Name: fast grid preparation for time-resolved cryo-electron microscopy
Uploaded: 2021-11-06T13:00:00
Description: Watch this Scientific Journal Video about Fast Grid Preparation for Time-Resolved Cryo-Electron Microscopy at JoVE.com

We would like to thank Molly S.C. Gravett for helpful discussions and the ABSL facility staff for help with cryo-EM data collection. David P. Klebl&#160;is a PhD student on the Wellcome Trust 4-year PhD program in The Astbury Centre funded by The University of Leeds. The FEI Titan Krios microscopes were funded by the University of Leeds (UoL ABSL award) and Wellcome Trust (108466/Z/15/Z). This work was funded by a BBSRC grant to Stephen P. Muench&#160;(BB/P026397/1) and supported by research grants to Howard D. White from the American Heart Association (AMR21-236078) and Howard D. White and Vitold Galkin from the U.S. National Institutes of Health (171261).

1. Preparing the system
NOTE: The following protocol describes how to prepare grids of a single sample. Usually, a minimum of 2 replicate grids are prepared for each sample or condition. For faster plunge speeds (less than ~ 20 ms time delay), 3 or 4 replicate grids are typically prepared to account for a reduced number of thin ice areas.
<ol>
	<li>Dilute the protein sample to the target concentration in the desired buffer. Typically, final concentrations &#8805; 2 mg/mL work well for grid p...

<ol>
	<li>Murphy, B. J., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Rotary+substates+of+mitochondrial+ATP+synthase+reveal+the+basis+of+flexible+F1-Fo+coupling.">Rotary substates of mitochondrial ATP synthase reveal the basis of flexible F1-Fo coupling.</a> Science. 364, (2019).</li><li>Benton, D. J., Gamblin, S. J., Rosenthal, P. B., Skehel, J. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Structural+transitions+in+influenza+haemagglutinin+at+membrane+fusion+pH.">Structural transitions in influenza haemagglutinin at membrane fusion pH.</a> Nature. , 1-4 (2020).</li><li>Dance, A. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Molecular+motion+on+ice.">Molecular motion on ice.</a> Nature Methods. , 1-5 (2020).</li><li>D'Imprima, E., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Protein+denaturation+at+the+air-water+interface+and+how+to+prevent+it.">Protein denaturation at the air-water interface and how to prevent it.</a> Elife. 8, 42747 (2019).</li><li>Noble, A. J., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Reducing+effects+of+particle+adsorption+to+the+air-water+interface+in+cryo-EM.">Reducing effects of particle adsorption to the air-water interface in cryo-EM.</a> Nature Methods. 15, 793-795 (2018).</li><li>Klebl, D. P., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Need+for+speed:+Examining+protein+behaviour+during+cryoEM+grid+preparation+at+different+timescales.">Need for speed: Examining protein behaviour during cryoEM grid preparation at different timescales.</a> BioRxiv. , (2020).</li><li>Ravelli, R. B., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Cryo-EM+structures+from+sub-nl+volumes+using+pin-printing+and+jet+vitrification.">Cryo-EM structures from sub-nl volumes using pin-printing and jet vitrification.</a> Nature Communications. 11, 1-9 (2020).</li><li>Arnold, S. A., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Blotting-free+and+lossless+cryo-electron+microscopy+grid+preparation+from+nanoliter-sized+protein+samples+and+single-cell+extracts.">Blotting-free and lossless cryo-electron microscopy grid preparation from nanoliter-sized protein samples and single-cell extracts.</a> Journal of Structural Biology. 197, 220-226 (2017).</li><li>Razinkov, I., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+new+method+for+vitrifying+samples+for+cryoEM.">A new method for vitrifying samples for cryoEM.</a> Journal of Structural Biology. 195, 190-198 (2016).</li><li>Feng, X., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+fast+and+effective+microfluidic+spraying-plunging+method+for+high-resolution+single-particle+cryo-EM.">A fast and effective microfluidic spraying-plunging method for high-resolution single-particle cryo-EM.</a> Structure. 25, 663-670 (2017).</li><li>Ashtiani, D., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Delivery+of+femtolitre+droplets+using+surface+acoustic+wave+based+atomisation+for+cryo-EM+grid+preparation.">Delivery of femtolitre droplets using surface acoustic wave based atomisation for cryo-EM grid preparation.</a> Journal of Structural Biology. 203, 94-101 (2018).</li><li>Rubinstein, J. L., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Shake-it-off:+a+simple+ultrasonic+cryo-EM+specimen-preparation+device.">Shake-it-off: a simple ultrasonic cryo-EM specimen-preparation device.</a> Acta Crystallographica Section D: Structural Biology. 75, (2019).</li><li>M&#228;eots, M. -. E., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Modular+microfluidics+enables+kinetic+insight+from+time-resolved+cryo-EM.">Modular microfluidics enables kinetic insight from time-resolved cryo-EM.</a> Nature Communications. 11, 1-14 (2020).</li><li>Kontziampasis, D., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+cryo-EM+grid+preparation+device+for+time-resolved+structural+studies.">A cryo-EM grid preparation device for time-resolved structural studies.</a> IUCrJ. 6, (2019).</li><li>Klebl, D. P., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Sample+deposition+onto+cryo-EM+grids:+from+sprays+to+jets+and+back.">Sample deposition onto cryo-EM grids: from sprays to jets and back.</a> Acta Crystallographica Section D: Structural Biology. 76, (2020).</li><li>White, H., Thirumurugan, K., Walker, M., Trinick, J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+second+generation+apparatus+for+time-resolved+electron+cryo-microscopy+using+stepper+motors+and+electrospray.">A second generation apparatus for time-resolved electron cryo-microscopy using stepper motors and electrospray.</a> Journal of Structural Biology. 144, 246-252 (2003).</li><li>Kaledhonkar, S., Fu, Z., White, H., Frank, J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=.">.</a> Protein Complex Assembly. , 59-71 (2018).</li><li>Trebbin, M., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Microfluidic+liquid+jet+system+with+compatibility+for+atmospheric+and+high-vacuum+conditions.">Microfluidic liquid jet system with compatibility for atmospheric and high-vacuum conditions.</a> Lab on a Chip. 14, 1733-1745 (2014).</li><li>Klebl, D. P., Sobott, F., White, H. D., Muench, S. P. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=On-grid+and+in-flow+mixing+for+time-resolved+Cryo-EM.">On-grid and in-flow mixing for time-resolved Cryo-EM.</a> Acta Crystallographica Section D: Structural Biology. , (2021).</li><li>He, S., Scheres, S. H. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Helical+reconstruction+in+RELION.">Helical reconstruction in RELION.</a> Journal of Structural Biology. 198, 163-176 (2017).</li><li>Millar, N. C., Geeves, M. A. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=The+limiting+rate+of+the+ATP-mediated+dissociation+of+actin+from+rabbit+skeletal+muscle+myosin+subfragment+1.">The limiting rate of the ATP-mediated dissociation of actin from rabbit skeletal muscle myosin subfragment 1.</a> FEBS Letters. 160, 141-148 (1983).</li><li>Kasas, S., Dumas, G., Dietler, G., Catsicas, S., Adrian, M. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Vitrification+of+cryoelectron+microscopy+specimens+revealed+by+high-speed+photographic+imaging.">Vitrification of cryoelectron microscopy specimens revealed by high-speed photographic imaging.</a> Journal of Microscopy. 211, 48-53 (2003).</li><li>Glaeser, R. M., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Defocus-dependent+Thon-ring+fading.">Defocus-dependent Thon-ring fading.</a> bioRxiv. , (2020).</li><li>Bagshaw, C. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+beginner's+guide+to+flow+kinetics.">A beginner's guide to flow kinetics.</a> The Biochemist. 42, (2020).</li></ol>

The protocols in this work can be used for fast grid preparation by direct spraying and TrEM experiments. Fast grid preparation can be used to reduce particle interactions with the air water interface5. The main limitations are the available sample concentration and ice thickness on the grid. Within these limits and provided that the sample quality is good, the protocol produces grids suitable for high resolution cryo-EM.
Troubleshooting 
Liquid fl...

Background 
Recent developments in cryo-electron microscopy (cryo-EM) have enabled structural studies of increasingly complex systems at high resolution. With few exceptions, such studies have been limited to biological macromolecules at equilibrium1 or relatively slow reactions2. Many processes in vivo occur on a faster timescale (milliseconds) and there is increasing interest in time-resolved cryo-EM (TrEM) on these timescales3. However, conventional cryo-EM sample preparation by the blotting method is too slow for millisecond TrEM.
The blotting method has other limitations besides poor time resolution. Proteins and protein complexes can suffer from denaturation or preferred orientation on grids4. Reducing the exposure time to the air-water interface during sample preparation has been shown to mitigate preferred orientation and protein denaturation5,6. Thus, fast grid preparation not only enables millisecond TrEM but can also improve grid quality.
Currently, there are three different approaches to automated grid preparation. The first approach uses a pin or capillary that holds a small amount of sample. After establishing contact between the liquid and the grid surface, the sample is &#39;written&#39; onto the grid7,8. The sample application process is relatively slow and takes a few seconds. An alternative approach uses controlled droplet generation by a piezo dispenser and self-wicking grids9. This allows faster dispense to freeze times, but is still limited by droplet and wicking speed (currently reaching 54 ms). The fastest approach so far is the direct spray approach, in which the sample is atomized in a spray nozzle and the small (~ 10 - 20 &#181;m) and fast (&#62; 5 m/s) droplets spread upon contact with the cryo-EM grid. The sample spray can be generated through different ways such as airblast atomizers, surface acoustic waves or ultrasonic humidifiers10,11,12,13. In our experience, the ice thickness with the direct spraying approach is greater but direct spraying enables dispense to freeze times &#60; 10 ms.
This protocol describes step-by-step how a time-resolved EM device (TED) equipped with a microfluidic spray nozzle can be used to prepare grids on a fast timescale14,15. The device has been used to prepare grids with a minimum delay time of 6 ms between sample application and freezing and to rapidly mix and freeze two samples. The design of the TED is based on a previous version16 and is similar to other spray-based time-resolved cryo-EM devices17.
First, the four main parts of the TED setup are described. The core of the TED is the liquid handling unit, which is responsible for sample aspiration and dispensing. A pneumatic plunger moves the grid through the spray into the liquid ethane. Generation of the spray is achieved with microfluidic spray nozzles and freezing is done in a liquid ethane container, which are described briefly. Lastly, the additional features to control the grid environment, especially humidity, are highlighted. This is followed by detailed protocols for the operation of the device and for conducting TrEM experiments. Representative results are given for fast grid preparation and a simple TrEM experiment.
Experimental Setup
The liquid handling unit 
The liquid handling system of the TED is formed by three syringe drive pumps (&#39;pumps 1 - 3&#39;), each equipped with a rotary valve (Figure 1). A power supply provides pumps 1 - 3 with 24 V DC. Communication with the control software (written in Visual Basic and C++) is via a RS232 interface to pump 1. Commands are distributed through the serial I/O expansion ports from pump 1 to pumps 2-3. Pumps 1-3 are equipped with glass syringes (&#39;syringes 1-3&#39;, we use 250 &#181;L/zero dead volume syringes here). Each valve has two positions, &#39;load&#39; and &#39;dispense&#39;. The &#39;load&#39; position is used to aspirate sample into the syringe. A short piece (~ 3 - 4 cm) of 1/16&#34; O.D., 0.01&#8242;&#8242; I.D. FEP tubing is connected via ETFE/ETFE flangeless fittings to the &#39;load&#39; position of valves 1-3. This short piece of tubing reaches into the sample reservoir (typically a 1.5 mL or 0.5 mL plastic tube). The &#39;dispense&#39; position leads to the spray nozzle. Connection between the &#39;dispense&#39; outlet and the spray nozzle is made by PE tubing (~ 20-30 cm length, 0.043&#34; O.D., 0.015&#34; I.D.), with a short piece of sleeve tubing (~ 0.5 cm) and ETFE/ETFE flangeless fittings.
The pneumatic plunger 
The TED uses a pneumatic plunger to accelerate the grid and move it through the sample spray into the liquid ethane container. Negative pressure tweezers hold the grid, screwed into a home-built holder which is mounted to a dual rod pneumatic cylinder (Figure 2A).
Pressure is supplied from a large nitrogen gas cylinder (size W), equipped with a multistage regulator (0 - 10 bar, &#39;main pressure&#39;). Flexible reinforced PVC tubing (12 mm O.D.) connects the regulator to a 12-port manifold where pressurized nitrogen is delivered to the nozzle and the pneumatic plunger. Gas flow through the nozzle is constant, regulated directly at the nitrogen cylinder (main pressure). The connection to the nozzle is made with PU tubing (4 mm O.D., 2.5 mm I.D.), a short piece of PE tubing (~ 8 cm length, 0.043&#34; O.D., 0.015&#34; I.D.) and appropriate connectors. Pressure on the pneumatic plunger is controlled through a solenoid valve. PU tubing (4 mm O.D., 2.5 mm I.D.) connects the solenoid valve with a regulator and the pneumatic plunger, to allow a reduced plunge pressure (&#8804; main pressure). The solenoid valve is computer controlled. A schematic overview of the setup is given in Figure 2B.
Note that with this setup the plunge pressure is always equal or smaller than the spray gas pressure (main pressure). However, the setup can easily be changed by incorporating a second regulator upstream of the spray nozzle to allow higher plunge speeds at low spray gas pressure. High pressures (&#62;&#62; 2 bar) can damage the PDMS spray nozzle.
CAUTION: This is a pressurized system and the &#39;main pressure&#39; should always be &#60; 7 bar.
Pressures between 0.5 and 2 bar are typically used for the pneumatic plunger and show an approximately linear relation between pressure and speed (at the vertical position of the spray). Plunge speeds are measured with an oscilloscope, connected in line with a slide potentiometer (10 k&#937;) and in parallel with a 2 k&#937; resistor (Figure 2C). A power supply provides the potentiometer with 9 V DC. While the approximate plunge speed is set prior to the experiment by setting the plunge pressure, the potentiometer gives a precise readout of the speed after the experiment.
Spray nozzles and liquid ethane container 
The fabrication and operation of gas-dynamic virtual nozzles for spray-based sample delivery has been described elsewhere in detail15. As described above, the &#39;dispense&#39; outlets of valves 1-3 are connected to the liquid inlets of the nozzle (Figure 3A). The pressurized spray gas is connected to the gas inlet of the nozzle. The inlets in the PDMS spray nozzles are such that 0.043&#34; O.D. PE tubing can be used directly without the need for fittings. Our nozzle design contains a &#39;jet-in-jet&#39; geometry for mixing of two samples, similar to the device described in ref.18. A schematic of the design is shown in Figure 3B, a microscopic image of a nozzle is shown in Figure 3C. The layout of the microfluidic device requires the use of three syringes to mix two samples. The spray nozzle is typically positioned at 1-1.5 cm distance from the grid (during sample application).
We use liquid ethane as a cryogen, in a liquid ethane/nitrogen container as used for the standard blotting method. Vertical positioning of the liquid ethane cup is achieved with a laboratory lifting platform.
Control of the spray and grid environment 
The plunger and spray nozzle are contained within a custom built PMMA (acrylic glass) box with a double door (Figure 4A). High relative humidity inside the box is achieved by an air-humidification system at the back of the TED (Figure 4B). Air is supplied by a pump and fed into a first 10&#34; canister (typically used for under sink water purification). The canister is filled with a low (~ 5-10 cm) level of water and also houses a humidifier unit. Mains power to the humidifier is controlled by a digital humidity/temperature controller and a humidity/temperature sensor located inside the acrylic glass box. The controller is set to turn off the pump when the relative humidity reaches &#8805; 90 %. Humidified air from the first canister is pumped through a diffuser, immersed in water in a second 10&#34; canister and then enters the acrylic glass box.
CAUTION: Because the sample is aerosolized in the spray nozzle, hazardous biological or chemical specimen are not suitable as samples.
The run sequence 
The Run Script button in the control software initiates the run sequence. This sequence of commands can be pre-defined in a script file and altered through the software. The most important variables are explained here:
Spray speed: The spray speed determines the liquid flowrate used by the syringe pump. The flowrate can be calculated as follows: The syringe pump motors used here have a fixed step size. The full range of the pump is divided into 48,000 steps. The second important factor is the syringe volume. We typically use 250 &#181;L syringes. The spray speed in the control software is set as number of steps/second. A spray speed of 1000 steps/second corresponds to:
<img alt="Equation 1" src="/files/ftp_upload/62199/62199eq01.jpg" />
Spray volume: The spray volume determines the total volume to be sprayed. Thus, it also determines the duration of the spray. The spray volume in the control software is set as a number of steps. A spray volume of 2000 steps, at a spray speed of 1000 steps/second, leads to a spray duration of 2 s and a total volume of 10.4 &#181;L.
Pre-spray time: This variable defines the time between initiation of the spray and plunge. It is important to choose the delay time such that the spray has sufficient time to stabilize before plunging the grid. Usually, the spray is given 1.5 - 4 s to stabilize before the grid is plunged. The spray is maintained until the grid has moved through. Usually, the liquid flow (and therefore the spray) is stopped 0.5 to 1 s after the grid has been plunged. Using a spray speed of 1000 steps/s and a spray volume of 2000 steps, a typical pre-spray time is 1.5 s, for example.
An exemplary sequence of commands is shown in Figure 5A, the grid position over time is illustrated in Figure 5B.

<table border="1" fo:keep-together.within-page="1" fo:keep-with-next.within-page="always">
	<tbody>
		<tr>
			<td>Time resolved device</td>
			<td></td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>acrylic glass box</td>
			<td>USA scientific</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>digital humidity/temperature controller</td>
			<td>THE20 digital humidity/temperature controller</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>dual rod pneumatic cylinder</td>
			<td>dual rod pneumatic cylinder TN 10x70</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>FEP tubing</td>
			<td>Upchurch Scientific 1/16&#8221; O.D., 0.01&#39;&#39; I.D. FEP tubing</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>flangeless fittings</td>
			<td>Upchurch Scientific ETFE/ETFE flangeless fittings</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>flexible reinforced PVC tubing</td>
			<td>12 mm OD. flexible reinforced PVC tubing</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>glass syringes</td>
			<td>Kloehn 250 &#181;L zero-dead volume</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>humidifier pump</td>
			<td>Interpret Aqua Air AP3</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>liquid ethane container</td>
			<td>from Thermo/FEI VitrobotTM Mark IV</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>multistage regulator</td>
			<td>GASARC class 3 multistage regulator</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>negative pressure tweezers</td>
			<td>Dumont N5 Inox B negative pressure tweezers</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>oscilloscope</td>
			<td>Hantek 6022BE oscilloscope</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>PE tubing</td>
			<td>Scientific Commodities Inc. 0.043&#8221; O.D., 0.015&#8221; I.D. PE tubing</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>power supply</td>
			<td>Mean Well GSM160A24-R7B</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>power supply</td>
			<td>Wanptek KPS305D power supply</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>PU tubing</td>
			<td>SMC TU0425 4 mm O.D., 2.5 mm I.D. PU tubing</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>regulator</td>
			<td>Norgren R72G-2GK-RMN</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>slide potentiometer</td>
			<td>PS100 slide potentiometer</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>solenoid valve</td>
			<td>SMC NVJ314M solenoid valve</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>syringe drive pumps</td>
			<td>Kloehn V6 48K model</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>Reagents &#38; Materials</td>
			<td></td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>apoferritin from equine spleen</td>
			<td>Sigma-Aldrich, A3660</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>ATP</td>
			<td>Sigma-Aldrich, A2383</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>cryo-EM grids</td>
			<td>Quantifoil 300 mesh Cu, R 1.2/1.3</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>EGTA</td>
			<td>Sigma Aldrich E3889</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>F-actin</td>
			<td>Provided by H.D. White (for preparation procedure, see ref. 1)</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>glow-discharger</td>
			<td>Cressington 208 carbon coater with a glow-discharge unit</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>HEPES</td>
			<td>Sigma-Aldrich, H7006</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>KAc</td>
			<td>Sigma-Aldrich, P1190</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>MgCl2</td>
			<td>Sigma-Aldrich, M8266</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>MOPS</td>
			<td>Sigma-Aldrich, M1254</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>NaCl</td>
			<td>Sigma-Aldrich, S9888</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>Skeletal muscle myosin S1</td>
			<td>Provided by H.D. White (for preparation procedure, see ref. 2)</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>Ref 1</td>
			<td>Spudich, J. A. &#38; Watt, S. The regulation of rabbit skeletal muscle contraction I. Biochemical studies of the interaction of the tropomyosin-troponin complex with actin and the proteolytic fragments of myosin. Journal of biological chemistry 246, 4866-4871 (1971).</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>Ref 2</td>
			<td>White, H. &#38; Taylor, E. Energetics and mechanism of actomyosin adenosine triphosphatase. Biochemistry 15, 5818-5826 (1976).</td>
			<td></td>
			<td></td>
		</tr>
	</tbody>
</table>

fast grid preparation for time-resolved cryo-electron microscopy

The field of cryo-electron microscopy (cryo-EM) is rapidly developing with new hardware and processing algorithms, producing higher resolution structures and information on more challenging systems. Sample preparation for cryo-EM is undergoing a similar revolution with new approaches being developed to supersede the traditional blotting systems. These include the use of piezo-electric dispensers, pin printing and direct spraying. As a result of these developments, the speed of grid preparation is going from seconds to milliseconds, providing new opportunities, especially in the field of time-resolved cryo-EM where proteins and substrates can be rapidly mixed before plunge freezing, trapping short lived intermediate states. Here we describe, in detail, a standard protocol for making grids on our in-house time-resolved EM device both for standard fast grid preparation and also for time-resolved experiments. The protocol requires a minimum of about 50 &#181;L sample at concentrations of &#8805; 2 mg/mL for the preparation of 4 grids. The delay between sample application and freezing can be as low as 10 ms. One limitation is increased ice thickness at faster speeds and compared to the blotting method. We hope this protocol will aid others in designing their own grid making devices and those interested in designing time-resolved experiments.

Fast grid preparation with the TED 
As a test specimen for fast grid preparation, we have used apoferritin from equine spleen at 20 &#181;M in 30 mM HEPES, 150 mM NaCl, pH 7.5. A reconstruction at 3.5 &#197; resolution was obtained from 690 micrographs as described in ref.15 (Figure 7A). The defocus range was chosen so that particles can easily be identified in the raw images (Figure 7B). A typical grid prepared with...

Watch this Scientific Journal Video about Fast Grid Preparation for Time-Resolved Cryo-Electron Microscopy at JoVE.com

Fast Grid Preparation for Time-Resolved Cryo-Electron Microscopy

Here, we provide a detailed protocol for the use of a rapid grid making device for both fast grid-making and for rapid mixing and freezing to conduct time-resolved experiments.

The field of cryo-electron microscopy (cryo-EM) is rapidly developing with new hardware and processing algorithms, producing higher resolution structures ...

Hello, and welcome to this JoVE"video. We want to introduce you to the setup that we've got here for rapid grid making, a time-resolved study that we're developing over in Leeds. Be aware this isn't a standard system, but we hope that by giving you a detailed account of all the things and the parameters that we do, you'll be able to develop similar systems in your own laboratories.A detailed description of the device is given in the Richmond protocol. Here, we're going to give a step-by-step guide for fast grid preparation and time-resolved EM.In our experience, protein concentration should be two milligrams per milliliter or higher. The protocol requires a minimum volume of about 50 microliters.Turn on the device. Then turn on the control PC and start the control software. Initialize all syringe pumps by pressing the initialize button on each syringe pump.Turn on the potentiometer power supply, set it to nine volts, and start the oscilloscope control software. Pressurized nitrogen gas is needed to generate the spray. Open the nitrogen cylinder and set the pressure to 2 bar.Ensure all syringe pump valves are in load position. To do this, switch all valves to dispense in the control software and then back to load. Set all syringes to zero.Any air bubbles present in the system should be removed at this stage. To do this the syringes may have to be unscrewed, bubbles removed manually, and the syringes mounted again when containing no more bubbles. The liquid handling system is usually stored in water.Before loading the sample, the system is equilibrated with buffer. This is done by washing the tubing with an excess of buffer. Place a tube containing at least 200 microliters of buffer onto syringe one.The top of the tube must be pierced to attach it. Aspirate a suitable amount of buffer, between 50 and a hundred microliters with syringe one using the control software. Switch valve one to dispense.Dispense all of the liquid in syringe one. Return valve one to the load position, and press the initialize button on syringe one to prepare the system for the next wash cycle. These steps are usually repeated three times to ensure thorough washing of the tubing.Next, the spray nozzle is positioned. Place an EM grid in the plunging arm. Position the grid in front of the spray nozzle.Dispense buffer using the control software. If nozzle and grid are aligned, liquid should accumulate after spraying for an extended period of time. If necessary, adjust the nozzle position and then check again where the liquid accumulates on the grid.Next, adjust the position of the ethane cup. The tip of the tweezers should reach approximately to the center of the ethane cup. Perform a test run to ensure all settings are correct.Close the humidity chamber. Make sure the path of the plunger is clear. Aspirate the volume of buffer required for a single run into syringe one.Switch valve one to dispense. Start the run by pressing run'in the control software. Check that syringe pump one is moving, two seconds in this case, and the grid is plunged after an appropriate delay, 1.5 seconds here.When the run is finished, set the pressure on the plunger arm to the desired value. Press OK'in the control software to release the pressure from the plunging arm. Now the ethane cup is cool and filled with liquid ethane.Glow-discharge the grids before use. A typical glow-discharge is 90 seconds at 10 milliamps in 0.1 millibar air. The tubing is then equilibrated with sample.If the available sample volume is low, the tubing may be equilibrated with only one dead-volume. Aspirate sample. Typically the dead volume is around 30 microliters.Switch valve one to dispense. Dispense the sample through tubing and nozzle. Then aspirate the amount of sample required for a single run.Switch valve one to dispense. Check that the relative humidity has reached the desired value. We typically prepare grids at 60%or higher.This can take a few minutes. Place the tweezers holding a glow-discharged grid in the plunging arm. Place the potentiometer slide in the start position, ready for speed measurement.Set the trigger for the speed measurement in the oscilloscope software. Place the liquid ethane cup, and close to humidity chamber. Make sure the path of the plunger is clear.Start the run in the control software. When the run is finished, press OK'in the control software to release pressure from the plunging arm. Open the humidity chamber, loosen the connection between plunging arm and tweezers.Move up the plunging arm while keeping the grid in liquid ethane. Then transfer the grids to liquid nitrogen and into storage. Save the oscilloscope measurement.Manually reset the position of the potentiometer slider and plunger. Repeat the protocol to prepare replicate grids. Time-resolved experiments are done in a similar way.Higher stock concentrations are needed for time-resolved experiments because of dilution in the mixing step. For a time-resolved experiment, use all three syringes. Tubing is attached to the syringe pumps and to the spray nozzle.The microfluidic spray nozzle used here also contains a mixing element. Note that longer tubes will give a larger dead-volume and washing equilibration steps require more buffer and sample. Equilibrate all syringes with buffer and sample separately.Typically, syringe one is used for sample A'and syringes two and three are used for sample B'After the tubing is equilibrated, load sample A into syringe one and sample B into syringes two and three. Then, switch valves one to three to dispense. Start the run in the control software.Note that a different run script is needed for a time-resolved experiment. Different time delays can be achieved in two ways. By adjusting the plunger speed, the time delay from mixing to freezing can be changed.A faster plunge speed will lead to a shorter time delay. Alternatively, the spray ethane distance is changed by adjusting the vertical position of the spray nozzle. Increasing the distance will result in a longer time delay.In the electron microscope at low magnification, a typical grid looks like this. Areas of thin ice, as indicated, are suitable for data acquisition. At higher magnifications, particles should be clearly visible.With a test specimen such as apoferritin, a relatively small data set from a single grid is sufficient for a reconstruction at three to four angstrom resolution. For time-resolved experiments, we collect data sets from different time points or grids. It's useful to combine the data for 3D classification and then trace particles back to their time points.This way the data can provide structural information and information on the reaction kinetics. In conclusion, we hope you enjoyed the video. We hope that with the detailed descriptions in the JoVE paper along with the video, you'll be able to conduct your own experiments via rapid grid making, which has been shown to alleviate some of the problems from mutation or to help with interactions at the air-water interface, all you need for conducting your own time-resolved studies to try and trap some of those non equilibrium states.So, happy grid making.

fast-grid-preparation-for-time-resolved-cryo-electron-microscopy

Research

JoVE Journal

Biochemistry

Time-resolved ElectroSpray Ionization Hydrogen-deuterium Exchange Mass Spectrometry for Studying Protein Structure and Dynamics

Intrinsically disordered proteins (IDPs) have long been a challenge to structural biologists due to their lack of stable secondary structure elements. Hydrogen-Deuterium Exchange (HDX) measured at rapid time scales is uniquely suited to detect structures and hydrogen bonding networks that are briefly populated, allowing for the characterization of transient conformers in native ensembles. Coupling of HDX to mass spectrometry offers several key advantages, including high sensitivity, low sample consumption and no restriction on protein size. This technique has advanced greatly in the last several decades, including the ability to monitor HDX labeling times on the millisecond time scale. In addition, by incorporating the HDX workflow onto a microfluidic platform housing an acidic protease microreactor, we are able to localize dynamic properties at the peptide level. In this study, Time-Resolved ElectroSpray Ionization Mass Spectrometry (TRESI-MS) coupled to HDX was used to provide a detailed picture of residual structure in the tau protein, as well as the conformational shifts induced upon hyperphosphorylation.

Conformational flexibility plays a critical role in protein function. Herein, we describe the use of time-resolved electrospray ionization mass spectrometry coupled to hydrogen-deuterium exchange for probing the rapid structural changes that drive function in ordered and disordered proteins.

Intrinsically disordered proteins (IDPs) have long been a challenge to structural biologists due to their lack of stable secondary structure elements. ...

Expression and Purification of the Human Lipid-sensitive Cation Channel TRPC3 for Structural Determination by Single-particle Cryo-electron Microscopy

Transient receptor potential channels (TRPCs) of the canonical TRP subfamily are nonselective cation channels that play an essential role in calcium homeostasis, particularly store-operated calcium entry, which is critical to maintaining proper function of synaptic vesicle release and intracellular signaling pathways. Accordingly, TRPC channels have been implicated in a variety of human diseases including cardiovascular disorders such as cardiac hypertrophy, neurodegenerative disorders such as Parkinson&#39;s disease, and neurologic disorders such as spinocerebellar ataxia. Therefore, TRPC channels represent a potential pharmacologic target in human diseases. However, the molecular mechanisms of gating in these channels are still unclear. The difficulty in obtaining large quantities of stable, homogeneous, and purified protein has been a limiting factor in structure determination studies, particularly for mammalian membrane proteins such as the TRPC ion channels. Here, we present a protocol for the large-scale expression of mammalian ion channel membrane proteins using a modified baculovirus gene transfer system and the purification of these proteins by affinity and size-exclusion chromatography. We further present a protocol to collect single-particle cryo-electron microscopy images from purified protein and to use these images to determine the protein structure. Structure determination is a powerful method for understanding the mechanisms of gating and function in ion channels.

This protocol describes techniques used to determine ion channel structures by cryo-electron microscopy, including a baculovirus system used to efficiently express genes in mammalian cells with minimum effort and toxicity, protein extraction, purification, and quality checking, sample grid preparation and screening, as well as data collection and processing.

Transient receptor potential channels (TRPCs) of the canonical TRP subfamily are nonselective cation channels that play an essential role in calcium ...

Preparation and Cryo-FIB micromachining of Saccharomyces cerevisiae for Cryo-Electron Tomography

Today, cryo-electron tomography (cryo-ET) is the only technique that can provide near-atomic resolution structural data on macromolecular complexes in situ. Owing to the strong interaction of an electron with the matter, high-resolution cryo-ET studies are limited to specimens with a thickness of less than 200 nm, which restricts the applicability of cryo-ET only to the peripheral regions of a cell. A complex workflow that comprises the preparation of thin cellular cross-sections by cryo-focused ion beam micromachining (cryo-FIBM) was introduced during the last decade to enable the acquisition of cryo-ET data from the interior of larger cells. We present a protocol for the preparation of cellular lamellae from a sample vitrified by plunge freezing utilizing Saccharomyces cerevisiae as a prototypical example of a eukaryotic cell with wide utilization in cellular and molecular biology research. We describe protocols for vitrification of S. cerevisiae into isolated patches of a few cells or a continuous monolayer of the cells on a TEM grid and provide a protocol for lamella preparation by cryo-FIB for these two samples.

Preparation and Cryo-FIB micromachining of Saccharomyces cerevisiae for Cryo-Electron Tomography

We present a protocol for lamella preparation of plunge frozen biological specimens by cryo-focused ion beam micromachining for high-resolution structural studies of macromolecules in situ with cryo-electron tomography. The presented protocol provides guidelines for the preparation of high-quality lamellae with high reproducibility for structural characterization of macromolecules inside the&#160;Saccharomyces cerevisiae.

Today, cryo-electron tomography (cryo-ET) is the only technique that can provide near-atomic resolution structural data on macromolecular complexes in ...

Single Particle Cryo-Electron Microscopy: From Sample to Structure

Cryo-electron microscopy (cryoEM) is a powerful technique for structure determination of macromolecular complexes, via single particle analysis (SPA). The overall process involves i) vitrifying the specimen in a thin film supported on a cryoEM grid; ii) screening the specimen to assess particle distribution and ice quality; iii) if the grid is suitable, collecting a single particle dataset for analysis; and iv) image processing to yield an EM density map. In this protocol, an overview for each of these steps is provided, with a focus on the variables which a user can modify during the workflow and the troubleshooting of common issues. With remote microscope operation becoming standard in many facilities, variations on imaging protocols to assist users in efficient operation and imaging when physical access to the microscope is limited will be described.

Structure determination of macromolecular complexes using cryoEM has become routine for certain classes of proteins and complexes. Here, this pipeline is summarized (sample preparation, screening, data acquisition and processing) and readers are directed towards further detailed resources and variables that may be altered in the case of more challenging specimens.

Cryo-electron microscopy (cryoEM) is a powerful technique for structure determination of macromolecular complexes, via single particle analysis (SPA). The ...

Micropatterning Transmission Electron Microscopy Grids to Direct Cell Positioning within Whole-Cell Cryo-Electron Tomography Workflows

Whole-cell cryo-electron tomography (cryo-ET) is a powerful technology that is used to produce nanometer-level resolution structures of macromolecules present in the cellular context and preserved in a near-native frozen-hydrated state. However, there are challenges associated with culturing and/or adhering cells onto TEM grids in a manner that is suitable for tomography while retaining the cells in their physiological state. Here, a detailed step-by-step protocol is presented on the use of micropatterning to direct and promote eukaryotic cell growth on TEM grids. During micropatterning, cell growth is directed by depositing extra-cellular matrix (ECM) proteins within specified patterns and positions on the foil of the TEM grid while the other areas remain coated with an anti-fouling layer. Flexibility in the choice of surface coating and pattern design makes micropatterning broadly applicable for a wide range of cell types. Micropatterning is useful for studies of structures within individual cells as well as more complex experimental systems such as host-pathogen interactions or differentiated multi-cellular communities. Micropatterning may also be integrated into many downstream whole-cell cryo-ET workflows, including correlative light and electron microscopy (cryo-CLEM) and focused-ion beam milling (cryo-FIB).

The goal of this protocol is to direct cell adhesion and growth to targeted areas of grids for cryo-electron microscopy. This is achieved by applying an anti-fouling layer that is ablated in user-specified patterns followed by deposition of extra-cellular matrix proteins in the patterned areas prior to cell seeding.

Whole-cell cryo-electron tomography (cryo-ET) is a powerful technology that is used to produce nanometer-level resolution structures of macromolecules ...

A Robust Single-Particle Cryo-Electron Microscopy (cryo-EM) Processing Workflow with cryoSPARC, RELION, and Scipion

Recent advances in both instrumentation and image processing software have made single-particle cryo-electron microscopy (cryo-EM) the preferred method for structural biologists to determine high-resolution structures of a wide variety of macromolecules. Multiple software suites are available to new and expert users for image processing and structure calculation, which streamline the same basic workflow: movies acquired by the microscope detectors undergo correction for beam-induced motion and contrast transfer function (CTF) estimation. Next, particle images are selected and extracted from averaged movie frames for iterative 2D and 3D classification, followed by 3D reconstruction, refinement, and validation. Because various software packages employ different algorithms and require varying levels of expertise to operate, the 3D maps they generate often differ in quality and resolution. Thus, users regularly transfer data between a variety of programs for optimal results. This paper provides a guide for users to navigate a workflow across the popular software packages: cryoSPARC v3, RELION-3, and Scipion 3 to obtain a near-atomic resolution structure of the adeno-associated virus (AAV). We first detail an image processing pipeline with cryoSPARC v3, as its efficient algorithms and easy-to-use GUI allow users to quickly arrive at a 3D map. In the next step, we use PyEM and in-house scripts to convert and transfer particle coordinates from the best quality 3D reconstruction obtained in cryoSPARC v3 to RELION-3 and Scipion 3 and recalculate 3D maps. Finally, we outline steps for further refinement and validation of the resultant structures by integrating algorithms from RELION-3 and Scipion 3. In this article, we describe how to effectively utilize three processing platforms to create a single and robust workflow applicable to a variety of data sets for high-resolution structure determination.

A Robust Single-Particle Cryo-Electron Microscopy cryo-EM Processing Workflow with cryoSPARC, RELION, and Scipion

This article describes how to effectively utilize three cryo-EM processing platforms, i.e., cryoSPARC v3, RELION-3, and Scipion 3, to create a single and robust workflow applicable to a variety of single-particle data sets for high-resolution structure determination.

Recent advances in both instrumentation and image processing software have made single-particle cryo-electron microscopy (cryo-EM) the preferred method ...

Preparation of Nucleosome Core Particles Complexed with DNA Repair Factors for Cryo-Electron Microscopy Structural Determination

DNA repair in the context of chromatin is poorly understood. Biochemical studies using nucleosome core particles, the fundamental repeating unit of chromatin, show most DNA repair enzymes remove DNA damage at reduced rates as compared to free DNA. The molecular details on how base excision repair (BER) enzymes recognize and remove DNA damage in nucleosomes have not been elucidated. However, biochemical BER data of nucleosomal substrates suggest the nucleosome presents different structural barriers dependent on the location of the DNA lesion and the enzyme. This indicates the mechanisms employed by these enzymes to remove DNA damage in free DNA may be different than those employed in nucleosomes. Given that the majority of genomic DNA is assembled into nucleosomes, structural information of these complexes is needed. To date, the scientific community lacks detailed protocols to perform technically feasible structural studies of these complexes. Here, we provide two methods to prepare a complex of two genetically fused BER enzymes (Polymerase &#946; and AP Endonuclease1) bound to a single-nucleotide gap near the entry-exit of the nucleosome for cryo-electron microscopy (cryo-EM) structural determination. Both methods of sample preparation are compatible for vitrifying quality grids via plunge freezing. This protocol can be used as a starting point to prepare other nucleosomal complexes with different BER factors, pioneer transcription factors, and chromatin-modifying enzymes.

This protocol outlines in detail the preparation of nucleosomal complexes using two methods of sample preparation for freezing TEM grids.

DNA repair in the context of chromatin is poorly understood. Biochemical studies using nucleosome core particles, the fundamental repeating unit of ...

Extracting Modified Microtubules from Mammalian Cells to Study Microtubule-Protein Complexes by Cryo-Electron Microscopy

Microtubules are an important part of the cytoskeleton and are involved in intracellular organization, cell division, and migration. Depending on the posttranslational modifications, microtubules can form complexes with various interacting proteins. These microtubule-protein complexes are often implicated in human diseases. Understanding the structure of such complexes is useful for elucidating their mechanisms of action and can be studied by cryo-electron microscopy (cryo-EM). To obtain such complexes for structural studies, it is important to extract microtubules containing or lacking specific posttranslational modifications. Here, we describe a simplified protocol to extract endogenous tubulin from genetically modified mammalian cells, involving microtubule polymerization, followed by sedimentation using ultracentrifugation. The extracted tubulin can then be used to prepare cryo-electron microscope grids with microtubules that are bound to a purified microtubule-binding protein of interest. As an example, we demonstrate the extraction of fully tyrosinated microtubules from cell lines engineered to lack the three known tubulin-detyrosinating enzymes. These microtubules are then used to make a protein complex with enzymatically inactive microtubule-associated tubulin detyrosinase on cryo-EM grids.

Here, we describe a protocol to extract endogenous tubulin from mammalian cells, which can lack or contain specific microtubule-modifying enzymes, to obtain microtubules enriched for a specific modification. We then describe how the extracted microtubules can be decorated with purified microtubule-binding proteins to prepare grids for cryo-electron microscopy.

Microtubules are an important part of the cytoskeleton and are involved in intracellular organization, cell division, and migration. Depending on the ...

Coating CryoEM Grids with Monolayer Graphene to Improve Cryo-Sample Preparation

Application of Monolayer Graphene to Cryo-Electron Microscopy Grids for High-resolution Structure Determination

In cryogenic electron microscopy (cryoEM), purified macromolecules are applied to a grid bearing a holey carbon foil; the molecules are then blotted to remove excess liquid and rapidly frozen in a roughly 20-100 nm thick layer of vitreous ice, suspended across roughly 1 &#181;m wide foil holes. The resulting sample is imaged using cryogenic transmission electron microscopy, and after image processing using suitable software, near-atomic resolution structures can be determined. Despite cryoEM&#39;s widespread adoption, sample preparation remains a severe bottleneck in cryoEM workflows, with users often encountering challenges related to samples behaving poorly in the suspended vitreous ice. Recently, methods have been developed to modify cryoEM grids with a single continuous layer of graphene, which acts as a support surface that often increases particle density in the imaged area and can reduce interactions between particles and the air-water interface. Here, we provide detailed protocols for the application of graphene to cryoEM grids and for rapidly assessing the relative hydrophilicity of the resulting grids. Additionally, we describe an EM-based method to confirm the presence of graphene by visualizing its characteristic diffraction pattern. Finally, we demonstrate the utility of these graphene supports by rapidly reconstructing a 2.7 &#197; resolution density map of a Cas9 complex using a pure sample at a relatively low concentration.

Author Spotlight: Enhancing CryoEM Sample Preparation Using Graphene Monolayer on Microscopy Grids 

The application of support layers to cryogenic electron microscopy (cryoEM) grids can increase particle density, limit interactions with the air-water interface, reduce beam-induced motion, and improve the distribution of particle orientations. This paper describes a robust protocol for coating cryoEM grids with a monolayer of graphene for improved cryo-sample preparation.

In cryogenic electron microscopy (cryoEM), purified macromolecules are applied to a grid bearing a holey carbon foil; the molecules are then blotted to ...

Accelerating Macromolecular Structural Analysis Using Smart Leginon Autoscreen

Cryo-Electron Microscopy Screening Automation Across Multiple Grids Using Smart Leginon

Advancements in cryo-electron microscopy (cryoEM) techniques over the past decade have allowed structural biologists to routinely resolve macromolecular protein complexes to near-atomic resolution. The general workflow of the entire cryoEM pipeline involves iterating between sample preparation, cryoEM grid preparation, and sample/grid screening before moving on to high-resolution data collection. Iterating between sample/grid preparation and screening is typically a major bottleneck for researchers, as every iterative experiment must optimize for sample concentration, buffer conditions, grid material, grid hole size, ice thickness, and protein particle behavior in the ice, amongst other variables. Furthermore, once these variables are satisfactorily determined, grids prepared under identical conditions vary widely in whether they are ready for data collection, so additional screening sessions prior to selecting optimal grids for high-resolution data collection are recommended. This sample/grid preparation and screening process often consumes several dozen grids and days of operator time at the microscope. Furthermore, the screening process is limited to operator/microscope availability and microscope accessibility. Here, we demonstrate how to use Leginon and Smart Leginon Autoscreen to automate the majority of cryoEM grid screening. Autoscreen combines machine learning, computer vision algorithms, and microscope-handling algorithms to remove the need for constant manual operator input. Autoscreen can autonomously load and image grids with multi-scale imaging using an automated specimen-exchange cassette system, resulting in unattended grid screening for an entire cassette. As a result, operator time for screening 12 grids may be reduced to ~10 min with Autoscreen compared to ~6 h using previous methods which are hampered by their inability to account for high variability between grids. This protocol first introduces basic Leginon setup and functionality, then demonstrates Autoscreen functionality step-by-step from the creation of a template session to the end of a 12-grid automated screening session.

Author Spotlight: Enhancing Cryo-Electron Microscopy by Automated Data Collection and Analysis Techniques

Cryo-electron microscopy (cryoEM) multi-grid screening is often a tedious process that demands hours of attention. This protocol shows how to set up a standard Leginon collection and Smart Leginon Autoscreen to automate this process. This protocol can be applied to the majority of cryoEM holey foil grids.

Advancements in cryo-electron microscopy (cryoEM) techniques over the past decade have allowed structural biologists to routinely resolve macromolecular ...