Previous Article | Next Article ![]()
Journal of Bacteriology, July 2003, p. 4226-4232, Vol. 185, No. 14
0021-9193/03/$08.00+0 DOI: 10.1128/JB.185.14.4226-4232.2003
Copyright © 2003, American Society for Microbiology. All Rights Reserved.
-Helical Core
Unidad de Biofísica (Centro Mixto CSIC-UPV/EHU) and Departamento de Bioquímica, Universidad del País Vasco, E-48080 Bilbao,1 Departamento de Biología Molecular (Unidad Asociada al C.I.B., CSIC), Universidad de Cantabria, E-39011, Santander, Spain2
Received 10 February 2003/ Accepted 16 April 2003
|
|
|---|
/ß structure with some amount of unordered structure. Fast heating and cooling does not change the secondary structure, whereas slow heating produces two bands in the infrared spectrum characteristic of protein aggregation. The denaturation temperature is increased in the protein after the fast-heating thermal shock. Two-dimensional infrared correlation spectroscopy shows that thermal unfolding is a very cooperative two-state process without any appreciable steps prior to aggregation. After aggregation, the
-helix percentage is not altered and
-helix signal does not show in the correlation maps, meaning that the helices are not affected by heating. The results indicate that the domain has an
-helix core resistant to temperature and responsible for folding after fast heating and an outer layer of ß-sheet and unordered structure that aggregates under slow heating. The combination of a compact core and a flexible outer layer could be related to the structural requirements of DNA-protein binding. |
|
|---|
Relaxases are classified into five families according to the DNA sequences around the nic sites and their amino acid sequences (9). The F family relaxase TrwC, from the IncW plasmid R388, is a dimeric protein of 996 amino acids in which the N-terminal domain has a DNA relaxase activity and the C-terminal domain is a DNA helicase (18). In addition to relaxase and helicase activities, the TrwC protein promotes site-specific recombination between oriT sequences in vivo. In addition, it can cleave a supercoiled plasmid DNA containing oriT in vitro in the absence of accessory proteins (17).
Infrared (IR) spectroscopy has become a widely used tool in the study of protein structure. In principle, a structure as large as a protein would give rise to an enormous number of overlapping vibrational modes, obscuring the information that could be obtained in practice, but because of the repeating patterns of the biological molecules, e.g., the secondary structure of the protein backbone, the spectra are much simpler, and useful structural information can be obtained. Structural analysis usually implies a mathematical approach in order to extract the information contained in the composite bands, designated "amide bands" in IR spectroscopy, obtained from proteins. Commonly used methods of analysis involve narrowing the intrinsic bandwidths to visualize the overlapping band components and then decomposing the original band contour into these components by means of an iterative process. The various components are finally assigned to protein or subunit structural features (3). External perturbations, such as temperature, are commonly used to obtain a deeper insight into protein structure by means of IR spectroscopy. Thermal profiles have often been used to study conformational changes in proteins (1). More recently, Noda (21) has proposed the use of two-dimensional correlation spectroscopy (2-D IR) to increase the amount of information obtained from the IR spectrum.
In the present work, we have used conventional and 2-D IR to study the structure and temperature effects of a truncated protein from TrwC, namely, its N275 segment, consisting of 275 amino acids from the N-terminal domain. It has been shown that the N-terminal domain, containing the relaxase activity, and the C-terminal domain, containing the helicase activity, can be dissected and reconstituted (18). N275 purification involves a step in which the homogenate is heated at 90°C while IR spectroscopy confirms that the protein is thermally stable under certain conditions and shows that an
-helical core is the basis of thermal stability.
|
|
|---|
IR studies. The protein samples were typically measured at 10 mg/ml in a 50 mM Tris-HCl-150 mM NaCl buffer, pH or pD 7.6. The H-D exchange was carried out by lyophilization. The spectra were recorded in a Nicolet Magna II 550 spectrometer equipped with a mercury-cadmium-telluride detector using a demountable liquid cell (Harrick Scientific, Ossining, N.Y.) with calcium fluoride windows and 6-µm spacers for samples in H2O medium or 50-µm spacers for samples in D2O medium. A tungsten-copper thermocouple was placed directly onto the window, and the cell was placed into a cell mount equipped with a thermostat. Typically, 1,000 scans for each background and sample were collected, and the spectra were obtained with a nominal resolution of 2 cm-1. The water contribution was subtracted as described earlier (1). Typically, a flat baseline between 1,900 and 1,300 cm-1 is obtained with the maximum subtraction factor. This is equivalent to suppressing the water band around 2,125 cm-1. The data treatment and band decomposition of the original amide I have been described elsewhere (2, 3, 5). The mathematical solution of the decomposition may not be unique, but if restrictions are imposed, such as maintenance of the initial band positions in an interval of ±1 cm-1, preservation of the bandwidth within the expected limits, or agreement with theoretical boundaries or predictions, the result becomes, in practice, unique.
Thermal analysis was performed in the 30 to 80°C interval in 3°C steps. At every step, the sample was left to stabilize and the spectra were measured as described above. To obtain the 2-D IR maps, heating was used as the perturbation to induce time-dependent spectral fluctuations and to detect dynamic spectral variations on the secondary structure of TrwC-N275. 2-D synchronous and asynchronous spectra were obtained as described elsewhere (8, 22)
|
|
|---|
![]() View larger version (52K): [in a new window] |
FIG. 1. Purification of protein TrwC-N275 and results of thermal treatment. (A) Sodium dodecyl sulfate-polyacrylamide gel electrophoresis (SDS-PAGE) of fractions obtained in a standard purification scheme, as reported by Llosa et al. (18). Lanes: 1, molecular mass markers (in kilodaltons); 2, soluble lysate after ultracentrifugation; 3, active fraction after phosphocellulose chromatography; 4, active fraction after gel filtration chromatography. (B) Fraction 2 in panel A was subjected to heating at 90°C for various times and developed by SDS-PAGE. Lanes: 1, soluble lysate after ultracentrifugation; 2, supernatant after 5-min heat treatment; 3, supernatant after 10-min heat treatment; 4, supernatant after 20-min heat treatment; 5, supernatant after 30-min heat treatment; 6, pure TrwC-N275 protein (fraction 3 in panel A) without heat treatment; 7, molecular mass markers.
|
O stretching vibration of the peptide bond. The band is conformationally sensitive and can be used to monitor either the secondary-structure composition or the conformational changes induced by external agents, such as temperature. Differences in dihedral angles and hydrogen bonding among the different protein conformations give rise to a composite band containing the structural information of the protein (2). The information can be extracted by using different mathematical techniques. Band-narrowing procedures allow the determination of the number and positions of the components, even if they do not improve resolution. Figure 2 shows the 1,800- to 1500-cm-1 regions of TrwC-N275 IR spectra in H2O and D2O media (Fig. 2A) and their corresponding deconvolved spectra in the 1,700- to 1,600-cm-1 amide I region (Fig. 2B), where the different band components can be seen. The combined use of H2O and D2O spectra is required in order to facilitate spectral analysis, because water absorbs strongly in this region of the IR spectrum. The amide II band, located between 1,600 and 1,500 cm-1 in H2O, arises mainly from NH bending of the peptide bond. However, this band is less conformationally sensitive than amide I, and it is not normally used in protein studies. In D2O, amide II shifts to
1,470 cm-1, and the bands remaining in the 1,600- to 1500-cm-1 regions of the spectra are assigned to amino acid side chains.
![]() View larger version (14K): [in a new window] |
FIG. 2. IR spectrum of TrwC-N275 in the 1,800- to 1,500-cm-1 region. (A) Original (nonsmoothed) spectra in H2O (bottom) or D2O (top) medium after buffer subtraction. (B) Amide I region (1,700 to 1,600 cm-1) after deconvolution using a half width at half height of 18 cm-1 and a narrowing factor of 2.
|
-helix, 39% ß-sheet, 18% ß-turns, and 20% unordered structure.
![]() View larger version (15K): [in a new window] |
FIG. 3. Amide I band decomposition of TrwC-N275 in D2O (A) or H2O (B). The dotted line corresponds to the sum of the band components. The numerical values are presented in Table 1.
|
|
View this table: [in a new window] |
TABLE 1. Band positions, percent area, and assignment of components obtained after curve fitting of TrwC-N275 in H2O and D2O
|
-helix, seems not to be affected by aggregation and that the band at 1,618 cm-1 arises mainly at the expense of the ß-sheet structure. |
View this table: [in a new window] |
TABLE 2. Parameters corresponding to amide I band decomposition of TrwC-N275 under different conditions
|
5°C in the denaturation temperature of the water bath-heated protein. However, no differences are seen in the starting or end points of the curves or in their slopes, pointing to similar cooperative processes in both cases. In the case of slow heating, the denaturation temperature is also affected by the protein concentration (Fig. 5B).
![]() View larger version (32K): [in a new window] |
FIG. 4. 3-D plot of the deconvolved amide I region in D2O in the 25 to 65°C interval showing the aggregation bands.
|
![]() View larger version (15K): [in a new window] |
FIG. 5. Thermal profile of TrwC-N275. (A) Profiles corresponding to protein concentrations of 15 ( ), 10 (), and 5 ( ) mg/ml. (B) Traces corresponding to the protein isolated without () or with ( ) heating to 90°C for 10 min.
|
-helix, confirming the data in Table 2, according to which an
-helix core resists thermal denaturation. The asynchronous map provides information about the time course of the events produced by temperature perturbation, depending on the peak intensity. The asynchronous map in Fig. 6 indicates that the most intense peaks correspond to bands cross-correlated with the 1,618-cm-1 aggregation peak. The simplicity of the aggregation-related pattern confirms the temperature-induced two-state denaturation of TrwC-N275.
![]() View larger version (48K): [in a new window] |
FIG. 6. Synchronous (left) and asynchronous (right) correlation map contours in the interval 1,700 to 1,600 cm-1 of TrwC-N275 in the interval 40 to 65°C, where thermal denaturation takes place.
|
|
|
|---|
The structure and temperature-induced perturbation of TrwC-N275 have been studied by classical and 2-D IR spectroscopy. From the spectra in H2O and D2O, it can be concluded that TrwC-N275 is an
/ß protein (Fig. 2). The thermal profile points to TrwC-N275 denaturation as a two-step process, and together with the simplicity of the 2-D correlation maps, to a very cooperative unfolding (Fig. 4 and 5).
The comparison between water bath-heated protein and protein warmed gradually provides some interesting information. The purification procedure of TrwC-N275 involves a fast heating and cooling process (see Materials and Methods). The data in Fig. 5 indicate that fast thermal denaturation is fully reversible and that the protein obtained following the purification protocol described above is in a state essentially similar to the native state. Slow warming, however, appears to cause irreversible denaturation (Table 2). The change in denaturation temperature has been associated, in other proteins, with variations in the protein compactness. However, we have observed in this protein, but not in others (e.g., concanavalin A [4], tyrosine hydroxilase [19], and cytochrome c [20]), that the protein concentration can affect the denaturation temperature. In fact, measuring denaturation at a 5- or 15-mg/ml protein concentration changes the denaturation temperature from 43 to 48°C (Fig. 5A). However, it has to be taken into account that thermal denaturation is a kinetic process that depends on the environmental conditions, such as the rate of heating (11). In TrwC-N275, we have observed that heating in a continuous mode (12) instead of the step method used here increases the denaturation temperature of TrwC-N275 to the same value as that of the water bath-heated protein (data not shown).
It is interesting that an
-helix is still present in the aggregated protein. The aggregation process usually involves unfolding of the protein, including its secondary-structure elements, such as the
-helix or ß-sheet, exposing the hydrophobic core that establishes intermolecular interactions and aggregation. This result from secondary-structure analysis is reinforced by 2-D maps in which no peaks involving the 1,650-cm-1 band are seen in the synchronous spectra (Fig. 6). A stepwise denaturation process with different temperatures for ß-sheet and
-helix unfolding has been seen in various proteins. In Paracoccus denitrificans, the cytochrome oxidase ß-sheet had a lower denaturation temperature than the
-helix (10), and this was attributed to the fact that whereas the
-helical structure was inside the membrane, the ß-sheet was exposed on the outside. Also, in low-density lipoprotein oxidation (7), the ß-sheet structure was affected only after
-helix oxidation had taken place. Moreover, in the tetrameric protein methionine adenosyl synthetase, in which the subunit-subunit interaction occurs through ß-sheet components, 2-D IR spectroscopy indicates that the
-helix unfolds first, and later, after the subunit-subunit interactions are loosened, the ß-sheet starts to unfold (J. L. R. Arrondo, unpublished data). Thus, it can be predicted from our data that TrwC-N275 has a core consisting mainly of
-helix, while the ß-sheet is more exposed, probably located in the outer part of the protein. This
-helix core does not unfold even after the aggregation process has been completed, and it would be responsible for the protein maintaining its activity even after being heated at 90°C for 10 min. The crystal structure of the adeno-associated virus replication protein has recently been solved (14). This protein also binds a replication origin and contains a three-histidine motif common to relaxases and rolling-circle replication initiation proteins (15). Thus, it is a probable structural homolog of TrwC-N275. Interestingly, this replication protein is also an
/ß protein in which the helices can establish contacts among themselves on one side of a ß-sheet and, according to the results presented here, probably constitute a compact core.
In summary, IR spectroscopy shows that TrwC is an
/ß protein not affected by fast heating and cooling, with an
-helix core that is not affected by thermal denaturation and an outer, more flexible layer composed of a ß-sheet plus unordered segments. This unique feature could be related to the fact that peptide-DNA binding induces secondary structure (24, 25). Thus, the flexible layer would bind DNA supported by the scaffold of the compact core.
|
|
|---|
This article has been cited by other articles:
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
Copyright © 2009 by the American Society for Microbiology. For an alternate route to Journals.ASM.org, visit: http://intl-journals.asm.org | More Info»