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Jan 1, 2024¡Microscopy Today
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Bob Price, Bev Maleeff

Dear colleagues, we have a Cressington 108 carbon coater that uses carbon rods. After shaping the rods, I use sandpaper to make a flat surface and I wipe the powder away from the surface with a cloth. We use the maximal distance, approximately 10 cm, 4 volts and 10 seconds (we repeat 6-8 times with 1 minute pause in-between). Sometimes, there are sparks coming from the shaped rod and I don't know what I can do to avoid them. Quite frankly, this doesn't seem to affect the quality of the coating but still I wonder (1) why they appear (2) how they can affect my sample and (3) how to avoid them. Any thoughts? Stephane Nizet [email protected] If you have a shutter and the sparks are coming in the beginning or at a specific time: use it. Maybe a longer burn time and a shutter will do the trick. Stefan Diller [email protected] I suspect that it has something to do with the structure of the rod and the bonds between particles. I have come to expect them and to live with them. As you say, they don't seem to affect the bulk of the coating. I do try to limit the number of sparks. I control the current/voltage to allow a few per second. If there are none, it seems that the coating rate is very low. If the rate gets too high, the rod often fails too quickly. Warren Straszheim [email protected] You can try rinsing the rod with EtOH and then air gas blow-drying before use. Also, you can try a light burn (rod fire-red) for a few seconds before increasing the current. I don't believe the sparks will ruin your coating. Mike Delannoy [email protected] The sparks are basically glowing chunks of carbon coming from the arc. My experience is that the higher the current the more chunks are present. Generally, the chunks don't significantly affect the final product. So, like Mike Delannoy, I would set the current so occasional “sparks” are present as the optimum for deposition. You don't want a spray of sparks like a fireworks sparkler. Henk Colijn [email protected] I usually find it is because there is loose carbon on the tip. We use a folded paper towel. When the end of the flat carbon is scraped across an emory paper to remove embers from the last coating, it is always wiped on the paper towel. If we use a rod we have sharpened to a point, again we wipe off any loose carbon on the paper towel. Elaine Humphrey [email protected] You may need to shape the carbon rod with a carbon rod shaper for sharpening the 6.5 mm carbon rods into 3.5/3 mm cylindrical tips and 1.75/1.50 mm (3 diameters). It is important that the carbon rod has a reduced diameter at the tip. It is best to increase the voltage to 0.5 V. Abdelyamine Naitbouda [email protected] Dear EM Experts, some of my crystallographer colleagues and I wonder about the fundamentally different appearance of density histograms in EM Coulomb potential maps versus X-ray electron density maps. Here is the question: What I've noticed is that they are on different scales. That is understandable, as e/A3 is different than V. But there are papers showing that these values are somewhat proportional to each other for lower resolutions. But the other thing that I have noticed is that electron density maps have close to normally distributed value distributions, whereas cryoEM maps have a sharp spike and a very long tail. As a result, an electron density blob in an X-ray map looks nice somewhere around 3 sigma, whereas for cryoEM it's sometimes 10 sigma, 17 sigma, 20 sigma, all over the place. I'm thinking of using thresholds based on percentiles rather than sigmas, but my main question is: shouldn't the values on cryoEM maps also be approximately normally distributed? What is the cause of this non-normality? Sharpening? The raw experimental data themselves? Here is a potential partial answer: In cryo-EM, there is no absolute scaling, which means that density values can vary significantly. This variability can explain why different sigma values are consistently encountered. I can confirm that the density value distribution behaves as described, and I have also observed this. However, I cannot provide a definitive answer as to why this occurs. My best guess is that it may be related to B factor weighting in motion correction, but I cannot provide a conclusive explanation. What are we missing here? Ben Rupp [email protected] According to PDB/EMDB validation reports, this spike in the voxel value histogram is caused by masking. One validation report I have says: “A spike in this graph at zero usually indicates that the volume has been masked”. You can probably also find this note in validation reports of released PDB/EMDB entries. Opening a map from 3D refinement and one of the two half-maps from the same job seems to confirm this. The map’s histogram shows this spike at zero, but the half-map’s histogram doesn’t. Half-maps are never filtered nor masked, whereas the main map is masked (in cryoSPARC this is done by default, unless one turns off automatic masking and doesn’t provide any mask). The fact that there is no absolute scale for contour level in cryoEM maps is indeed annoying (I would like to compare maps without worrying that maybe I chose inadequate contour levels). My understanding is that it is caused at least in part by the fact that the size of the box enclosing the particle is arbitrary. Different amounts of low-value voxels between different maps give them different voxel value histograms, therefore choosing a contour level in terms of a certain number of standard deviations above the mean produces different results with different maps. Electron density maps from crystallography don’t have this variability because the box always spans a full unit cell, without this variable padding around the region of high density. At least this is how I understand Tom Goddard’s explanation in this discussion from last month on the Chimerax-users list. Maybe there are other reasons adding to this. I hope this helps. Guillaume Gaullier [email protected] Unfortunately, a fundamental mistake has been made in the much-cited paper by Erickson and Klug (1971) [https://doi.org/10.1098/rstb.1971.0040] more than 50 years ago. They assumed that the EM amplitude contrast of the (stained) biological object is proportional to the phase contrast of the same object over all spatial frequencies. If that were indeed the case, one single transfer function would suffice to describe how the linear imaging device would generate an output image. In reality, the amplitude contrast and phase contrast are two separate properties of the complex transmission function of the object, and these are associated with different physical properties [HA Ferwerda and MG van Heel (1978) https://doi.org/10.1007/978-1-4757-0665-9_47]. The problem is that the proportionality error has crept into almost all popular CTF determination programs where, say, 10% or 15% amplitude contrast is suggested ab initio. Any percentage of amplitude contrast erroneously causes the average density of the cryo-EM 3D reconstruction to deviate from zero. Any phase-contrast image must yield a zero average as it should be for any phase contrast image where what is measured is the difference in phase between any point in the back focal plane of the system with respect to the phase at the origin! That means that the phase at the origin must be zero. (Zero being the average density over the image around which the phase information is a to the transfer function will the of the CTF and the values in programs longer the That results no longer to each other and will also any with density maps in X-ray more Heel [email protected] I would be so with that paper from is always a certain level of experimental and as as I understand it at that time and level it as amplitude and phase be As you point this is the case, and I may a we years into the CTF for an filtered Here a CTF to and the in the experimental and CTF an contrast contrast by the is I for the quality of the but it the best we to with that very at that I may a of to all too that uses this at present. The explanation is for the of very data a CTF to than a few But the problem with the density and the phase at Erickson and Klug (1971) and MG van Heel [email protected] I with about the of using a distribution of the amplitude But a single paper as you say, the problem is rather the of an by the have been of like to amplitude my paper on using and a paper with and where we to use on the cryo-EM in The thing the in the amplitude contrast so we something must have to the all and as we know part and part My 1 [email protected] is adding I guess I will some One to the amplitude contrast from the is from the amplitude contrast by using an as The to an more and I will to I with that a for amplitude contrast is to the We to this in of using and more of this contrast would almost that an as to information is so for that a to the for cryoEM I believe one the phase for the CTF is it is the as it may to for amplitude contrast in It would be we some to the terms in how we the of the experimental image and the of the This at all on the However, as is often the case, the biological paper paper in the paper Electron of an Electron and of In this shows how terms in the give to amplitude I what means by the amplitude contrast and phase contrast are two separate properties of the complex transmission function of the object, and these are associated with different physical is no the amplitude contrast the is by the same as the phase As with it is that is it is the discussion on the of amplitude contrast is I it gets to the of one be to use standard deviations of voxel values to compare different I it the to compare two cryoEM maps at a standard we have CTF and other in the image reconstruction so we have a What do you expect you the voxel The value in each voxel will the average value of the and you will have an approximately distribution of voxel What about the with we have on average one the distribution then be it be a and as the distribution of the potential by the imaging would be So, variable rate is one that may of maps of the same for there is no I can why the distribution should be the same between different or for [email protected] point about the density is the are we a physical unit then we should be to difference maps [email protected] I you are a different As you a difference I to it is between two maps of with a different or In that case, this should be for variable image and data quality you try a distributed with This will the average in each from one map to the average in each of to a difference be to to the lower quality map as it the on [email protected] Dear I never any distribution of the amplitude in my My paper on the and the part of the complex transmission function of the object in and to as as it to electron Any is in electron My paper is based on a with the size of the in the back focal and on an function which is an more van Heel [email protected] I a years and very of as the for the and at the The we are with is about to on a to the and a system for the to any and all from other for what system do you what do you like about your current what do you like least about your current what do you your system do but it what other are you of any or about also to from have can therefore and you have to to a different system and how that to for and tips to a you don’t to the list. to from a of [email protected] We use across (I 3 What do you like about your current it my data to current to do It for and are in the The or one or more to the to also in a across [email protected] gets the job done very because we have other the bulk of and is a that for all the If we as a to do this it would be a from I don’t have to generate reports because we can to do this. 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[email protected] you all for the of on the end of a the trick. on the I'm also the we as it seems that this is a problem with That will be for [email protected]

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Diamond and Carbon-based Materials Research
activated carbon and charcoal
Aerosol Filtration and Electrostatic Precipitation
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