With a highly convergent electron beam entering a small crystal area, the Bragg condition may be fulfilled simultaneously for many diffraction orders along a reciprocal-lattice direction, and reflections with (sin 0)/2 > 2 A-t are accessible. Considerations based on the dynamical theory of electron diffraction suggest that for Bragg reflections with (sin 0)/2>l/k -x, 100 keV electrons can be treated quasi-kinematically when the crystal thickness is less than 1000 ,~,, and this is supported by experiments. This simple approach has been used to determine the D-induced static displacement modulation 6 of V along the a axis (monochlinic indexing) in the/~ phase of VzD. From visual inspection of the Bragg intensities for large diffraction orders, up to (sin 0)/2=2.35/k -x, it is concluded that 6 = 0-070 (5)/k.