Discovering the Power of Single Molecules

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Discovering the Power of Single Molecules Robert A. Forties, Michelle D. Wang  Cell  Volume 157, Issue 1, Pages 4-7 (March 2014) DOI: 10.1016/j.cell.2014.02.011 Copyright © 2014 Elsevier Inc. Terms and Conditions

Figure 1 Some Novel Enhancements of Single-Molecule Manipulation Techniques (A) Torque measurement using the rotary bead assay (Bryant et al., 2003). One end of a DNA molecule was attached to a bead held in an optical trap, and the other end to a bead which was rotated by a micropipette. A smaller bead was attached internally to the DNA, just above a nick in the DNA backbone, which allowed this bead to rotate freely. The torque applied to the DNA was inferred by how much the rotation of this smaller bead, which experiences viscous drag, lagged behind the rotation of the micropipette. (B) Visualizing supercoil migration using magnetic tweezers and fluorescence (van Loenhout et al., 2012). A long DNA molecule was twisted by rotating the magnetic tweezers, and then extended laterally. The DNA was labeled with fluorescent dyes. Plectonemes were revealed as bright fluorescent spots. (C) Measurement of the torque generated by RNA polymerase (RNAP) using an angular optical trap (Ma et al., 2013). An RNAP was torsionally constrained to a coverslip surface, and the upstream DNA was torsionally constrained to the bottom of a nanofabricated quartz cylinder held in an angular optical trap. As the RNAP translocated along the DNA, RNAP generated (−) supercoils in the upstream DNA and eventually reached a stall. The angular optical trap monitored the transcription and the torque that RNAP generated in real time. (D) Abbreviated procedure for the measurement of the RecA homology search using a multichannel flow cell (Forget and Kowalczykowski, 2012). Step 1: A DNA molecule, labeled with YOYO1 for visualization, was tethered at both ends to beads held in optical traps. Step 2: the DNA was moved to a different channel of the flow cell to remove the YOYO1. Step 3: the DNA was moved to a reservoir containing fluorescently labeled RecA filaments and incubated at a fixed extension without flow. Step 4: the DNA was returned to the flow cell and extended to visualize RecA binding. (E) Characterization of single-stranded binding protein (SSB) diffusion using optical trapping and FRET (Zhou et al., 2011). SSB was bound to a segment of ssDNA held between two dsDNA anchors, with one anchor attached to a coverslip surface and the other attached to a bead held in an optical trap. Force applied by the optical trap was used to control the degree of ssDNA unwrapping from the SSB. A donor dye (green) was attached to SSB, and an acceptor dye (red) to the ssDNA, allowing motion of the ssDNA relative to SSB to be monitored using FRET. (F) A DNA curtain experiment used to observe collisions between RecBCD and a nucleosome (Finkelstein et al., 2010). An array of DNA molecules, each attached at one end to a fabricated surface, was fluorescently labeled and extended using flow. This allowed the progress of a RecBCD enzyme, attached to the free end of the DNA, to be monitored as it displaced the fluorophores attached to the DNA. The nucleosome was fluorescently labeled with a different dye. When RecBCD encountered a nucleosome, both the fates of the RecBCD and the nucleosome were monitored. Cell 2014 157, 4-7DOI: (10.1016/j.cell.2014.02.011) Copyright © 2014 Elsevier Inc. Terms and Conditions