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SOLUTIONSMANUAL TO ACCOMPANY ATKINS' PHYSICAL CHEMISTRY 529 In this case there are a total of ten terms to include, h = 0 to 9. Figure 15.1 shows a plot of Vρ(x) against x; the electron density is at a maximum of 142/V at x = 0 or x = 1, the boundaries of the unit cell. 0.0 0.2 0.4 0.6 0.8 1.0 −50 0 50 100 150 x V ρ( x) Figure 15.1 E15B.9(b) �e Patterson synthesis is given by [15B.5–653], P(r) = 1 V ∑ hk l ∣Fhk l ∣ 2 e−2πi(hx+ky+l z) In this case the structure factors are only given for the x direction so the sum is just over the index h. Furthermore, because Fh = F−h the summation can be taken from from h = 0 to h = +∞. Using a similar line of argument to that in Exercise E15B.7(b), the Patterson synthesis is VP(x) = F20 + 2 ∞ ∑ h=1 F2h cos(2πhx) In this case there are a total of ten terms to include, h = 0 to 9. Figure 15.2 shows a plot of VP(x) against x. As expected, there strong feature at the origin; this arises from the separation between each atom and itself.�ere is also a strong feature at x = 1 which indicate that atoms are separated by 1× a unit along the x-axis. E15B.10(b) To constructor the Patterson map, choose the position of one atom to be the origin.�en add peaks to the map corresponding to vectors joining each pair of atoms (Fig. 15.3). �e vector between atom A and atom B has the same magnitude as that between B and A, but points in the opposite direction; the map therefore includes two symmetry related peaks on either side of the origin. �e vectors between each atom and itself give a peak at the centre point of the Patterson map, and the many contributions at this position create an intense peak.