Double probe

The test gas must be of uniform and known composition. This generally requires on-line gas analysis if flammable mixtures are not supplied from a suitable reservoir. If concentration gradients are created in the surrounding air, errors can be introduced by releasing the test gas stream from a perforated probe doubling as an electrode. The maximum effective energy of a... 

Sampling probe Double-sided, single-sided probes when used with reflectance Double-sided or special ATR probes Single-ended... 

Figure 1. Assembly drawing of the screened probe double-channel ceramic...

Spin through a Sephadex G50 column, as described in Sambrook et al. (1989). Collect the eluate (should be exactly 100 /a1) and add 2 jul 5 A/ NaCl to make a final concentration of 0.1 M NaCI. This salt concentration helps in keeping the probe double-stranded. Store at -20°C. 

P, C, and A1 MAS NMR spectra were obtained at 7 T using a Varian Unityplus 300 NMR spectrometer equipped with a Doty Scientific 7 mm high-speed VT-MAS probe. Double O-ring sealed rotors (Doty Scientific) were used. Both direct polarization (DP) and cross-polarization (CP) spectra were... 

Zhang, X., Zhong, Y.X., Yan, J.W. et al. (2012) Probing double layer structures of Au (111)-BMIPFg ionic hquid interfaces from potential-dependent AFM force curves. Chemical Communications, 48, 582—584. 

P-labeled DNA fragment (400 bp) from the right terminal of Hindlll to Rsal (3) in pAT9sd was used as probe. Double digest of pATP9202... 

Research by Massarsch has led to an improved energy transmission using resonance vibro-compaction. The key features of the resonant compaction technique are the use of a specially designed compaction probe (double Y with adapted impedance) and a heavy vibrator with variable operating frequency on top of the probe. After probe insertion, the frequeney of the vibrator is adjusted to the resonance frequency of the soil layer, thereby amplifying the ground response (Massarsch, 2002). 

The probes are assumed to be of contact type but are otherwise quite arbitrary. To model the probe the traction beneath it is prescribed and the resulting boundary value problem is first solved exactly by way of a double Fourier transform. To get managable expressions a far field approximation is then performed using the stationary phase method. As to not be too restrictive the probe is if necessary divided into elements which are each treated separately. Keeping the elements small enough the far field restriction becomes very week so that it is in fact enough if the separation between the probe and defect is one or two wavelengths. As each element can be controlled separately it is possible to have phased arrays and also point or line focussed probes. 

Besides, because this probe is suitable for testing various artificial defects such as FBH, SDH, columned holes and cracks and its testing range is larger than ordinary one-transmitting-and-the-other-receiving double crystal creeping wave probe, we can conclude that this probe has a wide use value and prospect. 

Callegari A, Rebstein J, Muenter J S, Jost R and Rizzo T R 1999 The spectroscopy and intramolecular vibrational energy redistribution dynamics of HOCI in the u(OH) = 6 region, probed by infrared-visible double resonance overtone excitation J. Chem. Phys. 111 123-33... 

The main cost of this enlianced time resolution compared to fluorescence upconversion, however, is the aforementioned problem of time ordering of the photons that arrive from the pump and probe pulses. Wlien the probe pulse either precedes or trails the arrival of the pump pulse by a time interval that is significantly longer than the pulse duration, the action of the probe and pump pulses on the populations resident in the various resonant states is nnambiguous. When the pump and probe pulses temporally overlap in tlie sample, however, all possible time orderings of field-molecule interactions contribute to the response and complicate the interpretation. Double-sided Feymuan diagrams, which provide a pictorial view of the density matrix s time evolution under the action of the laser pulses, can be used to detenuine the various contributions to the sample response [125]. 

Por IR-Raman experiments, a mid-IR pump pulse from an OPA and a visible Raman probe pulse are used. The Raman probe is generated either by frequency doubling a solid-state laser which pumps the OPA [16], or by a two-colour OPA [39]. Transient anti-Stokes emission is detected with a monocliromator and photomultiplier [39], or a spectrograph and optical multichannel analyser [40]. 

Fig. 1. Southern blot analysis of DNA showing (a) step 1, an agarose gel containing separated restriction fragments of DNA, denoted by (—), which is immersed in NaOH to denature the double-stranded stmcture of DNA, and then transferred by capillary flow to a nitrocellulose filter. In step 2, the bound DNA is allowed to hybridize to a labeled nucleic acid probe, and the unbound probe is washed off In step 3, the filter is placed into contact with x-ray film resulting in (b) bands of exposure on the film which are detected after development and correspond to regions where the restriction fragment is...

Surface SHG [4.307] produces frequency-doubled radiation from a single pulsed laser beam. Intensity, polarization dependence, and rotational anisotropy of the SHG provide information about the surface concentration and orientation of adsorbed molecules and on the symmetry of surface structures. SHG has been successfully used for analysis of adsorption kinetics and ordering effects at surfaces and interfaces, reconstruction of solid surfaces and other surface phase transitions, and potential-induced phenomena at electrode surfaces. For example, orientation measurements were used to probe the intermolecular structure at air-methanol, air-water, and alkane-water interfaces and within mono- and multilayer molecular films. Time-resolved investigations have revealed the orientational dynamics at liquid-liquid, liquid-solid, liquid-air, and air-solid interfaces [4.307]. 

Radioactivation Techniques Neutron and thin layer (TLA) activation are non-intrusive techniques ofi ering the prospect of continuous, direct component monitoring, in addition to coupon or probe, monitoring. In principle, localised corrosion can be monitored using a double-layer technique. Process plant applications of the technique have been limited to date. ... 

Figure 10-5. Transient transmission changes AV/Po in PPV for different lime delays between the pump and probe pulse. The pump pulse is a 100 fs laser pulse at 325 nm obtained by frequency doubling ol amplified dye laser pulses, (a) and (b) correspond to different sides of a PPV-film. The spectra in (a) were obtained lor the unoxidized side of the sample while the set of spectra in (b) was measured for the oxidized side of the same sample. The main differences observed are a much lower stimulated emission effect for the oxidized side. The two bottom spectra depict the PL-spectra for comparison. The dashed line indicates the optical absorption (according to Kef. (281).

In large boiler plants, carryover is measured by employing a singleport sampling nozzle connected to a steam supply line between the top drum and the superheater. Sampling from superheaters is difficult, however, because a pump is needed to inject cool condensate water into a double-walled sample probe (via an attemperating nozzle). This is to remove the degrees of superheat and thus reduce the tendency for any contaminants to deposit in or on the sample probe, rather than be collected with the steam. 

Chronoamperometry is often used for measuring the diffusion coefficient of electroactive species or the surface area of the working electrode. Analytical applications of chronoamperometry (e.g., in-vivo bioanalysis) rely on pulsing of the potential of the working electrode repetitively at fixed tune intervals. Chronoamperometry can also be applied to the study of mechanisms of electrode processes. Particularly attractive for this task are reversal double-step chronoamperometric experiments (where the second step is used to probe the fate of a species generated in the first step). 

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