The cellular processes underpinning life are orchestrated by proteins and their interactions. The associated structural and dynamic heterogeneity, despite being key to function, poses a fundamental challenge to existing analytical and structural methodologies. We used interferometric scattering microscopy to quantify the mass of single biomolecules in solution with 2% sequence mass accuracy, up to 19-kilodalton resolution, and 1-kilodalton precision. We resolved oligomeric distributions at high dynamic range, detected small-molecule binding, and mass-imaged proteins with associated lipids and sugars. These capabilities enabled us to characterize the molecular dynamics of processes as diverse as glycoprotein cross-linking, amyloidogenic protein aggregation, and actin polymerization. Interferometric scattering mass spectrometry allows spatiotemporally resolved measurement of a broad range of biomolecular interactions, one molecule at a time.

Very often, the positions of flexible domains within macromolecules as well as within macromolecular complexes cannot be determined by standard structural biology methods. To overcome this problem, we developed a method that uses probabilistic data analysis to combine single-molecule measurements with X-ray crystallography data. The method determines not only the most likely position of a fluorescent dye molecule attached to the domain but also the complete three-dimensional probability distribution depicting the experimental uncertainty. With this approach, single-pair fluorescence resonance energy transfer measurements can now be used as a quantitative tool for investigating the position and dynamics of flexible domains within macromolecular complexes. We applied this method to find the position of the 5¢ end of the nascent RNA exiting transcription elongation complexes of yeast (Saccharomyces cerevisiae) RNA polymerase II and studied the influence of transcription factor IIB on the position of the RNA.In recent years, high-resolution structural models of large macromolecular complexes such as the ribosome 1 , the RecBCD helicase 2 or RNA polymerases 3,4 have been obtained using X-ray crystallography. Although these structures provide detailed insight into the molecular architecture of complex biological systems, the position of flexible domains can usually not be determined because of averaging effects.Single-molecule methods, on the other hand, provide the possibility of directly obtaining structural information because they allow the study of real-time conformational changes of macromolecular complexes 5 . In combination with fluorescence resonance energy transfer (FRET) 6 , a technique that has been termed a molecular ruler 7 , one can in principle measure distances within a macromolecule in real-time. However, because of experimental problems such as variations in quantum yield 8 or dependence of FRET on the orientations of the two dye molecules 9 , there are few examples in the literature of quantitative distance measurements 8,10-12 or position determination 13-16 using single-pair FRET (sp-FRET). Instead, these data are more often interpreted in a qualitative fashion monitoring conformational changes and length increases or decreases [17][18][19][20] .Using triangulation of several FRET distance measurements, it is possible to determine a previously unknown position [13][14][15][16][21][22][23] . Although these experiments are able to estimate the most likely position, they do not show how existing experimental uncertainties might affect the position determined. Therefore, these positions must be interpreted with great caution because one has no information about the experimental accuracy. In principle, one can conduct control measurements that provide validity tests of the position determined 14 , but to arrive at a quantitative technique, experimental uncertainties must be taken into account.Here we used bayesian parameter estimation 21 , a probabilitybased analysis method, to compute the three-dimen...

To dissect the kinetics of structural transitions underlying the stepping cycle of kinesin-1 at physiological ATP, we used interferometric scattering microscopy to track the position of gold nanoparticles attached to individual motor domains in processively stepping dimers. Labeled heads resided stably at positions 16.4 nm apart, corresponding to a microtubule-bound state, and at a previously unseen intermediate position, corresponding to a tethered state. The chemical transitions underlying these structural transitions were identified by varying nucleotide conditions and carrying out parallel stopped-flow kinetics assays. At saturating ATP, kinesin-1 spends half of each stepping cycle with one head bound, specifying a structural state for each of two rate-limiting transitions. Analysis of stepping kinetics in varying nucleotides shows that ATP binding is required to properly enter the onehead-bound state, and hydrolysis is necessary to exit it at a physiological rate. These transitions differ from the standard model in which ATP binding drives full docking of the flexible neck linker domain of the motor. Thus, this work defines a consensus sequence of mechanochemical transitions that can be used to understand functional diversity across the kinesin superfamily.kinesin | iSCAT | microscopy | structural kinetics | structure-function K inesin-1 is a motor protein that steps processively toward microtubule plus-ends, tracking single protofilaments and hydrolyzing one ATP molecule per step (1-6).Step sizes corresponding to the tubulin dimer spacing of 8.2 nm are observed when the molecule is labeled by its C-terminal tail (7-10) and to a two-dimer spacing of 16.4 nm when a single motor domain is labeled (4,11,12), consistent with the motor walking in a handover-hand fashion. Kinesin has served as an important model system for advancing single-molecule techniques (7-10) and is clinically relevant for its role in neurodegenerative diseases (13), making dissection of its step a popular ongoing target of study.Despite decades of work, many essential components of the mechanochemical cycle remain disputed, including (i) how much time kinesin-1 spends in a one-head-bound (1HB) state when stepping at physiological ATP concentrations, (ii) whether the motor waits for ATP in a 1HB or two-heads-bound (2HB) state, and (iii) whether ATP hydrolysis occurs before or after tethered head attachment (4,11,(14)(15)(16)(17)(18)(19)(20). These questions are important because they are fundamental to the mechanism by which kinesins harness nucleotide-dependent structural changes to generate mechanical force in a manner optimized for their specific cellular tasks. Addressing these questions requires characterizing a transient 1HB state in the stepping cycle in which the unattached head is located between successive binding sites on the microtubule. This 1HB intermediate is associated with the force-generating powerstroke of the motor and underlies the detachment pathway that limits motor processivity. Optical trapping (7,19,21,22) and sin...

Optical detection of individual proteins requires fluorescent labeling. Cavity and plasmonic methodologies enhance single molecule signatures in the absence of any labels but have struggled to demonstrate routine and quantitative single protein detection. Here, we used interferometric scattering microscopy not only to detect but also to image and nanometrically track the motion of single myosin 5a heavy meromyosin molecules without the use of labels or any nanoscopic amplification. Together with the simple experimental arrangement, an intrinsic independence from strong electronic transition dipoles and a detection limit of <60 kDa, our approach paves the way toward nonresonant, label-free sensing and imaging of nanoscopic objects down to the single protein level.

Single-pair fluorescence resonance energy transfer was used to track RNA exiting from RNA polymerase II (Pol II) in elongation complexes. Measuring the distance between the RNA 5 end and three known locations within the elongation complex allows us determine its position by means of triangulation. RNA leaves the polymerase active center cleft via the previously proposed exit tunnel and then disengages from the enzyme surface. When the RNA reaches lengths of 26 and 29 nt, its 5 end associates with Pol II at the base of the dock domain. Because the initiation factor TFIIB binds to the dock domain and exit tunnel, exiting RNA may prevent TFIIB reassociation during elongation. RNA further extends toward the linker connecting to the polymerase C-terminal repeat domain (CTD), which binds the 5-capping enzyme and other RNA processing factors.Pol II ͉ transcription ͉ FRET ͉ triangulation ͉ fluorescence P ol II synthesizes all eukaryotic mRNA and comprises 12 subunits, Rpb1 to Rpb12. An atomic model of Pol II has been obtained by x-ray crystallography (1, 2). Additional studies of Pol II-nucleic acid complexes have given insights into the elongation complex structure and molecular aspects of the transcription mechanism (3-7). Crystallographic analysis detected the position of the nascent RNA within the DNA-RNA hybrid above the active site (positions ϩ1 to Ϫ8, with ϩ1 denoting the nucleotide addition site) and for 2 nt upstream of the hybrid after the point of DNA-RNA strand separation (positions Ϫ9 and Ϫ10) (3, 7). The last-ordered RNA nucleotide is located at the entrance to a tunnel [called the RNA exit channel for the bacterial RNA polymerase (8)], which is formed among the polymerase wall, clamp, and lid. This tunnel leads from the active center cleft to the exterior and was proposed to accommodate exiting RNA (1,3,6,7). Beyond the putative exit tunnel, two prominent surface grooves on either side of the dock domain in principle could further accommodate exiting RNA (1, 9). Groove 1 winds along the base of the clamp toward the Rpb4/7 subcomplex, whereas groove 2 leads along Rpb11 toward Rpb8. Recently, nascent RNA could be crosslinked to Rpb7, providing apparent support for groove 1 (10). RNA beyond position Ϫ10 was present in one of the crystallographic studies of the elongation complex (3) but could not be observed in the tunnel or in the subsequent grooves, suggesting that its interactions, if they exist, are transient and cannot be detected in medium-resolution electron density maps.To study if the nascent RNA indeed exits through the proposed tunnel, and whether it follows a defined surface path beyond the tunnel, we used single-molecule fluorescence experiments. Singleparticle methods prevent the loss of information because of averaging that is inherent to bulk experiments and crystallography (11)(12)(13)(14). Fluorescence resonance energy transfer between two fluorophores [single-pair (sp)-FRET] provides a very sensitive tool for studying distances and conformational changes within biological complexes in the ...

Crystallographic studies of the RNA polymerase II (Pol II) elongation complex (EC) revealed the locations of downstream DNA and the DNA-RNA hybrid, but not the course of the nontemplate DNA strand in the transcription bubble and the upstream DNA duplex. Here we used single-molecule Fluorescence Resonance Energy Transfer (smFRET) experiments to locate nontemplate and upstream DNA with our recently developed Nano Positioning System (NPS). In the resulting complete model of the Pol II EC, separation of the nontemplate from the template strand at position +2 involves interaction with fork loop 2. The nontemplate strand passes loop β10-β11 on the Pol II lobe, and then turns to the other side of the cleft above the rudder. The upstream DNA duplex exits at an approximately right angle from the incoming downstream DNA, and emanates from the cleft between the protrusion and clamp. Comparison with published data suggests that the architecture of the complete EC is conserved from bacteria to eukaryotes and that upstream DNA is relocated during the initiation–elongation transition.

Supported lipid bilayers (SLB) are frequently used to study processes associated with or mediated by lipid membranes. The mechanism by which SLBs form is a matter of debate, largely due to the experimental difficulty associated with observing the adsorption and rupture of individual vesicles. Here, we used interferometric scattering microscopy (iSCAT) to directly visualize membrane formation from nanoscopic vesicles in real time. We observed a number of previously proposed phenomena such as vesicle adsorption, rupture, movement, and a wave-like bilayer spreading. By varying the vesicle size and the lipid-surface interaction strength, we rationalized and tuned the relative contributions of these phenomena to bilayer formation. Our results support a model where the interplay between bilayer edge tension and the overall interaction energy with the surface determine the mechanism of SLB formation. The unique combination of sensitivity, speed, and label-free imaging capability of iSCAT provides exciting prospects not only for investigations of SLB formation, but also for studies of assembly and disassembly processes on the nanoscale with previously unattainable accuracy and sensitivity.

Myosin 5a is a dual-headed molecular motor that transports cargo along actin filaments. By following the motion of individual heads with interferometric scattering microscopy at nm spatial and ms temporal precision we found that the detached head occupies a loosely fixed position to one side of actin from which it rebinds in a controlled manner while executing a step. Improving the spatial precision to the sub-nm regime provided evidence for an ångstrom-level structural transition in the motor domain associated with the power stroke. Simultaneous tracking of both heads revealed that consecutive steps follow identical paths to the same side of actin in a compass-like spinning motion demonstrating a symmetrical walking pattern. These results visualize many of the critical unknown aspects of the stepping mechanism of myosin 5 including head–head coordination, the origin of lever-arm motion and the spatiotemporal dynamics of the translocating head during individual steps.DOI: http://dx.doi.org/10.7554/eLife.05413.001