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Small angle neutron scattering SANS

Neutrons are produced at either reactor or spallation sources, and spectrometers for neutron-scattering experiments are therefore uniquely available at large-scale facilities. After production, the neutron beam is subjected to a process of moderation during which the neutron energy decreases through collisions with the moderator to [Pg.268]

FIGURE 10.9 Schematic diagram of a SAXS-WAXS experiment performed on a semicrystalline polymer SAXS provides a measure of lamellar spacing, whereas the crystal structure is derived from the WAXS measurements. [Pg.268]

Neutrons interact with the nuclei. Two quantities characterize the nucleus-muclear interaction the neutron-scattering laigth, b, and the scattering cross-section, a. The former, usually of the order cm for all nucld, defines the amphtude of the scattered wave with respect to that of the inddmt wave. The scattering cross-section represents the probability of a neutron being scattered somewhere in space, and it equals 4nb. o has dimraisions of area, and it is usually reported in units of a bam (1 bam = KF cm ). [Pg.269]

Coherent Scattering Lengths, b, for Selected Nuclei Commonly Encountered in Polymers [Pg.269]

Conventional SANS spectrometers make it possible to probe structures over a length scale from near to atomic (10 A) dimensions to a few microns. The ultrasmall-angle neutron-scattering (USANS) instruments that have recently become available have extended the experimental Q range down to 2 x 10- A, reaching distances up to about 30 pm. [Pg.270]

A mono-energetic, collimated beam of neutrons (wavelength. A, typically 0.5-1.5nm), is directed at the specimen, and the angular scattering is recorded using a position-sensitive neutron detector. A schematic of the 35m long SANS instrument. Dll, installed on the ILL high flux reactor at [Pg.223]

Evacuated detector tube (sample-detector distance 1.1 m-36m) [Pg.224]

The polychromatic beam from the cold source is monochronaated by a helical slot velocity selector which selects neutrons of +1- 10% about a mean wavelength determined by the rotation speed of the drum. Typically, a mean wavelength of -0.525 nm is used. The neutrons are then collimated by a series of movable guides. Guide sections are inserted into, or removed from, the beam depending on the incident beam divergence required. A position-sensitive neutron detector is located inside an evacuated tube and can be moved to any distance between 1.1 and 35 m from the sample. [Pg.224]

From the perspective of radiation damage studies, it is important to characterise the effect of irradiation rather than provide a comprehensive description of all microstructural features. Consequently, for each irradiated material examined it is useful to characterise an unirradiated sample of the same material so that the difference in scattering response can be used to assess directly the effect of irradiation. Typically, samples are 10 x 10 x 2mm These are simple to fabricate from Charpy specimens (10 x 10 x 55 mm ) and are sufficiently thick to enable a statistically significant number of neutrons to scatter and be detected. Use of thinner samples will result in a smaller fraction of the incident neutrons scattering but, with modem high flux neutron sources, SANS analysis of these thinner samples is perfectly possible. [Pg.224]

The range of Q (the magnitude of the scattering vector Q as defined in Fig. 9.8) covered in a particular experimental setup determines the range of dimensions of inhomogeneities to which the experiment is sensitive. [Pg.224]

We can imagine that each atom has a shield of area 4Trb to block the incident neutrons and scatter them in all directions. This area is called a scattering cross section. The cross section of the entire sample is denoted by S. The coherent part of the scattering intensity per unit solid angle dfl at q is related to the position r, and the scattering length of the /th nucleus by [Pg.137]

Now we apply the general formula to a solution of polymer. We consider that the polymer consists of hydrogenated chains (regular chains) and deuterated chains, both having the same distribution in the chain length. The coherent scattering by the solution of total concentration c is given as [Pg.137]

Extraction of 5 i(q) from 7(q) is facilitated by contrast matching in which Up and Us are brought to be equal by choosing an appropriate isotopic mixture of the solvents for a given isotopic mixture of the polymer samples. Because of the factor XhXd, the scattering intensity maximizes for a 50 50 mixture of the isotopes. Once we obtain 5 i(q), the methods used in the analysis of SLS data can be applied, including the Zimm plot. [Pg.138]


The structure of microemulsions have been studied by a variety of experimental means. Scattering experiments yield the droplet size or persistence length (3-6 nm) for nonspherical phases. Small-angle neutron scattering (SANS) [123] and x-ray scattering [124] experiments are appropriate however, the isotopic substitution of D2O for H2O... [Pg.517]

SANS. See Small-angle neutron scattering (SANS)... [Pg.600]

Silylated diamines, 156, 187-188 Silylated monomers, 72 Silylation, distillation and, 338 6NT6 alternating polyesteramide, synthesizing, 189-190 6,6 -linked polymers, 480 Size exclusion chromatography (SEC) analyses, 90, 490 Slabstock foam, 233-234 Slow monomer addition, 57 Small-angle neutron scattering (SANS), 282... [Pg.601]

Small angle neutron scattering (SANS) involves firing neutrons at a sample and measuring the angle through which they are scattered. This allows the momentum transfer, Q, to be determined according to the equation ... [Pg.141]

The conformation of polymer chains in an ultra-thin film has been an attractive subject in the field of polymer physics. The chain conformation has been extensively discussed theoretically and experimentally [6-11] however, the experimental technique to study an ultra-thin film is limited because it is difficult to obtain a signal from a specimen due to the low sample volume. The conformation of polymer chains in an ultra-thin film has been examined by small angle neutron scattering (SANS), and contradictory results have been reported. With decreasing film thickness, the radius of gyration, Rg, parallel to the film plane increases when the thickness is less than the unperturbed chain dimension in the bulk state [12-14]. On the other hand, Jones et al. reported that a polystyrene chain in an ultra-thin film takes a Gaussian conformation with a similar in-plane Rg to that in the bulk state [15, 16]. [Pg.56]

Overview. Considerable research activities in the fields of isotropic SAXS and small-angle neutron scattering (SANS) are devoted to the investigation of ensembles of uncorrelated but identical or almost identical complex particles. Frequently these particles are studied in solution. Samples for such investigations must be supplied in a solution in which the particles do not aggregate. [Pg.176]

The size and shape of polymer chains joined in a crosslinked matrix can be measured in a small angle neutron scattering (SANS) experiment. This is a-chieved by labelling a small fraction of the prepolymer with deuterium to contrast strongly with the ordinary hydrogenous substance. The deformation of the polymer chains upon swelling or stretching of the network can also be determined and the results compared with predictions from the theory of rubber elasticity. [Pg.257]

Small angle neutron scattering (SANS) of "marked" (isotopically labeled) chains in unmarked networks has proven to be of potential value in... [Pg.279]

Time-resolved in situ Small Angle Neutron Scattering (SANS) investigations have provided direct experimental evidence for the initial steps in the formation of the SBA-15 mesoporous material, prepared using the non-ionic tri-block copolymer Pluronic 123 and TEOS as silica precursor. Upon time, three steps take place during the cooperative self-assembly of the Pluronic micelles and the silica species. First, the hydrolysis of TEOS is completed, without modifications of the Pluronic spherical micelles. Then, when silica species begin to interact with the micelles, a transformation from spherical to cylindrical micelles takes place before the precipitation of the ordered SBA-15 material. Lastly, the precipitation occurs and hybrid cylindrical micelles assemble into the two-dimensional hexagonal structure of SBA-15. [Pg.53]

Using small-angle neutron scattering (SANS), it was shown that alkoxy-substituted triphenylenes associate in deuterated hexadecane.70 At low concentrations small aggregates are formed and at higher concentrations (10 3 M)... [Pg.398]

Small-angle neutron scattering (SANS), 14 710, 19 568, 20 339 Small-angle X-ray scattering (saxs), 20 339, 341-342, 26 432 of amorphous silica, 22 474 Small beer, 26 471 Small Business Innovation Research (SBIR) program, 24 395, 399 Small Business Technology Transfer (STTR) program, 24 395 Small communities... [Pg.851]

Characterization of Dendritically Branched Polymers by Small Angle Neutron Scattering (SANS), Small Angle X-Ray Scattering (SAXS) and Transmission Electron Microscopy (TEM)... [Pg.255]

Values obtained from small angle neutron scattering (SANS) data for PAMAMs in the same solution as in a for PPIs in D20. [Pg.334]


See other pages where Small angle neutron scattering SANS is mentioned: [Pg.1371]    [Pg.28]    [Pg.411]    [Pg.252]    [Pg.145]    [Pg.771]    [Pg.377]    [Pg.282]    [Pg.63]    [Pg.130]    [Pg.301]    [Pg.53]    [Pg.105]    [Pg.49]    [Pg.194]    [Pg.126]    [Pg.131]    [Pg.375]    [Pg.187]    [Pg.258]    [Pg.269]    [Pg.91]    [Pg.258]    [Pg.337]    [Pg.614]    [Pg.33]    [Pg.50]   
See also in sourсe #XX -- [ Pg.141 ]

See also in sourсe #XX -- [ Pg.141 ]




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