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Team:Wageningen UR/MethodsDetection
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Detection of Virus Like Particles
A key part of our project is the detection of VLPs. We need sufficient visualization to get conclusive evidence of VLP formation. Besides, we will investigate alternative methods to detect the formation and stability of Virus-Like Particles. In this paragraph we explain in short which methods we used and how these methods work. We also describe the limitations of the techniques, so that other people have an idea about what is possible and what is not.
Electron Microscopy (EM)
The most straight forward method to detect VLPs is Electron Microscopy (EM). We prepared and investigated multiple samples ourselves. This work was done at the Virology department of the Wageningen University.
Electron microscopy works similar to light microscopy, but instead of visible light being used to illuminate the sample, it is done by electrons. The EM has multiple lenses to focus the beam to magnify and light the sample. The lenses are electromagnetic instead of glass and therefore allow a much higher resolution than conventional light microscopy. In theory it is possible to reach a resolution of around 0.005 nm, but in practice it is mostly around 1-2 nm. Possible reasons are certain errors of the lenses, inexperience of the operator (for example our teammembers) or the sample not being thin enough. All these factors can reduce the resolution of the electron microscope. We investigated various samples obtained in our experiments with the help of the EM. The wild types of the Cowpea chlorotic mottle virus (CCMV) and Hepatitis B (HepB) were detected. Multiple variations of CCMV have been tested too, unfortunately with mixed results.
EM Course
The goal of the course was to get familiar with the EM and to handle it safely. Dr. Jan van Lent of the Virology department of Wageningen UR gave us an introduction to EM with a small presentation. During this instruction he explained in detail, the electron miscroscope itself, the preparation of good samples and how to operate the EM properly. Afterwards he showed the sample preparation in the wetlab. Preparation of the sample is critical to have a good resolution and during the course we learned how to do it. The sample must be thin, between 2 - 300nm, and stable in the electron microscope. This can be done by drying or cryo-freezing the sample. After drying or freezing, the sample is stained with a coating containing a heavy metal salt. This coating reflects the electron waves of the microscope, whereas the spots with the VLPs have no coating at all. The missing coating allows the electron waves to go through unhindered. The information of reflection and permeability is processed to an full image which shows the VLPs.
After the preparation of the samples Dr. van Lent explained the whole procedures of visualising a sample. After this last introduction we were able to analyse and investigate multiple samples ourselves.
At the end of the day we were able to use EM for our own experiments starting with sample preparation, handling of the microscope and proper visualization. After the course, the attending team members, were allowed and trained to use the EM without supervision.
Limits
Knowing the limits of techniques is needed to interpret the raw data properly, this is the same with electron microscopy. One of the most troubesome limitation is that the preparation of the sample is laborious and can lead to potential artifacts, which can ruin the sample. Another limitation is that the preparation of the sample, operation of the EM and the analysis of the data requires special training. We were lucky enough to recieve a course on how to use the EM. Also samples that are put into the EM must be resilient against the vacuum in the microscope.
Dynamic Light Scattering (DLS)
Another method to detect VLPs is dynamic light scattering (DLS), also known as photon correlation spectroscopy or quasi-elastic light scattering. This technique is used to measure the size of particles. We applied this technique as a complimentary method next to electron microscopy.
When light travels through the sample and hits a particle, it will scatter in all directions. This scattered light is detected by the DLS. Due to Brownian motion, the particles moves randomly in the solution. These movements of the particles changes the distance of the partilces to the detector. This change of distance to the detector results in constructive or deconstructive interference of the scattered light. The change of intensity of the scattered light by the interference is related to the radius of the particle and can be calculated by the Stokes-Einstein equation.
We investigated various samples with the help of DLS. The main issue was that the sample was not pure or not concentrated enough. After optimization of the production and purification protocol we succeeded to detect VLPs. The main improvement was the implementation of FPLC, which filters out all aggregates and subunits, yielding pure VLP solutions.
Limits
The same as electronmicroscopy, dynamic light scattering has its limits. To detect particles with the DLS, the particle has to have a different refractive index than the solvent. If not the particle doesn't scatter light. Also the sample must be very pure, any dust particle or aggregate can ruin the data output. This is because large particles scatter way more light than small particles. The data analysis requires vast amounts of knowledge and time.
Comparison between the EM and DLS
The electron microscope is used for years to detect VLPs, but is rather expensive to use. So we searched for alternatives. One of the alternatives we found was the technique dynamic light scattering. Dynamic light scattering is sometimes mentioned as a way to detect VLPs, but is never explained throughly. We didn't know any posibilities or limitations of the DLS, so we wanted to see if the output of the DLS is similar as the output of the EM. If the results are positive we can use the DLS as a cheap and easy way to detect VLPs. In order to quantify the DLS, we setup an experiment to compare the size distribution of the VLPs. We produced a large batch of wildtype CCMV monomers and assembeled them in vitro. After purification we split up the sample, one part is analyzed by the electron microscope and the other part is analyzed by the dynamic light scattering technique. To calculate the size distribution of the VLPs with the EM, we took multiple picture of the VLPs. We printed out the pictures and measure by hand each particle induvidually. After the measurments by hand, we calculate the actual radius of each particle and plotted it in a graph. To calculate the size distribution of the VLPs with the DLS, we took the sample and measure it multiple times, so that anomalies are reduced. After measurement we used the CONTIN method to get the size distribution and plotted it in excel.
As seen in figure 4, the size distribution calulated by both methods looks similar. Both the EM and DLS detect particles around 15 nm, precisely what you expect of the literature. The minor differences can be explained, by the methods used to calculate the size distribution. With the EM we visualized the particles first and then calculate the size distribution. With the DLS, the raw output is fitted and can be wrong if the sample is not pure or not concentrated enough. Measuring with the DLS we took that into account by measuring multiple times.
Both the EM and DLS can be used to detect VLPs. This means we've made a solid and secure method to detect and analyze VLPs. With this method it is possible to gain information about VLPs that previously wasn't possible. It is now possible to test the stability of VLPs and many other things.
Sources:
EM
- Jan van Lent
- Transmission Electron Microscopy: A Textbook for Materials Science - David B. Williams, C. Barry Carter
- Quantitative characterization of virus-like particles by asymmetrical flow field flow fractionation, electrospray differential mobility analysis, and transmission electron microscopy - Leonard F. Pease, Daniel I. Lipin, De-Hao Tsai, Michael R. Zachariah, Linda H.L. Lua, Michael J. Tarlov, Anton P.J. Middelberg
DLS
- Remco Fokkink
- Light Scattering from Polymer Solutions and Nanoparticle Dispersions - Wolfgang Schartl
- Nanoparticle-Templated Assembly of Viral Protein Cages - Chao Chen, Marie-Christine Daniel, Zachary T. Quinkert, Mrinmoy De, Barry Stein, Valorie D. Bowman, Paul R. Chipman, Vincent M. Rotello, C. Cheng Kao, and Bogdan Dragnea
- Dynamic Light Scattering: With Applications to Chemistry, Biology, and Physics - Door Bruce J. Berne,Robert Pecora
