Incident triangle

One example as to how occupational and process safety need to be distinguished is to do with the much-quoted Incident Triangle, shown in Figure 1.7, which uses created information. 

Accident investigation indicates that there are often many individual causes to an accident, and that a series of incidents occur simultaneously to cause the accident. The following figure is called the safety triangle", and shows the approximate ratios of occurrence of accidents with different severities. This is based on industrial statistics. 

Figure 4.10 The diffraction and rediffraction of an X-ray beam from a set of reflecting planes. The triangle bounded by the incident beam and the diffracted beam from the entry surface is called the Borrmann fan...

Figure 24 Incident photon energy dependence of the surface charge separation efficiency (h" / photon) measured by PITCS. Squares, circles, triangles, and diamonds represent the results obtained for Cr-implanted rutile, Cr-doped rutile, undoped rutile, and anatase Ti02 films, respectively.

Figure 17.33 Jsc versus incident irradiance plot Lil/I2 0.3/0.03 M + 0.1M Tbpy in acetonitrile in conjunction with N3 (squares) Lil/I2 0.3/0.03 M + 0.1 M Tbpy in acetonitrile in conjunction with Z907 (circles) Co(II)(DTB)32 + 0.15M + 0.5 M Li+ + 0.1 M Tbpy in acetonitrile in conjunction with Z907 (triangles) 120 pm spacer. From Bignozzi et al., unpublished results.

Consequently, the third face incident to v2 is a 10-gon, thus the sought /-fulleroid must contain the substructure depicted in Figure 19.5, where the 3- and the 5-fold rotation centers are indicated by a small triangle and a 5-gon, respectively. By applying these rotations in a systematic way, we obtain the structure shown in Figure 19.3. ... 

At 795 cm 1 LiI03 has a transverse A phonon. Fig. 5 shows the shift of the Raman line towards lower wave numbers for decreasing angles between the directions of the incident and scattered light. Because the wave vector triangle lies in the isotropic Ary-plane, k is always perpendicular to the optical axis and no directional dispersion is to be expected, therefore the shift of the line is due only to the variation of the magnitude of the wave vector. 

Figure 4.24 Extraction of one-dimensional position information from a channelplate detector by using a discrete multianode with an RC line. For an explanation of the strips and the dashed circular area see the caption of Fig. 4.23. Each strip is connected to the RC line indicated by the resistor and capacitor symbols. The total charge Q of the electron avalanche (shaded area) incident on the multianode flows to both ends of the RC line, giving Qi and Q2 in amounts proportional to the distances (P, L) and (0, P), respectively. The two preamplifiers in which these charges are collected are indicated by triangles. From...

Figure 9 Probability distributions for the reaction times, defined at the total time between the start of the trajectory and the point at which the product molecule is 7 A above the surface, for H incident on a D-covered Ni(l 00) surface, and an initial D coverage of 0.93 ML. Results are shown for HD formed on a rigid (open squares) and moving (open circles) lattice, and D2 formed on a rigid (filled triangles) and moving (open diamonds) lattice.

Figure 16 Incidence kinetic energy dependence of the excitation and de-excitation probability for NO(v = 2) scattering from Au(l 1 1) for two surface temperatures. De-excitation (v = 2 -> 1) triangles and diamonds. Excitation (v = 2 -> 3) squares and circles. Lines are explained in the original reference. From Huang et al. [135].

Fig. 1.2. Age-specific rates of all events and of incident events for stroke (i.e. not including transient ischemic attack closed circles), myocardial infarction and sudden cardiac death combined (i.e. not including unstable angina open circles), and acute peripheral vascular events (triangles) in men and women in Oxfordshire from 2002 to 2005 (Rothwell et a . 2005).

Figure 5. The distributions of the recrossing trajectories over configurational surface S qi = 0) at time t = 0 on the phase-space planes (pf (p,q), (p,q)) at E = 0.5e, where most modes are strongly chaotic—except 4i(p,q). (a) First and (b) second orders The circle and triangle symbols denote the system trajectories having negative and positive incident momenta p (t = 0) on the S(qi = 0), and the open and filled symbols denote those whose final states were predicted correctly and falsely by Eq. (11), respectively [45].

Figure 15.10 Simulated intensity images, Ix (top) and ly (bottom) of the electromagnetic field distribution for 2.45 GHz microwave frequencies incident upon (2) 2-D equilateral triangles with 12.3 mm length and oriented with the sample geometry shown (middle). The incident field is held constant and the gap size is varied in subsequent simulations, 1 mm (left) and 12 mm (right) gap size examples are shown. Bottom Maximum I (lx (Ey2) + ly (Ey2)) pixel intensity versus gap (Top, Inset), expanded view of maximum pixel intensity versus gap size.

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