helical microfibers are chiral, highly stretchable, and can be employed as micro-motors [7] and -swimmers. [8] However, current microfiber fabrication approaches offer limited control of the helical geometry.Microfluidic spinning technology (MST) has emerged as a tool to precisely tune the spatiotemporal chemical composition within microfibers. [9,10] MST employs a liquid precursor solution, which transforms into a semisolid fiber after flowing out of a microscopic orifice. Typical solidification mechanisms include ionic or chemical cross-linking, [11] photopolymerization, [12] and phase separation. [13] Helical fibers are formed in MST via the liquid rope coiling effect. [14,15] This hydrodynamic instability results in helices with large pitch lengths. [2] However, it remains difficult to combine multiple fibers into double, triple, or higher-order helices via liquid rope coiling. A better control of the helical multiplicity and shape can be realized upon actively rotating the microfibers. This has been shown for instance by Yasuda et al. in a planetary centrifuge. [16] But, these and other prevailing active fiber twisting methods are based on batch processing, limiting their technological potentials. [17,18] Recently, we have introduced microfluidic twisting (MT) to continuously generate composite helical fiber assemblies. [19] microfluidic twisting enables the combination of multiple helical fibers into high-order helices. The constituent fibers can have different sizes, twisting degrees, or chemical compositions. Although our prior work has explained the effect of the hydrodynamic forces controlling the helical pitch, the fundamental driving force of the helical assembly has not been elaborated. This knowledge gap has restricted the controlled collection of uniform helical fibers. Moreover, it has limited the choices of fiber precursor dispersions, resulting in strong, but inflexible helical fibers. [19] Here, we close this knowledge gap and show how centrifugal forces during microfluidic twisting enable the continuous assembly and collection of flexible, stimuli-responsive microropes. The assembly and collection of the microropes depends on the direction of the centrifugal force, which is determined by the density difference between the individual rope filaments and the surrounding fluid. The rope filaments in our work are composed of bicontinuous interfacially jammed emulsions gels (bijels) [20,21] formed via solvent transfer induced phase separation (STrIPS). [22][23][24][25] Bijels have potential applications as catalytic emulsions, [26] separation membranes, [23] battery components, [27,28] and sensors. [29] Interestingly, the density of the In microfluidics, centrifugal forces are important for centrifugal microfluidic chips and curved microchannels. Here, an unrecognized use of the centrifugal effect in microfluidics is introduced. The assembly of helical soft matter fibers in a rotating microcapillary is investigated. During assembly, the fibers undergo phase separation, generating particle stabilized...