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Wavelength observation

What wavelength will be observed at a detector that is placed at 23.5° when the light source strikes the reflection grating at an angle of 45.3° and the grating has 1250 lines per mm. Assume that the order of diffraction is first order. What is the second order wavelength observed ... [Pg.161]

Conversely, in the case of the n >7T transition of a ketone, the interaction of the lone pair of the ground state carbonyl with a polar solvent lowers the energy of the lone pair n orbital, and thereby increases the energy required to promote an electron to the ti energy level. Consequently, there is often a blue (hypsochromic) shift - to lower wavelength - observed when the UV spectrum of a ketone is recorded in ethanol rather than cyclohexane. [Pg.14]

The upper limit is the longest wavelength observed for the transition and is tentatively identified as the 0-0 band (42). [Pg.48]

The vision literature contains a great variety of different absorption profiles for the chromophores of vision. They have been acquired using a variety of means. The chemist prefers to measure the absorbance of individual chromophores in a standard one centimeter cell as a function of wavelength. The chromophore is usually present in a dilute solution. The psychophysiologist prefers an in-vivo test under conditions of differential adaptation. The results from these two methods have shown considerable disparity. This work will show that, for the in-vivo situation (and adequate differential adaptation in the psychophysical situation), the actual L-channel peak is in human vision is at 625 nm. This is the peak wavelength observed in all other biological species. [Pg.48]

SEDs) demonstrate that massive disks often extend to hundreds of astronomical units. A lower estimate for the initial mass distribution of our Solar System is provided by the minimum mass solar nebula (MMSN) model, which is the minimum mass required to produce the observed distribution of solids from a disk with solar composition. This analysis predicts a disk mass between 0.01 and 0.07 M extending out to 40 AU. Mass estimates for circumstellar disks derived from submillimeter and longer-wavelength observations are consistent with the range estimated for the MMSN (e.g. Beckwith et al. 1990 Williams etal. 2005). [Pg.10]

Mid- and far-infrared, submillimeter, and radio-wavelength observations allow probing the presence and abundance of simple molecules in these zones and provide constraints and boundary conditions for coupled disk evolution and chemical network models. The observed abundances and predictions from the disk models can be directly compared to constraints derived from the early Solar System. [Pg.11]

The effect of low pH on a-lactalbumin was studied further by Permyakov et al. (1981). In addition to the spectral shift toward shorter wavelengths (observed by Kronman et al., 1965), they found a decrease in Trp fluorescence quantum yield. They suggested that the replacement of Ca(II) by H(I) is basically responsible for these effects. [Pg.261]

Bohr developed an equation to calculate all of the possible energies of the electron in a hydrogen atom. His values agreed with those calculated from the wavelengths observed in hydrogen s line-emission spectrum. In fact, his values matched with the experimental values so well that his atomic model that is described earlier was quickly accepted. [Pg.111]

Repeat step 4 with the K2SO4 and with each of the remaining solutions in the well strip. For each solution that you test, record the color of each flame and the wavelength observed with the spectroscope. After the solutions are tested, clean the wire thoroughly, rinse the well strip with distilled water, and collect the rinse water in the waste beaker. [Pg.792]

This result relates the evolution of the universe (a0/ae) as the photon travels from emission to observation, to the change in its frequency (is) or wavelength (A). As the universe expands (or contracts ), wavelengths expand (contract) and frequencies decrease (increase). The redshift of a spectral line is defined by relating the wavelength at emission (the lab or rest-frame wavelength Ae) to the wavelength observed at a later time ta,... [Pg.3]

FTIR microscopy was discussed earlier in the chapter, and given the complementary nature of IR and Raman, it is reasonable that laboratories performing IR microscopy might well need Raman microscopy and vice versa. Two microscope systems were required and the sample had to be moved from one system to the other. The difficulty of relocating the exact spot to be sampled can be imagined. A combination dispersive Raman and FTIR microscopy system, the LabRAM-IR2 (HORIBA Scientific, Edison, NJ), allows both Raman and IR spectra to be collected at exactly the same location on the sample. The resolution depends on the wavelength observed, because resolution is limited by diffraction, but is <1 pm for the Raman spectrum and 10-20 pm for the IR spectrum. Examples of the type of data that can be obtained with this combination microscopy system are shown in Figures 4.76 and 4.77. [Pg.339]

Feldman and Batistoni discuss the connection for steady state and/or transient background radiation. They point out that the degree of selectivity exhibited by a spectral emission detector is intimately connected with the level and time variation of the spectral background at the wavelength observed. The situation can best be comprehended in terms of a few typical situations. [Pg.486]

Fig. 4.2 Temperature and density of H2 profiles in the envelope of the low mass proto-star IRAS 16293-2422 based on multi-wavelength observations from Grimier et ai. [19]... Fig. 4.2 Temperature and density of H2 profiles in the envelope of the low mass proto-star IRAS 16293-2422 based on multi-wavelength observations from Grimier et ai. [19]...
One possibility for improving the theory is to take into account higher order terms in the virial expansion. This has been done by Mulder for an aligned hard-rod fluid [66]. Mulder has taken into account the third- and fourth-order terms and has been able to obtain the numerical values of the transition density and the smectic period in very good agreement with the results of computer simulations [67]. The critical packing fraction and the dimensionless smectic wavelength observed are rjf ji =036 and 1.27 while the theoretical results are tlN-A 0-37 and A =1.34 [66]. Recently Poniwierski performed an asymptotic analysis of the nematic-smectic A transition in the system of... [Pg.98]


See other pages where Wavelength observation is mentioned: [Pg.146]    [Pg.153]    [Pg.281]    [Pg.69]    [Pg.256]    [Pg.13]    [Pg.223]    [Pg.703]    [Pg.599]    [Pg.95]    [Pg.98]    [Pg.263]    [Pg.547]    [Pg.703]    [Pg.383]    [Pg.265]    [Pg.146]    [Pg.134]    [Pg.703]    [Pg.305]    [Pg.11]    [Pg.89]    [Pg.312]    [Pg.421]    [Pg.3550]    [Pg.124]    [Pg.652]    [Pg.488]    [Pg.247]    [Pg.30]    [Pg.487]    [Pg.303]    [Pg.317]    [Pg.795]    [Pg.63]    [Pg.117]   
See also in sourсe #XX -- [ Pg.3 , Pg.16 ]




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