Correct reconstruction of macromolecular structure by cryo-electron microscopy (cryo-EM) relies on accurate determination of the orientation of single-particle images. For small (<100 kDa) DNA-binding proteins, obtaining particle images with sufficiently asymmetric features to correctly guide alignment is challenging. We apply DNA origami to construct molecular goniometers—instruments that precisely orient objects—and use them to dock a DNA-binding protein on a double-helix stage that has user-programmable tilt and rotation angles. We construct goniometers with 14 different stage configurations to orient and visualize the protein just above the cryo-EM grid surface. Each goniometer has a distinct barcode pattern that we use during particle classification to assign angle priors to the bound protein. We use goniometers to obtain a 6.5-Å structure of BurrH, an 82-kDa DNA-binding protein whose helical pseudosymmetry prevents accurate image orientation using traditional cryo-EM. Our approach should be adaptable to other DNA-binding proteins as well as small proteins fused to DNA-binding domains.
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The cryo-EM map of BurrH has been deposited in the Electron Microscopy Data Bank (EMD-21443). The cryo-EM movie files have been deposited at the Electron Microscopy Public Image Archive (EMPIAR-10373). The p9344-BurrH scaffold sequence has been submitted to GenBank (MT081208) and the plasmid deposited with AddGene (no. 140326).
Source code is available at https://github.com/douglaslab/cryoorigami.
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We thank F. Wang for furnishing amino-graphene-oxide grids and protocols for early tests. We thank D. Bulkley and A. Myasnikov for help with cryo-EM data collection. We thank J. Brown and C. Gingold for help with visualization. T.A. was supported by the Ruth L. Kirschstein NRSA Postdoctoral Fellowship grant no. F32GM119322. S.M.D. was supported by the UCSF Program for Breakthrough Biomedical Research, Pew-Stewart Scholars Program, NSF CAREER award no. 1453847 and NIH grant no. R35GM125027. Y.C. is an investigator of the Howard Hughes Medical Institute and was supported by NIH grant nos. R01GM098672, R01HL134183, S10OD021741 and S10OD020054.
The authors declare no competing interests.
Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Extended Data Fig. 1 Comparison of grid adsorption orientation and signal delocalization for two chassis designs.
a, Representative negative-stain micrographs of chassis with 0.67 aspect ratio. b, Representative cryo-EM micrograph of chassis with 0.59 aspect ratio. Desired orientations assessed by manual counting. c, Top: Representative 2D class average of 0°-rotation goniometer from a. The chassis aperture exhibits a shadow that overlaps the DNA stage and BurrH protein. Bottom: Representative 2D class averages of BurrH, exhibiting artifacts that we hypothesized are due to delocalized origami signal in the 0.5–2.0 µm defocus range used for image acquisition. d, Top: 2D class of 0°-rotation goniometer from b designed to reduce shadow overlap. Bottom: Representative BurrH 2D class averages. Artifacts observed in c are significantly reduced. Scale bars: a, b: 100 nm, c, d: 25 nm (top), 10 nm (bottom).
Independent 2D views of a 3D object can be derived using only two orthogonal rotational transformations. In cryo-EM, the two orthogonal rotations can be referred to as tilt and rotation angles, respectively12,30. The reference coordinate system for the rotation operations can be chosen arbitrarily, and here we define the goniometer tilt angle as the angle between the stage DNA and the normal vector perpendicular to the goniometer face (the normal vector is parallel to the electron beam (Fig. 1a, orange line labeled e–) when the goniometer adsorbs in the desired face-up orientation. We define the goniometer rotation angle as the rotation angle with respect to the axis parallel to the DNA stage helical axis.
a, Bit and rotation angles for each column. b, +90 tilt, 414-nt rotation bit designs. TILT bit is inactive (red outline in bottom right corner of each schematic). c, –90 tilt, 414-nt rotation bit designs. TILT bit is active. d, +90 tilt, 222-nt rotation bit designs. TILT bit is inactive.
a, +90 tilt, 414-nt bit b, –90 tilt, 414-nt bit (flipped), c, +90 tilt, 222-nt bit. Scale bars: 100 nm.
a, Centering goniometer classes at tilt DNA. b, Picking protein particles from the center of goniometers. c, 2D classification of BurrH particles and removing “bad” classes. d, Recentering “good” classes. e, Building an initial model 3D model with tilt and rot angle constraints. f, Aligning BurrH particles to initial model with tilt and rot angle constraints and regularization parameter, T, set to 6 for better alignment. g, Classifying particles into five 3D classes with tilt angle constraint on and regularization parameter, T, set to 2 to minimize overfitting during classification. Best 3D class (magenta) is at 7.3 Å resolution. h, Refining the best 3D class with only the tilt angle constraint. Estimated resolution of the refined map is 6.5 Å.
Representative 2D classes of stage DNA with BurrH after one round of 2D classification. Classes with high background signal, with empty tilt DNA and DNA origami signal are removed before further 2D classification of BurrH bound to stage DNA. b, “Good” 2D classes retained for 3D reconstruction and refinement of BurrH. Scale bar is 20 nm.
Extended Data Fig. 7 Measured tilt, rotation, and psi angle distributions for all goniometer designs.
Polar plots and histograms follow the convention from Fig. 6. The inner tick mark represents the goal angle, and the arc shows the bounds of the Gaussian angle prior. Average rotation angles are plotted as magenta lines for tilt and rotation plots.
a, Individual directional FSCs (gray lines), global FSC value (blue line) and ±1 standard deviation from global FSC (magenta dashed lines). b, Directional FSC map and its 2D projections. The minimum resolution (blue) and maximum resolution (magenta) are indicated for each 2D projection.
a, ResLog plots showing FSC vs. resolution for 3D refinement of BurrH using 1,000 to 68,482 particles. b, Resolution estimates from FSC0.143 vs. particles count. The resolution plateaus at 40k particles, suggesting our resolution is not limited by particle count. c, BurrH resolution vs. maximum micrograph defocus used in 3D reconstruction. d, Resolution estimates from FSC0.143 vs. maximum defocus. The resolution reaches a plateau at 1.5 µm and the addition of higher defocus particles doesn’t comprise the resolution. Inset shows the distribution of BurrH particle defocus in µm.
FSC and ResLog plots for BurrH 3D reconstructions in which particles are filtered when their estimated angles from the unfiltered 3D refinement differ from the goniometer goal angle. a, We compared three conditions: No filter (that is, identical to Fig. 6), and two conditions in which particles with assigned rotation angles that differ by >45°, and >90° from the goal angle. b, FSC curves comparing the 3D reconstruction for the three filtering conditions. c, Plot of particle count versus resolution estimate. Filtering reduces the particle count available for the 3D reconstruction, which in turn reduces the final resolution (see Extended Data Fig. 8b). Compared to the unfiltered reconstructions, removing particles in the indicated angle ranges does not improve the final BurrH resolution.
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Aksel, T., Yu, Z., Cheng, Y. et al. Molecular goniometers for single-particle cryo-electron microscopy of DNA-binding proteins. Nat Biotechnol 39, 378–386 (2021). https://doi.org/10.1038/s41587-020-0716-8
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