want to pull the water back down toward the ground, water sticks to itself and these tubes. This capillary action keeps water in the xylem in much the same way as water stays in a straw when you suck water through it, except evaporation and biochemical reactions provide the initial upward pull.

Chalk Chromatography

Separate Pigments Using Chalk Chromatography

By , About.com Guide

These chalk chromatogaphy examples were made using chalk with ink and food coloring.

These chalk chromatogaphy examples were made using chalk with ink and food coloring.

Anne Helmenstine
Chromatography is a technique used to separate components of a mixture. There are many different types of chromatography. While some forms of chromatography require expensive lab equipment, others can be performed using common household materials. For example, you can use chalk and alcohol to perfom chromatography to separate the pigments in food colorings or inks. It's a safe project and also a very quick project, since you can see bands of color forming within minutes. After you've finished making your chromatogram, you'll have colored chalk. Unless you use a lot of ink or dye, the chalk won't be colored all the way through, but it will still have an interesting appearance.

Chalk Chromatography Materials

  • chalk
  • alcohol (isopropyl alcohol or rubbing alcohol seems to work best)
  • ink, dye, or food coloring
  • small jar or cup
  • plastic wrap
  1. Apply your ink, dye or food coloring to a piece of chalk about 1 cm from the end of the chalk. You can place a dot of color or stripe a band of color all the way around the chalk. If you are mainly interested in getting bands of pretty colors rather than separating individual pigments in the dye, then feel free to dot multiple colors, all in the same place.

  2. Pour enough rubbing alcohol into the bottom of a far or cup so that the liquid level is about half a centimeter. You want the liquid level to be below the dot or line on your piece of chalk.

  3. Place the chalk in the cup so that the dot or line is about half a centimeter higher than the liquid line.

  4. Seal the jar or put a piece of plastic wrap over the cup to prevent evaporation. You can probably get away with not-covering the container.

  5. You should be able to observe the color rising up the chalk within a few minutes. You can remove the chalk whenever you are satisfied with your chromatogram.

  6. Let the chalk dry before using it for writing.

Chalk Chromatography

Separate Pigments Using Chalk Chromatography

By , About.com Guide

These chalk chromatogaphy examples were made using chalk with ink and food coloring.

These chalk chromatogaphy examples were made using chalk with ink and food coloring.

Anne Helmenstine
Chromatography is a technique used to separate components of a mixture. There are many different types of chromatography. While some forms of chromatography require expensive lab equipment, others can be performed using common household materials. For example, you can use chalk and alcohol to perfom chromatography to separate the pigments in food colorings or inks. It's a safe project and also a very quick project, since you can see bands of color forming within minutes. After you've finished making your chromatogram, you'll have colored chalk. Unless you use a lot of ink or dye, the chalk won't be colored all the way through, but it will still have an interesting appearance.

Chalk Chromatography Materials

  • chalk
  • alcohol (isopropyl alcohol or rubbing alcohol seems to work best)
  • ink, dye, or food coloring
  • small jar or cup
  • plastic wrap
  1. Apply your ink, dye or food coloring to a piece of chalk about 1 cm from the end of the chalk. You can place a dot of color or stripe a band of color all the way around the chalk. If you are mainly interested in getting bands of pretty colors rather than separating individual pigments in the dye, then feel free to dot multiple colors, all in the same place.

  2. Pour enough rubbing alcohol into the bottom of a far or cup so that the liquid level is about half a centimeter. You want the liquid level to be below the dot or line on your piece of chalk.

  3. Place the chalk in the cup so that the dot or line is about half a centimeter higher than the liquid line.

  4. Seal the jar or put a piece of plastic wrap over the cup to prevent evaporation. You can probably get away with not-covering the container.

  5. You should be able to observe the color rising up the chalk within a few minutes. You can remove the chalk whenever you are satisfied with your chromatogram.

  6. Let the chalk dry before using it for writing.

27 January 2010

Mosquito control with Bioinsektisida


So far for controlling Aedes aegypti mosquito and Anopheles, there are still many people who use chemicals (insecticide). In fact, it's not environmentally friendly and had no indication of resistance of mosquitoes Aedes aegypti and Anopheles in various places on certain types of insecticides.

"To Aedes aegypti is a tendency organofosfat tolerant of compounds," said Head of Research Center of Disease Vectors and Reservoir, Ministry of Health, Dr MS Damar Tri Boewono in Republika. This is Organofosfat chemicals to control mosquitoes and larva. For this reason, he continued, the Research Center of Disease Vectors Reservoir bioinsektisida efficacy test Bacillus thuringiensis and Bacillus sphaericus against mosquito larvae of malaria vectors and dengue hemorrhagic fever (DHF). "The result was good enough," said Rosin.

Research carried out is an oasis (as much as a cotton buds) from cultured spores of Bacillus thuringiensis inserted into the coconut water. Coconut intact opened slightly. Having entered the spores then closed again. After one week left in the coconut, Bacillus sphaericus and Bacillus thurigiensis is already a lot, obviously the laboratory Damar already recommended by the WHO (World Health Organization) for testing insecticides that will be performed by a program or households.

He further said that if the target of bioinsektisida is the Anopheles mosquito larvae, the spores must be floating. Conversely, if the target Aedes aegypti mosquito larvae spores must then be at the bottom. Now, bioinsektisida is already used by Newmont and Freeport. Thus, Damar said, when bioinsektisida will be used to control the Anopheles larva and Aedes aegypti, the material must be designed as such in accordance with the behavior of the mosquito larva is. He admitted that bioinsektisida is safe, no side effects, and environmentally friendly.

According to him, never existed in the public demonstration to prove the security bioinsektisida. Way, bioinsektisida incorporated into drinking water, then drink. Proved that people who drink do not die, he explained. In another part he says with organofosfat mosquito control can still be, but should increase the dose. Thus the cost is more expensive and resistance will be higher. "If I am telling the truth from the farm, this organofosfat more toxic to the soil," said Rosin.

Once insekstisda material goes into the ground, he will carry the rain water and will be collected in one place. Mosquitoes will breed there and will adapt to the environment so that the resistance will emerge. Both these spores, he explained, was sold in the market. These spores must be stored in a cool place so as not to die.

Source: Republika (December 11, 2004)

25 January 2010

Supercooling Water

How to Supercool Water

By , About.com Guide

You can cool water below its stated freezing point and then crystallize it into ice on command. This is known as supercooling. These are step-by-step instructions for supercooling water at home.
Supercooling Water - Method #1
The simplest way to supercool water is to chill it in the freezer.

1. Place an unopened bottle of distilled or purified water (e.g., with reverse osmosis) in the freezer. Mineral water or tap water will not supercool very well because they contain 'impurities' that can lower the freezing point of the water or else serve as nucleation sites for crystallization.

2. Allow the bottle of water to chill, undisturbed, for about 2-1/2 hours. The exact time needed to supercool the water varies depending on the temperature of your freezer. One way to tell your water is supercooled is to put a bottle of tap water (impure water) into the freezer with the bottle of pure water. When the tap water freezes, the pure water is supercooled. If the pure water also freezes, you either waited too long, somehow disturbed the container, or else the water was insufficiently pure.

3. Carefully remove the supercooled water from the freezer.

4. You can initiate crystallization into ice in several different ways. Two of the most entertaining ways to cause the water to freeze are to shake the bottle or to open the bottle and pour the water onto a piece of ice. In the latter case, the water will often freeze backwards from the ice cube back into the bottle.

Supercooling Water - Method #2
If you don't have a couple of hours, there is a quicker way to supercool water.

1. Pour about 2 tablespoons or 20 ml of distilled or purified water into a very clean glass.

2. Place the glass in a bowl of ice such that the level of the ice is higher than the level of water in the glass. Avoid spilling any ice into the glass of water.

3. Sprinkle a couple of tablespoons of salt onto the ice. Do not get any of the salt in the glass of water.

4. Allow about 15 minutes for the water to cool below freezing. Alternatively, you can insert a thermometer into the glass of water. When the temperature of the water is below freezing, the water has been supercooled.

5. You can make the water freeze by pouring it over a piece of ice or by dropping a small piece of ice into the glass.


Anne Marie Helmenstine, Ph.D.
Chemistry Guide

15 January 2010

Teknologi Proses Produksi Pupuk ZK (Bagian 1)

by Anita Pravitasari on 30/07/09 at 8:33 pm | No Comment | Print article | Email article


Potassium Sulphate (ZK) biasa digunakan sebagai pupuk pada tanaman

Potassium Sulphate (ZK) atau biasa disebut Sulphate of Potash (SOP) telah dikenal sejak abad ke-14 yang merupakan garam berwarna putih dan memiliki sifat tidak mudah terbakar serta larut di dalam air. ZK digunakan sebagai pupuk yakni sumber senyawa kalium dan sulfur pada tanaman perkebunan seperti rami, kapas, dan tembakau. Di Indonesia pupuk ini tidak disubsidi sehingga harganya relatif tinggi di pasaran. Bahan baku sulfat alami untuk pembuatan ZK yang berasal dari pertambangan antara lain adalah lanbeinite (K2SO4.2MgSO4), leonite (K2SO4.MgSO4.4H20), schoenite (K2SO4.MgSO4.6H2O), dan glaserite (K3Na(SO4)2). Pertambangan sumber batuan tersebut banyak terdapat di negara Rusia, Kanada, benua Eropa, Israel, negara-negara timur tengah, Cina, Thailand, Kongo, dan Amerika Serikat.

Pemilihan proes produksi yang digunakan di dalam suatu pabrik pupuk ZK bergantung pada ketersediaan bahan baku. Secara umum ada 7 proses produksi pembuatan pupuk ZK, yaitu:

1. Dekomposisi KCl dengan Na2SO4
2. Dekomposisi KCl dengan CaSO4
3. Dekompisisi KCl dengan MgSO4
4. Dekomposisi KCl dengan (NH4)2SO4
5. Proses Hargreaves yaitu mereaksikan gas SO2, O2, dan H2O dengan KCl
6. Proses Mannheim yaitu mencampur langsung KCl dengan H2SO4 dengan rasio mol tertentu
7. Pemurnian sumber sulfat alami seperti langbeinite dan kainit

1. Proses Produksi ZK dengan Dekomposisi KCl dengan Na2SO4

Dewasa ini, sumber yang umum digunakan berasal dari Sodium Sulphate Na2SO4 yang dapat diperoleh dari hasil samping dari beberapa proses produksi yakni:

1. Pengolahan bijih chromium
2. Pemurnian flue gas
3. Pembuatan serat (viscose fibres)
4. Produksi HCl, pigmen silica, asam lemak, dan trimethylolpropane
5. Pengolahan limbah asam sulfat

Diagram alir proses ditampilkan pada Gambar 1.
Gambar 1. Diagram alir proses produksi ZK dengan melalui dekomposisi KCl dengan Na2SO4

Gambar 1. Diagram alir proses produksi ZK dengan melalui dekomposisi KCl dengan Na2SO4

Penjelasan proses:
Bahan baku yang digunakan adalah sodium sulphate baik dalam bentuk anhydrous (Na2SO4) maupun dalam bentuk hydrated (Na2SO4.10H2O). Selain itu digunakan juga potassium chloride (KCl) dalam bentuk larutan pada temperatur 20 – 25ºC. Umpan KCl, Na2SO4, dan recycle mother liquor yang mengandung kristalin glaserite K3Na(SO4)2 dan KCl, serta kondensat hasil kondensasi dari uap evaporator diumpankan ke reaktor. Reaksi yang terjadi adalah sebagai berikut:

4Na2SO4 + 6KCl -> 2K3Na(SO4)2 + 6NaCl
2KCl + 2K3Na(SO4)2 -> 4K2SO4 + 2NaCl

Rasio mol Na2SO4 : KCl dibuat sangat berlebih yakni antara 1 : 6 sampai 1 : 10 untuk mendapatkan konversi yang tinggi (96 – 99%), sedangkan untuk rasio mol ZK : Na2SO4 dijaga 2 : 1. Beberapa variasi rasio mol (mr) bahan baku dan produk terhadap konversi yang diperoleh di dalam reaktor ditampilkan pada Gambar 2.

Gambar 2. Pengaruh rasio mol reagent terhadap derajat konversi Na2SO4 menjadi K2SO4

Gambar 2. Pengaruh rasio mol reagent terhadap derajat konversi Na2SO4 menjadi K2SO4

Setelah bereaksi di reaktor, produk ZK dipisahkan di filter dan selanjutnya mother liquor yang terbentuk diuapkan di unit konsentrasi 2 tingkat secara bertahap dan diikuti dengan proses kristalisasi pada temperatur rendah (? 2ºC) untuk tahap 1. Setiap mother liquor yang sudah terpisah baik di tahap 1 maupun 2 akan dipisahkan di filter untuk selanjutnya di-recycle kembali ke reaktor, sedangkan uap dari unit konsentrasi akan dikondensasikan terlebih dahulu dan selanjutnya dikirim ke reaktor.

Selain produk ZK juga diperoleh by-product berupa NaCl. Adapun spesifikasi produk ZK adalah sebagai berikut:
K2SO4: 96%-w
Cl- : 0,5%-w
Na+ : 0,2%-w

2. Proses Produksi ZK dengan bahan baku KCl dan CaSO4

Ada 3 tahapan utama dalam metode proses ini, yaitu:

1. Pelarutan gypsum
2. Konversi satu tahap (T = 25ºC)
3. Siklus amoniak dalam proses

Diagram alir proses dapat dilihat pada gambar 3.
Gambar 3. Diagram alir proses produksi ZK dengan melalui dekomposisi KCl dengan CaSO4

Gambar 3. Diagram alir proses produksi ZK dengan melalui dekomposisi KCl dengan CaSO4

Reaksi yang terjadi dalam proses ini antara lain:

CaSO4.2H2O + (NH4)2CO3 -> (NH4)2SO4 + CaCO3
2KCl + (NH4)2CO3 -> K2SO4 + 2NH4Cl

Adapun reaksi samping:

CaCO3 -> CaO + CO2
2NH4Cl + CaO + H2O -> CaCl2 + 2NH4OH
2NH4OH + CO2 -> (NH4)2CO3

Karakter dasar dari proses ini ialah adanya sistem recovery multistage untuk gas amoniak dan KCl, juga produk ZK yang dihasilka akan selalu mengandung amonium sulfat yang sangat dipengaruhi oleh komposisi mother liquor.

Akhir Bagian 1

Sumber:
Fertilizer Manual, 1967
Chemical Paper, B. U. Grzmil and B. Kic, 2005
http://www.k-utec.com/download/Te04-01.pdf, 2004

12 January 2010

Chemistry Laboratory Glassware Gallery Glassware Photos, Names & Descriptions

Glassware used in a chemistry laboratory is special. It needs to resist chemical attack. Some glassware has to withstand sterilization. Other glassware is used to measure specific volumes, so it can't change its size appreciably over room temperatures. Chemicals may be heated and cooled so the glass needs to resist shattering from thermal shock. For these reasons, most glassware is made from a borosilicate glass, such as Pyrex or Kimax. Some glassware isn't glass at all, but inert plastic such as Teflon.

See More >>

28 December 2009

Liquids and their interfaces Viscosity, surface tension, wetting, bubbles

Source :

http://www.chem1.com/acad/webtext/states/liquids.html

The molecular units of a liquid, like those of solids, are in direct contact, but never for any length of time and in the same locations. Whereas the molecules or ions of a solid maintain the same average positions, those of liquids are continually jumping and sliding to new ones, giving liquids something of the mobility of gases. From the standpoint of chemistry, this represents the best of two worlds; rapid chemical change requires intimate contact between the agents undergoing reaction, but these agents, along with the reaction products, must be free to move away to allow new contacts and further reaction to take place. This is why so much of what we do with chemistry takes place in the liquid phase.

1 What is a liquid?

Liquids occupy a rather peculiar place in the trinity of solid, liquid and gas. A liquid is the preferred state of a substance at temperatures intermediate between the realms of the solid and the gas. But if you look at the melting and boiling points of a variety of substances , you will notice that the temperature range within which many liquids can exist tends to be rather small. In this, and in a number of other ways, the liquid state appears to be somewhat tenuous and insecure, as if it had no clear right to exist at all, and only does so as an oversight of Nature.

liquid temperature ranges

Certainly the liquid state is the most complicated of the three states of matter to analyze and to understand. But just as people whose personalities are more complicated and enigmatic are often the most interesting ones to know, it is these same features that make the liquid state of matter the most fascinating to study.


How do we know it’s a liquid?

Anyone can usually tell if a substance is a liquid simply by looking at it. What special physical properties do liquids possess that make them so easy to recognize? One obvious property is their mobility, which refers to their ability to move around, to change their shape to conform to that of a container, to flow in response to a pressure gradient, and to be displaced by other objects. But these properties are shared by gases, the other member of the two fluid states of matter. The real giveaway is that a liquid occupies a fixed volume, with the consequence that a liquid possesses a definite surface. Gases, of course, do not; the volume and shape of a gas are simply those of the container in which it is confined. The higher density of a liquid also plays a role here; it is only because of the large density difference between a liquid and the space above it that we can see the surface at all. (What we are really seeing are the effects of reflection and refraction that occur when light passes across the boundary between two phases differing in density, or more precisely, in their refractive indexes.)

Flow properties of liquids: the viscosity

viscometerThe term viscosity is a measure of resistance to flow. It can be measured by observing the time required for a given volume of liquid to flow through the narrow part of a viscometer tube.

The viscosity of a substance is related to the strength of the forces acting between its molecular units. In the case of water, these forces are primarily due to hydrogen bonding. Liquids such as syrups and honey are much more viscous because the sugars they contain are studded with hydroxyl groups (–OH) which can form multiple hydrogen bonds with water and with each other, producing a sticky disordered network.

substance
viscosity
water H(OH) 1.00
diethyl ether (CH3-CH2)2O 0.23
benzene C6H6 0.65
glycerin C3H2(OH)3 280
mercury 1.5
motor oil, SAE30 200
honey ~10,000
molasses ~5000
pancake syrup ~3000

Specific viscosity (i.e., relative to water) of some liquids at 20°C.

Even in the absence of hydrogen bonding, dispersion forces are universally present (as in mercury). Because these forces are additive, they can be very significant in long carbon-chain molecules such as those found in oils used in cooking and for lubrication. Most "straight-chain" molecules are really bent into complex shapes, and dispersion forces tend to preserve their spaghetti-like entanglements with their neighbors.

Temperature dependence of viscosity

The temperature dependence of the viscosity of liquids is well known to anyone who has tried to pour cold syrup on a pancake. Because the forces that give rise to viscosity are weak, they are easily overcome by thermal motions, so it is no surprise that viscosity decreases as the temperature rises.

Viscosity of Water as a Function of Temperature
T/°C 0 10 20 40 60 80 100
viscosity/cP 1.8 1.3 1.0 0.65 0.47 0.36 0.28
Automotive lubricating oils can be too viscous at low temperatures (making it harder for your car to operate on a cold day), while losing so much viscosity at engine operating temperatures that their lubricating properties become impaired. These engine oils are sold in a wide range of viscosities; the higher-viscosity oils are used in warmer weather and the lower-viscosity oils in colder weather. The idea is to achieve a fairly constant viscosity that is ideal for the particular application. By blending in certain ingredients, lubricant manufacturers are able to formulate “multigrade” oils whose viscosities are less sensitive to temperatures, thus making a single product useful over a much wider temperature range.

For more on viscosity, see this Physics Hypertextbok page.

How viscosity impedes flow

The next time you pour a viscous liquid over a surface, notice how different parts of the liquid move at different rates and sometimes in different directions. In order to flow freely, the particles making up a fluid must be able to move independently. Intermolecular attractive forces work against this, making it difficult for one molecule to pull away from its neighbors and force its way in between new neighbors.


The pressure drop that is observed when a liquid flows through a pipe is a direct consequence of viscosity. Those molecules that happen to find themselves near the inner walls of a tube tend to spend much of their time attached to the walls by intermolecular forces, and thus move forward very slowly. viscosityMovement of the next layer of molecules is impeded as they slip and slide over the slow-movers; this process continues across successive layers of molecules as we move toward the center of the tube, where the velocity is greatest. This effect is called viscous drag, and is directly responsible for the pressure drop that can be quite noticeable when you are taking a shower bath and someone else in the house suddenly turns on the water in the kitchen.

Liquids and gases are both fluids and exhibit resistance to flow through a confined space. But it's interesting (and not often appreciated) that their viscosities have entirely different origins, and that they vary with temperature in opposite ways. Why should the viscosity of a gas increase with temperature? Find out here.

Surface tension

A molecule within the bulk of a liquid experiences attractions to neighboring molecules in all directions, but since these average out to zero, there is no net force on the molecule because it is, on the average, as energetically comfortable in one location within the liquid as in another.

surface tension

Liquids ordinarily do have surfaces, however, and a molecule that finds itself in such a location is attracted to its neighbors below and to either side, but there is no attraction operating in the 180° solid angle above the surface. As a consequence, a molecule at the surface will tend to be drawn into the bulk of the liquid. Conversely, work must be done in order to move a molecule within a liquid to its surface.

Why liquids form drops

Clearly there must always be some molecules at the surface, but the smaller the surface area, the lower the potential energy. Thus intermolecular attractive forces act to minimize the surface area of a liquid.

The geometric shape that has the smallest ratio of surface area to volume is the sphere, so very small quantities of liquids tend to form spherical drops. As the drops get bigger, their weight deforms them into the typical tear shape.

... and bubbles

Think of a bubble as a hollow drop. Surface tension acts to minimize the surface, and thus the radius of the spherical shell of liquid, but this is opposed by the pressure of vapor trapped within the bubble. For a more detailed analysis, see here. We discuss bubbles in much more detail farther down on this page.

The surface film

raft spiderpaperclip on waterThe imbalance of forces near the upper surface of a liquid has the effect of an elastic film stretched across the surface. You have probably seen water striders and other insects take advantage of this when they walk across a pond. Similarly, you can carefully "float" a light object such as a steel paperclip on the surface of water in a cup. (How to do it)

Left: Raft spider by thomsonalasdair; Right: photo by Jeffffd

Surface tensions of common liquids

Surface tension is defined as the amount of work that must be done in order to create unit area of surface. The SI units are J m–2 (or N m–1) but values are more commonly expressed in mN m–1 or in cgs units of dyn cm–1 or erg cm–2.
substance
surface tension
water H(OH) 72.7 dyne/cm
diethyl ether (CH3-CH2)2O 17.0
benzene C6H6 40.0
glycerin C3H2(OH)3 63
mercury (15°C) 487
n-octane 21.8
sodium chloride solution (6M in water) 82.5

sucrose solution
(85% in water)

76.4
sodium oleate (soap) solution in water 25

The table shows the surface tensions of several liquids at room temperature. Note especially that

  • hydrocarbons and non-polar liquids such as ether have rather low values
  • one of the main functions of soaps and other surfactants is to reduce the surface tension of water
  • mercury has the highest surface tension of any liquid at room temperature. It is so high that mercury does not flow in the ordinary way, but breaks into small droplets that roll independently.

Surface tension and viscosity are not directly related, as you can verify by noting the disparate values of these two quantities for mercury. Viscosity depends on intermolecular forces within the liquid, whereas surface tension arises from the difference in the magnitudes of these forces within the liquid and at the surface.

Surface tension and temperature

Surface tension is also affected by the electrostatic charge of a body. This is most dramatically illustrated by the famous "mercury beating heart" demo; click here to pop up a video with audio narration.
Surface tension of water
°C dynes/cm
0 75.9
20 72.7
50 67.9
100 58.9

Surface tension always decreases with temperature as thermal motions reduce the effect of intermolecular attractions. This is one reason why washing with warm water is more effective; the lower surface tension allows water to more readily penetrate a fabric.

2 Interfacial effects in liquids

The surface tension discussed immediately above is an attribute of a liquid in contact with a gas (ordinarily the air or vapor) or a vacuum. But if you think about it, the molecules in the part of a liquid that is in contact with any other phase (liquid or solid) will experience a different balance of forces than the molecules within the bulk of the liquid. Thus surface tension is a special case of the more general interfacial tension which is defined by the work associated with moving a molecule from within the bulk liquid to the interface with any other phase.

Wetting

Take a plastic mixing bowl from your kitchen, and splash some water around in it. You will probably observe that the water does not cover the inside surface uniformly, but remains dispersed into drops.

The same effect is seen on a dirty windshield; running the wipers simply breaks hundreds of drops into thousands. By contrast, water poured over a clean glass surface will wet it, leaving a uniform film.

← This photo of water drops on a leaf shows how the waxy coating naturally present on most leaves prevents its wetting. [omnia]

When a molecule of a liquid is in contact with another phase, its behavior depends on the relative attractive strengths of its neighbors on the two sides of the phase boundary. If the molecule is more strongly attracted to its own kind, then interfacial tension will act to minimize the area of contact by increasing the curvature of the surface. This is what happens at the interface between water and a hydrophobic surface such as a plastic mixing bowl or a windshield coated with oily material.

A liquid will wet a surface if the angle at which it makes contact with the surface is less than 90°. The value of this contact angle can be predicted from the properties of the liquid and solid separately.

wetting of a surface

A clean glass surface, by contrast, has –OH groups sticking out of it which readily attach to water molecules through hydrogen bonding; the lowest potential energy now occurs when the contact area between the glass and water is maximized. This causes the water to spread out evenly over the surface, or to wet it.

Surfactants

surfactant moleculeThe surface tension of water can be reduced to about one-third of its normal value by adding some soap or synthetic detergent. These substances, known collectively as surfactants, are generally hydrocarbon molecules having an ionic group on one end. The ionic group, being highly polar, is strongly attracted to water molecules; we say it is hydrophilic. The hydrocarbon (hydrophobic) portion is just the opposite; inserting it into water would break up the local hydrogen-bonding forces and is therefore energetically unfavorable. What happens, then, is that the surfactant molecules migrate to the surface with their hydrophobic ends sticking out, effectively creating a new surface. Because hydrocarbons interact only through very weak dispersion forces, this new surface has a greatly reduced surface tension.

surfactant

Washing

detergent actionHow do soaps and detergents help get things clean? There are two main mechanisms. First, by reducing water's suface tension, the water can more readily penetrate fabrics (see the illustration under "Water repellency" below.) Secondly, much of what we call "dirt" consists of non-water soluble oils and greasy materials which the hydrophobic ends of surfactant molecules can penetrate. When they do so in sufficient numbers and with their polar ends sticking out, the resulting aggregate can hydrogen-bond to water and becomes "solubilized".

Washing is usually more effective in warm water; higher temperatures reduce the surface tension of the water and make it easier for the surfactant molecules to penetrate the material to be removed.

magnetic laundry diskCan magnets reduce the surface tension of water? The answer is no, but claims that they can are widely circulated in promotions of dubious products such as "magnetic laundry disks" which are supposed to reduce the need for detergents. (See here for more on these scams.)

Water repellency

In Gore-Tex, one of the more successful water-proof fabrics, the fibers are made non-wettable by coating them with a Teflon-like fluoropolymer.

watter repellency

Water is quite strongly attracted to many natural fibers such as cotton and linen through hydrogen-bonding to their cellulosic hydroxyl groups. A droplet that falls on such a material will flatten out and be drawn through the fabric. One way to prevent this is to coat the fibers with a polymeric material that is not readily wetted. The water tends to curve away from the fibers so as to minimize the area of contact, so the droplets are supported on the gridwork of the fabric but tend not to fall through.

Capillary rise

If the walls of a narrow tube can be efficiently wetted by a liquid, then the the liquid will be drawn up into the tube by capillary action. This effect is only noticeable in narrow containers (such as burettes) and especially in small-diameter capillary tubes. The smaller the diameter of the tube, the higher will be the capillary rise.

A clean glass surface is highly attractive to most molecules, so most liquids display a concave meniscus in a glass tube.

capillary rise

To help you understand capillary rise, the above diagram shows a glass tube of small cross-section inserted into an open container of water. The attraction of the water to the inner wall of the tube pulls the edges of the water up, creating a curved meniscus whose surface area is smaller than the cross-section area of the tube. The surface tension of the water acts against this enlargement of its surface by attempting to reduce the curvature, stretching the surface into a flatter shape by pulling the liquid farther up into the tube. This process continues until the weight of the liquid column becomes equal to the surface tension force, and the system reaches mechanical equilibrium.

Capillary rise results from a combination of two effects: the tendency of the liquid to wet (bind to) the surface of the tube (measured by the value of the contact angle), and the action of the liquid's surface tension to minimize its surface area.

capillary rise, meniscus

In the formula shown at the left (which you need not memorize!)

h = elevation of the liquid (m)
γ = surface tension (N/m)
θ = contact angle (radians)
ρ = density of liquid (kg/m3)
g = acceleration of gravity (m/s–2)
r = radius of tube (m)

For the derivation of this relation, see this Wikipedia article.

The contact angle between water and ordinary soda-lime glass is essentially zero; since the cosine of 0 radians is unity, its capillary rise is especially noticable. In general, water can be drawn very effectively into narrow openings such as the channels between fibers in a fabric and into porous materials such as soils.

mercury meniscusNote that if θ is greater than 90° (π/2 radians), the capillary "rise" will be negative — meaning that the molecules of the liquid are more strongly attracted to each other than to the surface. This is readily seen with mercury in a glass container, in which the meniscus is upwardly convex instead of concave.

The Meniscus Madness page is a good source
of photos and activities aimed at middle school.

Devices employing capillary action to create perpetual motion machines have been proposed. The Museum of Unworkable Devices illustrates two of them, and explains why they won't work.

Capillary action and trees

Capillary rise is the principal mechanism by which water is able to reach the highest parts of trees. Water strongly bonds to the narrow (25 μM) cellulose channels in the xylem. (Osmotic pressure and "suction" produced by loss of water vapor through the leaves also contribute to this effect, and are the main drivers of water flow in smaller plants.) For an interesting discussion of these effects, see this site.

Bubbles

Bubbles can be thought of as "negative drops" — spherical spaces within a liquid containing a gas, often just the vapor of the liquid. Bubbles within pure liquids such as water (which we see when water boils) are inherently unstable because the liquid's surface tension causes them to collapse. But in the presence of a surfactant, bubbles can be stabilized and given an independent if evanescent existence.

bubble pressureThe pressure of the gas inside a bubble Pin must be sufficient to oppose the pressure outside of it (Pout, the atmospheric pressure plus the hydrostatic pressure of any other fluid in which the bubble is immersed. But the force caused by surface tension γ of the liquid boundary also tends to collapse the bubble, so Pin must be greater than Pout by the amount of this force, which is given by 4γ/r:

LaPlace law

See here for a derivation of the LaPlace equation. This page explains more about LaPlace's law and relates it to the behavior of balloons.

The most important feature of this relationship (known as LaPlace's law) is the that the pressure required to maintain the bubble is inversely proportional to its radius. This means that the smallest bubbles have the greatest internal gas pressures! This might seem counterintuitive, but if you are an experienced soap-bubble blower, or have blown up a rubber balloon (in which the elastic of the rubber has an effect similar to the surface tension in a liquid), you will have noticed that you need to puff harder to begin the expansion.

Soap bubbles

shefali Nayan "Soap Bubbles"

All of us at one time or another have enjoyed the fascination of creating soap bubbles and admiring their intense and varied colors as they drift around in the air, seemingly aloof from the constraints that govern the behavior of ordinary objects — but only for a while! Their life eventually comes to an abrupt end as they fall to the ground or pop in mid-flight. (But in this fascinating commentary on the subject, the author cites the case of one that lasted just one day short of a year!)

image: Soap Bubbles (2007) by Shefali Nyan

soap bubble structureThe walls of these bubbles consist of a thin layer of water molecules sandwiched between two layers of surfactant molecules. Their spherical shape is of course the result of water's surface tension. Although the surfactant (soap) initially reduces the surface tension, expansion of the bubble spreads the water into a thiner layer and spreads the surfactant molecules over a wider area, deceasing their concentration. This, in turn, allows the water molecules to interact more strongly, increasing its surface tension and stabilizing the bubble as it expands.

The bright colors we see in bubbles arises from interference between light waves that are reflected back from the inner and outer surfaces, indicating that the thickness of the water layer is comparable the range of visible light (around 400-600 nm).

Once the bubble is released, it can endure until it strikes a solid surface or collapses owing to loss of the water layer by evaporation. The latter process can be slowed by adding a bit of glycerine to the liquid. A variety of recipes and commercial "bubble-making solutions" are available; some of the latter employ special liquid polymers which slow evaporation and greatly extend the bubble lifetimes. Bubbles blown at very low temperatures can be frozen, but these eventually collapse as the gas diffuses out.

alveoli

Click here to pop up a more detailed view of the alveoli and the lung.

Bubbles, surface tension, and breathing

The sites of gas exchange with the blood in mammalian lungs are tiny sacs known as alveoli. In humans there are about 150 million of these, having a total surface area about the size of a tennis court. The inner surface of each alveolus is about 0.25 mm in diameter and is coated with a film of water, whose high surface tension not only resists inflation, but would ordinarily cause the thin-walled alveoli to collapse. In order to counteract this effect, special cells in the alveolar wall secrete a phospholipid pulmonary surfactant that reduces the surface tension of the water film to about 35% of its normal value. But there is another problem: the alveoli can be regarded physically as a huge collection of interconnected bubbles of varying sizes. As noted above, the surface tension of a surfactant-stabilized bubble increases with their size. So by making it easier for the smaller alveoli to expand while inhibiting the expansion of the larger ones, the surfactant helps to equalize the volume changes of all the alveoli as one inhales and exhales.

Pulmonary surfactant is produced only in the later stages of fetal development, so premature infants often don't have enough and are subject to respiratory distress syndrome which can be fatal.

3 Structure of liquids

You can think of a simple liquid such as argon or methane as a collection of loosely-packed marbles that can assume various shapes.liquid structure Although the overall arrangement of the individual molecular units is entirely random, there is a certain amount of short-range order: the presence of one molecule at a given spot means that the neighboring molecules must be at least as far away as the sum of the two radii, and this in turn affects the possible locations of more distant concentric shells of molecules.

An important consequence of the disordered arrangement of molecules in a liquid is the presence of void spaces. These, together with the increased kinetic energy of colliding molecules which helps push them apart, are responsible for the approximately 15-percent decrease in density that is observed when solids based on simple spherical molecules such as Ne and Hg melt into liquids. These void spaces are believed to be the key to the flow properties of liquids; the more “holes” there are in the liquid, the more easily the molecules can slip and slide over one another.

As the temperature rises, thermal motions of the molecules increase and the local structure begins to deteriorate, as shown in the plots below.

liquid structure

There is very little experimental information on the structure of liquids, other than the X-ray diffraction studies that yield plots such as this one for liquid mercury.

This plot shows the relative probability of finding a mercury atom at a given distance from another atom located at distance 0. You can see that as thermal motions increase, the probabilities even out at greater distances.

It is very difficult to design experiments that yield the kind of information required to define the microscopic arrangement of molecules in the liquid state.

Many of our current ideas on the subject come from computer simulations based on hypothetical models. In a typical experiment, the paths of about 1000 molecules in a volume of space are calculated. The molecules are initially given random kinetic energies whose distribution is consistent with the Boltzmann distribution for a given temperature. The trajectories of all the molecules are followed as they change with time due to collisions and other interactions; these interactions must be calculated according to an assumed potential energy-vs.-distance function that is part of the particular model being investigated.

These computer experiments suggest that whatever structure simple liquids do possess is determined mainly by the repulsive forces between the molecules; the attractive forces act in a rather nondirectional, general way to hold the liquid together. It is also found that if spherical molecules are packed together as closely as geometry allows (in which each molecule would be in contact with twelve nearest neighbors), the collection will have a long-range order characteristic of a solid until the density is decreased by about ten percent, at which point the molecules can slide around and move past one another, thus preserving only short-range order. In recent years, experimental studies based on ultra-short laser flashes have revealed that local structures in liquids have extremely short lifetimes, of the order of picoseconds to nanoseconds.

liquid-solid interfaceIt has long been suspected that the region of a liquid that bounds a solid surface is more ordered than within the bulk liquid. This has been confirmed for the case of water in contact with silicon, in which the liquid's layers form layers, similar to what is found in liquid crystals. (The illustration is from a 1999 article in Physical Review Focus.)

Some useful references

BubbleTown - all abut how to blow large and long-lasting soap bubbles.

The SoapBubbler site has a wonderful commentary on bubbles, their applications, and history.

This MIT site features some interesting photos and videos on bubbles.

Soap bubbles, their colours and the forces which mold them. This classic popular book by Charles V. Boys, first published in 1890, was reprinted in 1958 and is still inexpensively available. It can also be viewed on Google Books.

Bubble Physics - This 2003 article in Physics Today contains some math, but also descriptions of many practical applications that are not commonly known.

What you should be able to do

Make sure you thoroughly understand the following essential ideas which have been presented above. It is especially imortant that you know the precise meanings of all the green-highlighted terms in the context of this topic.

  • Liquids are both fluids and condensed phases. Explain what this tells us about liquids, and what other states of matter fit into each of these categories.
  • Define viscosity, and comment on the molecular properties that correlate with viscosity.
  • Define surface tension and explain its cause.
  • State the major factors that determine the extent to which a liquid will wet a solid surface.
  • Explain what a surfactant is, and how it reduces the surface tension of water and aids in cleaning.
  • Explain the origins of capillary rise and indicate the major factors that affect it.
  • Describe the structure of a soap bubble, and comment on the role of the "soap" molecules in stabilizing it.
  • Comment on the applicability of the term "structure" when describing a pure liquid phase.

Concept map

liquids concept map