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Journal of Bacteriology, August 2002, p. 4313-4315, Vol. 184, No. 15
0021-9193/02/$04.00+0 DOI: 10.1128/JB.184.15.4313-4315.2002
Copyright © 2002, American Society for Microbiology. All Rights Reserved.
Department of Cell Biology, Duke University Medical Center, Durham, North Carolina 27710-3709,1 Department of Molecular Biology and Microbiology, School of Medicine, Case Western Reserve University, Cleveland, Ohio 44106-49602
Received 27 February 2002/ Accepted 6 May 2002
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Purified ZipA derivatives (5) were subjected to sedimentation through a glycerol gradient and then examined by rotary shadowing electron microscopy (EM) as previously described (2). Figure 1a shows a micrograph of ZipA(23-328), which contains the complete charged domain, the P/Q domain, and the C-terminal globular domain of native ZipA (5). Figure 1b shows ZipA(186-328), which comprises only the C-terminal globular domain. These two constructs were described previously (4). The C-terminal domain appears as small globular particles about 3.5 to 4 nm in diameter (the diameter was estimated after subtracting 2 nm for the thickness of the platinum shell), consistent with the size (2.5 by 3.5 by 5 nm) of the C-terminal domain determined by X-ray crystallography (10) and nuclear magnetic resonance analysis (11). ZipA(23-328) showed globular particles that were indistinguishable from the C-terminal domain alone. Occasionally, a very small globular particle or a thin extension could be seen close to the main globular particle but, for the most part, there was no visible structure corresponding to the charged and P/Q domains in ZipA(23-328). This suggested that the P/Q domain may be a largely unfolded polypeptide and invisible in the rotary shadowed specimen, consistent with the previous prediction from the sequence (3). We suggest that the charged domain may be unstructured as well because, in our experience, a 60-aa globular domain should be visible in rotary shadowing. This is supported by the lack of predicted secondary structure in the charged domain (13).
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FIG. 1. Rotary shadowing EM of ZipA(23-328) (a) and ZipA(186-328) (b) (the C-terminal domain alone). Both samples show small globular particles of similar sizes. The charged-plus-P/Q domain of ZipA(23-328) is mostly invisible, although occasionally a faint projection or small domain may be discerned. (c) EM of GFP-ZipA. The GFP-ZipA(39-328) fusion protein is visible as pairs of globular domains; presumably, these domains are connected by the charged-plus-P/Q domain, which is not visible. The middle panels show selected pairs with two globular domains of similar sizes, and the bottom panels show pairs with different-sized globular domains.
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An unfolded polypeptide can be modeled as a worm-like chain characterized by a contour length L and a persistence length p. Rivetti et al. (15) provided an elegant analysis of DNA on mica, modeled as a worm-like chain, and concluded that the molecules rearranged by diffusion on the two-dimensional mica substrate. For our analysis, we assume that the flexible polypeptide can also assume a random two-dimensional distribution on mica (see reference 15 for a detailed discussion of the two-dimensional structure versus the three-dimensional structure of the worm-like chain). The distribution of end-to-end lengths of the worm-like chains is given by the formula <R2> = 4pL (for the case in which L >> p), where R is the distance between the ends of the chain, <R2> is the average value of R2, L is the contour length, and p is the persistence length.
The R value needed for the above formula is the distance between the ends of the flexible chain, but the best estimate we can make is to measure the center-to-center distance between the two globular domains. A histogram of center-to-center distances is shown in Fig. 2. We considered subtracting 4 nm, the sum of the predicted radii of the N- and C-terminal globular domains, from the measured center-to-center distance. This correction would be appropriate if the exit points of the polypeptide from the two globular domains were facing each other (as illustrated in Fig. 3b, c, and e). However, it is also possible that these exit points face away from each other and the polypeptide crosses over or around the domains (as in Fig. 3d), in which case we should add 4 nm. If we assume that the P/Q segment is quite flexible and the orientation of the globular domains is random, the simple center-to-center distance seems to be the best estimate of the end-to-end length of the charged-plus-P/Q segment. Note, however, that each measurement includes an up to ±5-nm error due to the unknown orientation of the globular domains.
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FIG. 2. Histogram of the center-to-center distance between the globular particles in GFP-ZipA(39-328) used as an estimate of the end-to-end length of the charged-plus-P/Q domain (see text for details). The histogram shows a broad distribution of distances, with an average of 12 nm.
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FIG. 3. Molecular models of conformations of the unstructured charged-plus-P/Q domain of ZipA. The GFP domain is shown at the N terminus, which, in native ZipA, would be replaced by the transmembrane anchor. The maximally extended polypeptide is shown in panel a. A single-loop (b) or winding-chain (c, d, and e) structure can bring the termini closer together. The model was constructed from the atomic structures of GFP and the ZipA C-terminal domain, obtained from the protein database (1ema and 1F47). The extended polypeptide was modeled on segments of beta strands.
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We also characterized the ZipA(23-328) and GFP-ZipA(39-328) proteins by sedimentation analysis. Determination of sedimentation coefficients by analytical ultracentrifugation (20,000 rpm in the ANL rotor, Beckman XLA analytical ultracentrifuge) yielded values of 2.2S for ZipA(23-328) and 3.2S for GFP-ZipA(39-328). To estimate the shape of the proteins, we calculated Smax/S, where Smax is the sedimentation coefficient of an unhydrated sphere of protein of the same mass. Smax/S was calculated to be 1.73 for ZipA(23-328) and 1.75 for GFP-ZipA(39-328). These values are indicative of moderately elongated proteins (16) and are consistent with the EM studies described above, suggesting that the P/Q domain of ZipA is largely unfolded.
Figure 3 presents molecular models of the GFP-ZipA structure showing the charged-plus-P/Q domains as unstructured polypeptide. Note that the GFP in our construct is at the position of the transmembrane segment. We propose, on the basis of our EM analyses, that the tether is flexible and can span a maximum distance of 60 nm. In the more relaxed conformations, FtsZ subunits that are bound to the C-terminal FtsZ binding domain of ZipA could be an average of 12 nm from the membrane. Since the FtsZ protofilaments are only 3 to 4 nm thick, the tether is long enough to loop around and bind the C terminus of FtsZ, even if it is facing away from the membrane (see reference 1 for a diagram).
This study was supported by National Institutes of Health grants CA47056 (H.P.E.) and GM-57059 (P.D.B.).
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