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Field stop

Let us consider the following protocol the dipole starts in the down state —p at H = —Hq. The field is then ramped from —Ho to +Ho at a constant speed r = H, so H t) = rt (Fig. 13a). The protocol lasts for a time tn x = 2//o/r and the field stops changing when it has reached the value Ho- The free energy difference between the initial and final states is 0 because the free energy is an even function of H. To ensure that the dipole initially points down and that this is an equilibrium state, we take the limit Hq oo but we keep the ramping speed r finite. In this way we generate paths that start at H = oo at t = —oo and end up at H = oo at t = oo. We can now envision all possible paths followed by the dipole. The up configuration is statistically preferred for H > 0,... [Pg.83]

Fig. 8.2.1. Low angle laser light scattering photometer (Chromatix KMX-6) simplified optical diagram. 1 Flelium-neon laser 2 prism system 3,4,5 measuring attenuators 6 calibrating/ shutter attenuator 7 condensing lens 8 sample compartment 9 annuli 10 safety attenuator 11 relay lens 12 field stops 13 interference filter 14 analyzing polarizer 15 microscope objective 16 photomultiplier... Fig. 8.2.1. Low angle laser light scattering photometer (Chromatix KMX-6) simplified optical diagram. 1 Flelium-neon laser 2 prism system 3,4,5 measuring attenuators 6 calibrating/ shutter attenuator 7 condensing lens 8 sample compartment 9 annuli 10 safety attenuator 11 relay lens 12 field stops 13 interference filter 14 analyzing polarizer 15 microscope objective 16 photomultiplier...
The scattered light is then imaged by a relay lens (11) onto the field stops (12), which are contained on a wheel and vary in size from 1.5 to 0.005 mm. Beyond the field stops are two lenses between which are inserted an interference filter (13) centered on 633 nm and with a bandwidth of 4nm to eliminate the fluorescence and an analyzing polarizer (14) which measures both the vertical and horizontal components of the scattered light. Immediately behind the field stops lies a microscope objective (15) which allows observation of the light scattered from the sample solution so that the system can be aligned appropriately. [Pg.502]

Selection of the annulus and field stop this allows determination of a and 1 ... [Pg.503]

Fig. 2 Fractograms were obtained with a Sd-FFF apparatus (77 X 1 X 0.0125 cm), (a) RBC elution profile on a new or properly washed FFF channel. Elution conditions flow injection of 5 X 10 RBCs (1/20 dilution of total blood in phosphate buffer saline pH 7.4/0.1 % of bovine albumin) external field 9.45g (1 g = 9.81 cm/s ) flow rate 0.7 mL/min, photometric detection at A = 313 nm. (b) Channel poisoning effect observed after 47 identical injections Idescribed in (A)], (c) Two sequences of RBC elution and channel cleaning procedure. Each sequence is RBC fractogram (flow injection of 5 X 10 RBCs (1/20 dilution of total blood in phosphate buffer saline pH 7.4), external field 25.7g, flow rate of 1.02 mL/min, photometric detection at A = 313 nm), external field stopped (S.R.), hypo-osmolar shock with doubly distilled water, cleaning agent (C.A.) signal, second water washing, (d) Example of fragile nucleated cells eluted in Sd-FFF neuroblasts (NB) case. Elution conditions flow injection of 1.5 X 10 neuroblasts in phosphate buffer saline pH 7.4/0.1 % of bovine albumin), external field 60.0g, flow rate of 1.25 mL/min, photometric detection at A = 254 nm. (e) Separation of components from an artificial mixture of neuroblasts and RBC. Elution conditions flow injection of 1.5 X 10 neuroblasts and 5 X 10 RBC in phosphate buffer saline pH 7.4/0.1 % of bovine albumin, external field 50.0g, flow rate of 1.25 mL/min, photometric detection at A = 254 nm. Fig. 2 Fractograms were obtained with a Sd-FFF apparatus (77 X 1 X 0.0125 cm), (a) RBC elution profile on a new or properly washed FFF channel. Elution conditions flow injection of 5 X 10 RBCs (1/20 dilution of total blood in phosphate buffer saline pH 7.4/0.1 % of bovine albumin) external field 9.45g (1 g = 9.81 cm/s ) flow rate 0.7 mL/min, photometric detection at A = 313 nm. (b) Channel poisoning effect observed after 47 identical injections Idescribed in (A)], (c) Two sequences of RBC elution and channel cleaning procedure. Each sequence is RBC fractogram (flow injection of 5 X 10 RBCs (1/20 dilution of total blood in phosphate buffer saline pH 7.4), external field 25.7g, flow rate of 1.02 mL/min, photometric detection at A = 313 nm), external field stopped (S.R.), hypo-osmolar shock with doubly distilled water, cleaning agent (C.A.) signal, second water washing, (d) Example of fragile nucleated cells eluted in Sd-FFF neuroblasts (NB) case. Elution conditions flow injection of 1.5 X 10 neuroblasts in phosphate buffer saline pH 7.4/0.1 % of bovine albumin), external field 60.0g, flow rate of 1.25 mL/min, photometric detection at A = 254 nm. (e) Separation of components from an artificial mixture of neuroblasts and RBC. Elution conditions flow injection of 1.5 X 10 neuroblasts and 5 X 10 RBC in phosphate buffer saline pH 7.4/0.1 % of bovine albumin, external field 50.0g, flow rate of 1.25 mL/min, photometric detection at A = 254 nm.
By using a field stop in front of the detector, light from outside the focus can be suppressed. This can be useful to suppress fluorescence of the cuvette walls, fluorescence of dye moleeules bound to the cuvette walls, or distortions by scattering or reabsorption. Confocal detection can also be used to reduce the daylight-sensitivity of the detection system. [Pg.73]

As a rule of thumb, no parts of the housing, lens holders, or the inside of optical tubes should be visible from the active area of the detector. This can be achieved by circular stops that restrict either the field of view of the detector (field stops) or the effective aperture of a beam (aperture stops). The term baffle is often used baffles are cylindrical or conical tubes or circular stops that keep off unwanted light from the detector [71]. [Pg.288]

Another way to suppress stray light is through field stops and aperture stops. A field stop is placed in a conjugate image plane of the excited spot in the sample. An aperture stop is placed most efficiently in the image plane of another aperture, which can be another stop, a lens, or a mirror. Two examples are shown in Fig. 7.29. A lens, LI, focuses a laser beam into a sample. The light emitted by the... [Pg.288]

An extreme example of a field stop is eonfoeal deteetion, where the stop is a pinhole that blocks all light that does not eome from a diffraetion-limited spot in... [Pg.289]

Fig. 1. TIRF microscope. (A) A view of the TIRF system. (B)View looking down on the back of the microscope (environmental chamber at bottom, back of the system at the top). Arrow b indicates the location of the Selection Prism containing the 80%/ 20% beamsplitter. Pulling the knob at the top to its full upwards position sets the beamsplitter to 100%/ 0% (all Epi-illumination input to the microscope). Pushing it downward sets the beamsplitter to 80% laser and 20% epifluo-rescence illumination. (B ) Location of the Field Diaphragm and the Field Stop on the epifluorescence arm of the split box. Two arrows AS and FS indicate Aperture Stop and Field Stop, respectively. Adjustment of these is vital for good IRM imaging. (B ) The laser input from which the screw white arroW) for TIRF angle adjustment projects. This pair of screws laterally translocates the laser path off center in the objective so that the angle of reflection is altered. Fig. 1. TIRF microscope. (A) A view of the TIRF system. (B)View looking down on the back of the microscope (environmental chamber at bottom, back of the system at the top). Arrow b indicates the location of the Selection Prism containing the 80%/ 20% beamsplitter. Pulling the knob at the top to its full upwards position sets the beamsplitter to 100%/ 0% (all Epi-illumination input to the microscope). Pushing it downward sets the beamsplitter to 80% laser and 20% epifluo-rescence illumination. (B ) Location of the Field Diaphragm and the Field Stop on the epifluorescence arm of the split box. Two arrows AS and FS indicate Aperture Stop and Field Stop, respectively. Adjustment of these is vital for good IRM imaging. (B ) The laser input from which the screw white arroW) for TIRF angle adjustment projects. This pair of screws laterally translocates the laser path off center in the objective so that the angle of reflection is altered.
Adjust the Field Diaphragm or Field Stop (FS, a second light intensity control after AS before 20/80 prism in the light path) to obtain the best contrast of adhering membranes or structures and background (Fig. lb and B , see FS). [Pg.219]

Due to the anisotropy of conductivity, space charges will develop as indicated in fig. 3.10.7 till the transverse electric field stops the transverse current. The local transverse field in the steady state is easily seen to be... [Pg.185]

As mentioned earlier, it is not likely that the entire spectral region would be included in a single spectrum. Instead, optical filters are used to restrict the spectral region. In order to optimize the overall system performance, it is desirable to match the angular field-of-view to the selected spectral region. This can be done by inserting a variable aperture at a field-stop in the optical... [Pg.431]

Light or magnetic sensing field stop machine or prevent starting if any part of body is within the sensing field. [Pg.643]

Fluorescence detection is usually performed on column, using an approach similar to that described for absorbance detectors. Excitation is collected through an objective at 90° to the excitation beam. Filters and field stops are used to block scatter and... [Pg.352]


See other pages where Field stop is mentioned: [Pg.220]    [Pg.225]    [Pg.240]    [Pg.296]    [Pg.55]    [Pg.274]    [Pg.173]    [Pg.110]    [Pg.263]    [Pg.268]    [Pg.110]    [Pg.217]    [Pg.153]    [Pg.618]    [Pg.325]    [Pg.328]    [Pg.108]    [Pg.238]    [Pg.91]    [Pg.91]    [Pg.464]    [Pg.124]    [Pg.287]    [Pg.288]    [Pg.289]    [Pg.289]    [Pg.212]    [Pg.212]    [Pg.222]    [Pg.368]    [Pg.371]    [Pg.799]   
See also in sourсe #XX -- [ Pg.98 ]

See also in sourсe #XX -- [ Pg.159 , Pg.161 ]




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