The nematic twist-bend (N TB ) liquid crystal phase possesses a local helical structure with a pitch length of a few nanometres and is the first example of spontaneous symmetry breaking in a fluid system. All known examples of the N TB phase occur in materials whose constituent mesogenic units are aromatic hydrocarbons. It is not clear if this is due to synthetic convenience or a bona fide structural requirement for a material to exhibit this phase of matter. In this work we demonstrate that materials consisting largely of saturated hydrocarbons can also give rise to this mesophase.Furthermore, we find that replacement of 1,4-disubstituted benzene with trans 1,4-cyclohexane or 1,4-cubane does not especially alter the transition temperatures of the resulting material nor does it appear to impact upon the heliconical tilt angle. Each of these three units is effectively rigid and linear; calculating the probability distribution of bend angles for each compound reveals that the isosteric groups has little impact on the overall molecular shape, demonstrating the shape-driven nature of the N TB phase. Conversely, we find that incorporation of 2,6-disubstituted cuneane -a saturated hydrocarbon which is rigid but not linear -supresses the formation of the N TB phase.Liquid crystals are a collection of states of matter (mesophases) which possess orientational and/or positional order not found in the liquid state. Different LC mesophase are principally characterised by their degree of positional order; the nematic LC phase possesses long range orientational order, whereas smectic phases also exhibit positional order in one dimension. The discovery of nematic phases in which the average orientational order varies periodically -so called modulated nematics -has recently attracted significant interest. [1][2][3][4][5][6] The twist-bend nematic phase (N TB ) exhibits a heliconical precession of the nematic director through space with a periodic length scale of a few tens of nanometers. [7][8][9] This phase is typically found in materials comprising two or more mesogenic units which are mutually appended by a central spacer of such a length as to impart a gross bent shape. The incidence of the N TB phase is intimately linked to molecular shape, specifically the bend angle between adjacent mesogenic units. [10][11][12][13][14] The mesogenic units themselves are almost exclusively constructed from multiple benzene rings, and to date (as far as the authors are aware) the spacer is always appended to an aromatic ring rather than a saturated hydrocarbon; [15][16][17][18][19][20][21][22][23] it is not clear if this is a consequence of synthetic convenience or a real structural requirement for materials to exhibit this phase of matter.