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WATER.
It covers
70 percent of Earths surface, makes up 60 percent of the human
body, and forms 90 percent of the composition of blood. Life as
we know it wouldnt exist without water. Yet, each molecule
of this common, seemingly simple substanceone oxygen atom
bound to two hydrogen atomsholds a world of mystery within
its subnanometer-size structure.
Of particular interest to
physical and structural chemists is what happens at the interfaces
where water meets air or other substances such as proteins. The
density of the water molecules, for example, can change by many
orders of magnitude between the liquid below the surface and the
vapor above the surface. What happens in the transition zone? Much
has been theorized and calculated, but corroborating experiments
have been difficult to conductuntil now.
A team of researchers from
Lawrence Livermore and Lawrence Berkeley national laboratories and
the University of California at Berkeley has developed a technique
using soft x rays for studying in detail the surfaces of liquid
microjets. The groundbreaking work of the collaboration, which included
Livermore chemist James Tobin, UC Berkeley chemistry graduate student
Kevin Wilson, and UC Berkeley chemistry professor Richard Saykally,
was reported in both Physical Review Letters and a cover
article in the Journal of Physical Chemistry B.
The standard technique for
examining the chemical structure of a protein at the molecular and
atomic levels, for example, uses a frozen sample. Yet, the three-dimensional
structure of molecules in a frozen sample differs from that of molecules
in a sample at body temperature. Theres a strong drive
to find ways of studying the molecular structures of such substances
in their normal biological state, explains Tobin. The
experimental technique we developed is one possible method.
Ultimately, this technique may allow scientists to better determine
the structure of biological systems such as hemoglobin in blood
and to understand how proteins move through solution.
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The
water jet. |
X
Rays Measure Atomic Interfaces at Waters Surface
One of the primary tools
for probing the electronic structure of interfaces is x-ray absorption
spectroscopy. However, this x-ray technique has difficulty measuring
the structural interfaces at the atomic and molecular level for
liquids, particularly those containing hydrogen atoms. And
hydrogen is a key atomic component in many systems, says Wilson.
Many of the interesting properties of water are due to the
hydrogen bonds between neighboring molecules. (See the box
below entitled "Water Basics.")
One problem facing scientists
who want to examine hydrogens role in water or other liquids
is that the amount of spectroscopic data gathered from hydrogen
on the surface or interior of a water sample is extremely small.
This weak signal is usually overwhelmed by signals generated from
the water vapor that blankets the surface of liquid. Another problem
is that with x-ray spectroscopy systems, the sample must be in a
vacuum, which means the liquid must be contained or behind a barrier
such as a window. Windows, even thin-walled cells, will interact
with the surface of the liquid and absorb a majority of the x-ray
signal, leaving us nothing to measure by, Tobin explains.
The team overcame these problems,
using liquid microjet technology and Lawrence Berkeleys Advanced
Light Source (ALS). In the experiments, a 20-micrometer-diameter
jet of liquid pressurized to about 3.4 megapascals (500 pounds per
square inch) squirts through a very small nozzle. The smaller
the dimensions of a liquid sample, the less vapor there is,
explains Wilson. Two other team members, Lawrence Berkeley beamline
scientists Bruce Rude and Tony Catalano, devised a pumping system
that not only allowed the system to meet the vacuum requirements
of the ALS but also reduced the amount of residual vapor. As
far as I know, these experiments were the first time that experiments
on a liquid jet were conducted at the ALS, notes Wilson.
To probe the structure of
water molecules at the surface of the water jet, researchers use
intense x-ray beams of energies at the soft end of the
spectrum generated by the ALS. The x rays are directed at the jet
about 1 to 2 millimeters in front of the nozzle. At this distance,
the liquid is still at room temperature and has not yet begun to
expand and cool. Because it is impossible to examine anything smaller
than the wavelength of light being used, the light waves for studying
atoms and molecules must be extremely short. The ALS is ideal for
these sorts of measurements, because it can produce light at wavelengths
of a few tenths of a nanometerabout the sizes of atoms, molecules,
chemical bonds, and the distances between atomic planes in crystals.
Even more importantly, the ALS can supply x rays at 530 electronvolts
and abovethe amount required to kick an electron
from the innermost shell of an oxygen atom out of the water molecule.
(See the box below entitled "How the ALS Works.")
Water
Basics
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Water
is the most familiar and abundant liquid on Earth. Given
its low molecular weight, it should, by all rights, be
a gas at such temperatures. The fact that it is not has
much to do with its molecular structure. The atoms in
a water moleculetwo hydrogen and one oxygenare
arranged at the corners of an isosceles triangle. The
oxygen atom is located where the two equal sides meet,
and the angle between these sides is about 105 degrees.
The asymmetrical shape of the molecule arises from a tendency
of the four electron pairs in the outermost shell of oxygen
to arrange themselves symmetrically at the vertices of
a tetrahedron around the oxygen nucleus. Two electron
pairs from each oxygen form covalent bonds with the two
hydrogen atoms. (A covalent bond is created when two atoms
share a pair of electrons.) The hydrogen atoms are drawn
slightly together, resulting in the V-shaped water molecule.
This arrangement results in a polar molecule, with a net
negative charge toward the oxygen end and a net positive
charge at the hydrogen end. When water molecules are close
enough, each oxygen attracts the nearby hydrogen atoms
of two other water molecules, forming hydrogen bonds.
Although much weaker than the covalent bonds holding the
water molecule together, hydrogen bonds are strong enough
to keep water liquid at ordinary temperatures, despite
its low molecular weight. These hydrogen bonds are also
responsible for various other properties of water, such
as its high specific heat. |
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X-ray
absorption spectra at the oxygen K edge (530 electronvolts)
of water vapor showing the near-edge x-ray absorption-fine-structure
(NEXAFS) and extended x-ray absorption-fine-structure (EXAFS)
regions of the spectra. |
Electrons
at the Edge
Two x-ray spectroscopy
techniques were used to examine the structure of the water surface
in the microjet: extended x-ray absorption fine structure (EXAFS)
and near-edge x-ray absorption fine structure (NEXAFS). Both techniques
are based on the fact that atoms will absorb x rays, the amount
of absorption depending on the energy level of the x ray and the
type of atom doing the absorbing. Generally, the proportion of x
rays absorbed (called the absorption coefficient) decreases as x-ray
energies increase. However, at energy levels specific to each element,
a sudden increase in the absorption coefficient is observed. These
energies, called absorption edges, correspond to the energy required
to eject an electron from the atom. For an isolated atom, the sudden
peak at the absorption edge occurs as the electron is ejected and
then a gradual decrease in x rays absorbed occurs as the x-ray energy
levels are increased. However, for atoms in a molecule or in a liquid
or solid state, the closeness of other atoms around the absorbing
atom causes oscillations in the amount of x-ray absorption just
past the absorption edge. These wiggles detected in
the absorption edge, called EXAFS oscillations, arise from the ejected
electron backscattering off neighboring atoms. The structure of
the oscillationsthat is, their frequency and amplitudedepends
on the distance and number of neighboring atoms. The length of bonds
between neighboring atomssuch as oxygen atoms or hydrogen
atoms in water, for instancecan be determined by analyzing
these EXAFS oscillations.
Whereas
EXAFS is sensitive to distances between atoms and molecules, NEXAFS
is sensitive to bond angles and bond lengths between atoms and molecules.
NEXAFS is similar to EXAFS, but instead of providing enough energy
to eject an electron, a NEXAFS x ray has just enough energy to cause
an electron to jump up to an unoccupied higher energy level. The
steplike vertical rise in absorption intensity resides between the
absorption edge and the EXAFS region, hence the near-edge
designation. The energy at which this rise occurs differs according
to the individual element, chemical bond, or molecular orientation.
With NEXAFS, researchers tune the x-radiation to different frequencies
to help determine the orientation of a molecule on the surface of
a liquid and its intramolecular bond lengths.
How
the ALS Works
|
Water
is the most familiar and abundant liquid on Earth. Given
its low molecular weight, it should, by all rights, be
a gas at such temperatures. The fact that it is not has
much to do with its molecular structure. The atoms in
a water moleculetwo hydrogen and one oxygenare
arranged at the corners of an isosceles triangle. The
oxygen atom is located where the two equal sides meet,
and the angle between these sides is about 105 degrees.
The asymmetrical shape of the molecule arises from a tendency
of the four electron pairs in the outermost shell of oxygen
to arrange themselves symmetrically at the vertices of
a tetrahedron around the oxygen nucleus. Two electron
pairs from each oxygen form covalent bonds with the two
hydrogen atoms. (A covalent bond is created when two atoms
share a pair of electrons.) The hydrogen atoms are drawn
slightly together, resulting in the V-shaped water molecule.
This arrangement results in a polar molecule, with a net
negative charge toward the oxygen end and a net positive
charge at the hydrogen end. When water molecules are close
enough, each oxygen attracts the nearby hydrogen atoms
of two other water molecules, forming hydrogen bonds.
Although much weaker than the covalent bonds holding the
water molecule together, hydrogen bonds are strong enough
to keep water liquid at ordinary temperatures, despite
its low molecular weight. These hydrogen bonds are also
responsible for various other properties of water, such
as its high specific heat. |
Courtesy
of the Advanced Light Source, Lawrence Berkeley National
Laboratory.
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Near-edge
x-ray absorption-fine-structure (NEXAFS) spectra of water
vapor (top), liquid water surface (middle), and bulk, or interior,
water (bottom), showing the surface to have an intermediate
electronic structure between vapor and the bulk liquid.
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Measuring
the Ties That Bind
In their first experiment,
reported in Physical Review Letters,1 the team members made
the first definitive observation of EXAFS from hydrogen and quantified
the covalent oxygenhydrogen bond in water vapor as 0.095 ±
0.003 nanometer in length. Their research showed that hydrogen bonds
can be directly detected in liquid water, paving the way for future
studies of intermolecular hydrogen bondsstructures that are
critical to understanding the unique properties of liquid water.
In their second experiment,
reported in The Journal of Physical Chemistry B,2 the researchers
obtained NEXAFS spectra for the water surface that appear as intermediate
between the bulk- and the gas-phase spectra. The appearance of the
surface spectrum is consistent with an interface or surface in which
molecules are in transition from the bulk phase to the vapor phase
as in evaporation. The researchers measured distances of 0.3 ±
0.005 nanometer between neighboring oxygen atoms on the surface
of the microjet, and distances of 0.285 ± 0.005 nanometer
between neighboring oxygen atoms about 2.5 nanometers inside the
jet. The latter result is in line with previous studies of the bulk
liquid. The surface measurement supports results from computer simulations,
which predicted that on the surface, weaker hydrogen bonds would
exist, leading to water molecules that would be further apart and
more mobile compared to molecules below the surface.
What
these experiments showed was that this technique works and works
well, says Tobin. Since the results were published, the team
has moved forward, using this technique to examine molecular structures
of other solvents such as methanol, ethanol, and isopropyl alcohol.
One of the next steps will be to examine sodium chloride solutionin
other words, salt water. Its all just the beginning of obtaining
a better understanding of liquid surface chemistryone of the
big unknowns in modern science.
—Ann Parker
Key Words:
Advanced Light Source (ALS), extended x-ray absorption fine structure
(EXAFS), hydrogen bonds, liquid surface chemistry, microjet, molecular
structure, near-edge x-ray absorption fine structure (NEXAFS), water,
x-ray spectroscopy.
References:
1. Kevin Wilson, James G. Tobin, A. L. Ankudinov, J. J. Rehr, and
R. J. Saykally, Extended X-Ray Absorption Fine Structure from
Hydrogen Atoms in Water, Physical Review Letters 85(20),
42894292 (2000). http://www.llnl.gov/str/refs/tobin.r1.html
2. Kevin R. Wilson, Bruce S. Rude, Tony Catalano, Richard D. Schaller,
James G. Tobin, Dick T. Co, and R. J. Saykally, X-Ray Spectroscopy
of Liquid Water Microjets, The Journal of Physical Chemistry
B 105(17), 33463349 (2001). http://www.llnl.gov/str/refs/tobin.r2.html
For further
information contact James Tobin (925) 422-7247 (tobin1@llnl.gov).
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