We describe a super-resolution imaging method to probe the structural organization of the bacterial FtsZ-ring, an essential apparatus for cell division. This method is based on quantitative analyses of photoactivated localization microscopy (PALM) images and can be applied to other bacterial cytoskeletal proteins.
Bacterial cell division requires the coordinated assembly of more than ten essential proteins at midcell1,2. Central to this process is the formation of a ring-like suprastructure (Z-ring) by the FtsZ protein at the division plan3,4. The Z-ring consists of multiple single-stranded FtsZ protofilaments, and understanding the arrangement of the protofilaments inside the Z-ring will provide insight into the mechanism of Z-ring assembly and its function as a force generator5,6. This information has remained elusive due to current limitations in conventional fluorescence microscopy and electron microscopy. Conventional fluorescence microscopy is unable to provide a high-resolution image of the Z-ring due to the diffraction limit of light (~200 nm). Electron cryotomographic imaging has detected scattered FtsZ protofilaments in small C. crescentus cells7, but is difficult to apply to larger cells such as E. coli or B. subtilis. Here we describe the application of a super-resolution fluorescence microscopy method, Photoactivated Localization Microscopy (PALM), to quantitatively characterize the structural organization of the E. coli Z-ring8.
PALM imaging offers both high spatial resolution (~35 nm) and specific labeling to enable unambiguous identification of target proteins. We labeled FtsZ with the photoactivatable fluorescent protein mEos2, which switches from green fluorescence (excitation = 488 nm) to red fluorescence (excitation = 561 nm) upon activation at 405 nm9. During a PALM experiment, single FtsZ-mEos2 molecules are stochastically activated and the corresponding centroid positions of the single molecules are determined with <20 nm precision. A super-resolution image of the Z-ring is then reconstructed by superimposing the centroid positions of all detected FtsZ-mEos2 molecules.
Using this method, we found that the Z-ring has a fixed width of ~100 nm and is composed of a loose bundle of FtsZ protofilaments that overlap with each other in three dimensions. These data provide a springboard for further investigations of the cell cycle dependent changes of the Z-ring10 and can be applied to other proteins of interest.
1. Sample Preparation
[1] Note: The above induction protocol (steps 1.1-1.3) has been optimized for the expression system of strain JB281. Detailed induction conditions may vary for other expression systems or proteins of interest.
2. Assembly of the Imaging Chamber
3. Image Acquisition
[2] Note: The integrated intensity of the green fluorescence of a cell is directly proportional to the total number of FtsZ-mEos2 molecules expressed in the cell. The 488-nm excitation power and ensemble fluorescence acquisition settings should be kept constant for all cells so that the relative FtsZ-mEos2 expression levels in different cells can be compared.
[3] Note: Fixed cells are imaged with the Neutral Density (ND) filter (Figure 1, Optical Component #5) in place in order to achieve a slow activation rate so that each individual molecule can be accurately identified. The ND filter is removed when imaging live cells to increase the activation rate, while maintaining a low probability of two molecules being activated simultaneously in a diffraction-limited area. The faster rate applied to live-cell imaging is needed to decrease the total acquisition time, thereby “freezing” the Z-ring in time and limiting the effect of photodamage to the cell.
[4] Note: The numbers of frames acquired were optimized for our system and are dependent on the particular cellular structure, labeling density, activation rate and whether exhausting the entire pool of fluorophores is important for analysis. In live cells, it is important to obtain a sufficient number of localizations in as short a period of time as possible to avoid the blurring of the image due to movement of the cellular structure.
4. PALM Image Construction
[5] Note: The minimum required localization precision was determined empirically for each imaging method by plotting the precisions of all molecules for a given sample and selecting an appropriate cutoff.
5. PALM Image Analysis
[6] Note: We used total internal reflection PALM (TIR-PALM, Figure 1 and 5) to restrict the activation and excitation to a thin layer (~200 nm) above the cell/glass interface. so that only FtsZ molecules associated with the membrane closest to the coverslip will be detected.
Illustrated in Figure 3Aiv is a two-dimensional, super-resolution rendering of the Z-ring generated from the PALM imaging method described above. Below, we summarize qualitative and quantitative information that can be obtained from them.
Qualitatively, we observed that the Z-ring is an irregular structure that adopts multiple configurations (single band or helical arc) that are not distinguishable in conventional fluorescence images (compare Figure 3A-Dii and iv). Observations such as these can be used to determine the percent of the cell population that displays a particular structural configuration.
We can also quantitatively measure the dimensions of the Z-ring. Our approach for determining the ring width and diameter are described in step 5.1 and illustrated in Figure 4. From Figure 4B, the ring width was determined to be 113 nm (FWHM). This value is wider than the expected width of a single FtsZ protofilament (5-10 nm based on in vitro EM11). In Figure 4C, the ring diameter is measured as 1,050 nm. This diameter can be used to quantitatively describe the degree of constriction during cell division.
Another quantitative approach is to calculate the molecule density by counting the number of molecules localized within a defined region. The density measurement provides information about how tightly molecules are packed in the structure. Molecule density can be described in both relative and absolute terms. Relative density (e.g. fraction of molecules in the Z-ring vs. the whole cell) provides information about the distribution of molecules into different cellular regions. Absolute density measurement is complicated by the fact that the PALM image (Figure 3Aiv) is actually a 2D projection of a 3D object. To circumvent this complication, we employ TIR-PALM, which restricts the detection plane to a single side of the Z-ring. The resulting data is illustrated in Figure 5E. Since the plotted molecules represent a subset of the total FtsZ population, the density determined is a lower limit of the actual density. The maximal density observed in the TIR images of the Z-ring suggest that some sections contain overlapping protofilaments 10.
Figure 1. A simplified schematic of our microscope setup. All three lasers are controlled by a custom imaging program developed in MetaMorph that enables precise control over the appropriate excitation wavelength. The dark gray line indicates the excitation light path, while the light gray line indicates the emission path. For total internal reflection (TIR) microscopy, the adjustable platform is translated perpendicular to the light path so as to change the incident angle.
Figure 2. A summary of the PALM method. Initially, all FtsZ-mEos2 molecules are in the green-fluorescence state. Upon exposure to continuous illumination by the 405 and 561 lasers, single molecules are stochastically converted to the red fluorescence state. The rate of this process is determined by the power of the 405 laser, while the photobleaching rate is determined by the power of both the 405 and the 561 laser. Ideally, the rate of activation and photobleaching are balanced in such a way that only one molecule is detected per frame. Once a sufficient number of frames are acquired, the images are processed in Matlab by fitting each identified spot as described in step 4.1. Each unique molecule is then plotted (step 4.4) on a single plane, thus generating a PALM image, shown here in pseudo-red color. The frame outlined in red was determined to contain a repeat spot from the same molecule as the preceding frame and was therefore not included during the construction of the PALM image.
Figure 3. Representative images of fixed (A and B) and live (C and D) cells expressing FtsZ-mEos2. For all cells, the outline and general shape can be visualized in the brightfield image (i). Ensemble fluorescence images (ii) are acquired with excitation from the 488 laser (step 3.8) and represent the distribution of the entire pool of FtsZ-mEos2. The ensemble image reconstructed from the PALM data (iii, step 5.4) provides a qualitative check for the method’s faithful representation of the true ensemble structure. The generated PALM image (iv) is the summation of all unique FtsZ-mEos2 localizations and represents a probability density map for FtsZ-mEos2. The cell outline is represented by the yellow dotted line in images iii and iv. Cells A and C show FtsZ in a single band conformation, while cells B and D illustrate FtsZ adopting a helical arc conformation, which is undetectable in the diffraction-limited ensemble image (iii). Scale bars, 500 nm.
Figure 4. A. A PALM image showing schematic representations of Z-ring width (red) and Z-ring diameter (green). B. Ring width is calculated by fitting the projected intensity profile (blue X’s) along the long axis of the cell with a Gaussian function (gray line) and then determining the FWHM (red dotted line). Here, the ring width was determined to be 113 nm. C. Ring diameter is determined by first projecting the intensity profile along the short axis of the cell and then calculating the full length (green dotted line) of the intensity profile above zero. The diameter of the Z-ring was determined to be 1,050 nm.
Figure 5. TIR-PALM allows for the accurate counting of molecules. As in Figure 3, the brightfield image (A), ensemble fluorescence image (B), reconstructed ensemble fluorescence image (C) and PALM image (D) are illustrated for a given cell expressing FtsZ-mEos2. The same data used to construct D is replotted as a contour plot of molecule density (molecules per pixel) in E. From this density analysis, FtsZ-mEos2 was determined to be maximally present at 8 molecules per pixel. Because a single layer of FtsZ protofilaments would result in a maximum density of 5 molecules per pixel10, this analysis suggests that the Z-ring is composed of multiple layers of FtsZ protofilaments.
PALM images contain information about molecule counts and positions within a cell, allowing detailed analysis of the distribution and arrangement of target protein molecules that is difficult to achieve by other means. Below we outline precautions that should be taken to extract accurate quantitative information while maintaining the biological relevance of PALM images. We also explore the information that can be best obtained using live vs. fixed cells. Finally, we suggest avenues for obtaining additional super-resolution information about the cell division machinery.
The method described above was optimized to produce accurate PALM images in the following ways. First, we characterized and optimized the functionality of the fusion protein to ensure that it serves as a reliable marker of Z-ring structure10. Second, we fine-tuned the expression of the fusion protein since both over- and under-expression results in aberrant structure formation 10,12,13 . Third, we chose thresholds for unique molecule determination (step 4.1.5) based on fluorophore photoblinking properties14. Photoblinking complicates the determination of unique molecules and if disregarded, leads to overcounting of single molecules. Although overcounting does not affect dimension measurements, it does amplify absolute density measurements and may create the appearance of false clusters. All of these factors should be carefully considered when applying this method to other proteins of interest.
The selection of live or fixed cells for imaging depends on the desired information and throughput. Live-cell imaging is fast (30 s), but only reports on localizable (i.e. slow-moving) molecules. This usually means that only membrane-associated molecules are observed in live cells, while fixed cells provide information on all labeled molecules. Live-cell imaging provides high-resolution structural dimensions and morphology, but cannot provide accurate molecule density measurements due to the movement of individual molecules. Fixed cell images can provide all of this information, but require low UV activation level so that unique molecules can be identified. This leads to extended imaging times (> 15 min). In addition, fixation may cause structural aberrations. All of these factors should be balanced when choosing which sample type to use.
The PALM method we have described provides super-resolution details of the Z-ring structure that can be compared across different strains, cell-cycle states, and growth conditions. Implementation of recent technological advances may provide added insight in the cytokinetic mechanism of the Z-ring. For instance, introducing astigmatism into the detection pathway is the simplest way to add three-dimensional capability (~100 nm z-resolution) to the optical setup illustrated in Figure 115. Also, simultaneously imaging of two or more proteins at the same time has become a realistic option with the rapid emergence of spectrally-distinct photoactivatable fluorescent proteins. Finally, the development of a fluorescent protein that photoactivates in a UV-independent manner would allow long-term monitoring of a single cell without generating the DNA damage induced by 405 nm illumination.
The authors have nothing to disclose.
Grant: 5RO1GM086447-02.
Name of Reagent/Material | Company | Catalogue Number | Comments |
50 x MEM Amino Acids | Sigma | M5550 | |
100 x MEM Vitamins | Sigma | M6895 | |
IPTG | Mediatech | 46-102-RF | |
16% Paraformaldehyde | Electron Micrsocopy Sciences | 15710-S | |
SeaPlaque GTG Agarose | Lonzo | 50111 | |
50 nm Gold Beads | Microspheres-Nanospheres | 790113-010 | |
FCS2 Imaging Chamber | Bioptechs | ||
Stage Adaptor | ASI | I-3017 | |
Inverted Microscope | Olympus | IX71 | |
1.45 NA, 60x Objective | Olympus | ||
IXON EMCCD Camera | Andor Technology | DU897E | |
488-nm Sapphire Laser | Coherent | ||
561-nm Sapphire Laser | Coherent | ||
405-nm CUBE Laser | Coherent |