Observations of phase changes in monoolein during high viscous injection

Wells, D.J.; Berntsen, P.; Balaur, E.; Kewish, C.M.; Adams, P.; Aquila, A.; Binns, J.; Boutet, S.; Broomhall, H.; Caleman, C.; Christofferson, A.; Conn, C.E.; Dahlqvist, C.; Flueckiger, L.; Gian Roque, F.; Greaves, T.L.; Hejazian, M.; Hunter, M.; Hadian Jazi, M.; Jönsson, H.O.; Pathirannahalage, S.K.; Kirian, R.A.; Kozlov, A.; Kurta, R.P.; Marman, H.; Mendez, D.; Morgan, A.; Nugent, K.; Oberthuer, D.; Quiney, H.; Reinhardt, J.; Saha, S.; Sellberg, J.A.; Sierra, R.; Wiedorn, M.; Abbey, B.; Martin, A.V.; Darmanin, C.

doi:10.1107/S1600577522001862

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Figure 3
Radial diffraction profiles showing the coexistence of crystal lamellar (L_c) and cubic (Pn3m and Ia3d) phases when injected into air at the Australian Synchrotron: (a, c) sample A1, (b, d) sample A2. Both samples were mixed with the ratio of 60:40 MO/water (w/w). Panels (a) and (b) represent the average diffraction profile. Vertical lines indicate the peak positions implied by the crystallographic space group and the stated lattice parameter. Panels (c) and (d) show the evolution of the diffraction profiles over the course of the data collection of a single sample and indicate the simultaneous presence of the lamellar and cubic phases.

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ISSN: 1600-5775

Volume 29| Part 3| May 2022| Pages 602-614

https://doi.org/10.1107/S1600577522001862

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