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Centre for Cellular and Molecular Biology, Hyderabad, India
Correspondence: Address reprint requests to Amitabha Chattopadhyay, Centre for Cellular and Molecular Biology, Uppal Road, Hyderabad 500 007, India. Tel.: 91-40-2719-2578; Fax: 91-40-2716-0311; E-mail: amit{at}ccmb.res.in.
| ABSTRACT |
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| INTRODUCTION |
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The linear peptide gramicidin forms prototypical ion channels specific for monovalent cations and has been extensively used to study the organization, dynamics, and function of membrane-spanning channels (Killian, 1992
; Koeppe and Andersen, 1996
; Wallace, 2000
). The transmembrane gramicidin channel is formed by the head-to-head dimerization of ß6.3 helices (O'Connell et al., 1990
). The channel interior is lined by the polar carbonyl and amide moieties of the peptide backbone, a feature shared with the selectivity filter of the bacterial KcsA K+ channel (Wallace, 2000
). An important aspect of this conformation is the membrane interfacial location of the tryptophan residues, a common feature of many transmembrane helices (Reithmeier, 1995
; Yau et al., 1998
; Ulmschneider and Sansom, 2001
).
Gramicidins are linear pentadecapeptide antibiotics with a molecular weight of
1900. They are produced by the soil bacterium Bacillus brevis, and consist of alternating L- and D-amino acids (Sarges and Witkop, 1965
). The natural mixture of gramicidins, often denoted as gramicidin A' (termed gramicidin D in older literature), consists of
85% of gramicidin A, which has four tryptophan residues at positions 9, 11, 13, and 15. Gramicidin A' is readily available commercially and is fluorescent, due to the presence of tryptophan residues (Mukherjee and Chattopadhyay, 1994
). It has one of the most hydrophobic sequences known and has been widely used as a model peptide for membrane-spanning regions of intrinsic membrane proteins (Andersen et al., 1999
; Martinac and Hamill, 2002
).
The unique sequence of alternating L- and D-chirality renders gramicidin sensitive to the environment in which it is placed. Gramicidin therefore adopts a wide range of environment-dependent conformations. Two major folding motifs have been identified for gramicidin in various media: 1), the single-stranded helical dimer (the "channel" form), and 2), the double-stranded intertwined helix (collectively known as the "nonchannel" form) (Urry, 1971
; Ramachandran and Chandrasekaran, 1972
; Veatch et al., 1974
). The head-to-head (amino terminal-to-amino terminal) single-stranded ß6.3 helical dimer form is the cation-conducting channel conformation of gramicidin in membranes, originally termed the
helix (Urry, 1971
; Urry et al., 1971
; Ramachandran and Chandrasekaran 1972
; Veatch et al., 1974
, 1975
). This dimer form is stabilized by six intermolecular hydrogen bonds and has been characterized by NMR, circular dichroism (CD), and fluorescence spectroscopy. In this conformation, the carboxy terminus of the peptide is exposed to the membrane interface and the amino terminus is buried in the lipid bilayer. The interior of the channel is formed by the polar peptide backbone and side chains project outward in contact with neighboring lipid fatty acyl chains and help in modulating the channel conductance. The first well-resolved structure of gramicidin in a membrane-mimetic environment, which confirmed and extended the above structural eatures, was obtained by solution NMR (Arseniev et al., 1985
). Later, the high resolution structure of the membrane-bound gramicidin A in a lipid bilayer was deduced by solid-state NMR (Cornell et al., 1988
; Ketchem et al., 1993
). Other conformations (which can be collectively termed as nonchannel conformations) have been shown to exist in membranes with polyunsaturated lipids (Sychev et al., 1993
), and in membranes with increased acyl chain lengths (Killian et al., 1988
; Galbraith and Wallace, 1998
; Zein and Winter, 2000
).
The detailed molecular mechanism of gramicidin adopting various conformations in membranes is not known. However, it has been reported that the initial conformation that gramicidin adopts when incorporated into membranes is dependent on the nature of the solvent in which it was dissolved before incorporation in membranes (LoGrasso et al., 1988
; Killian et al., 1988
). Thus, when gramicidin is dissolved in solvents such as chloroform/methanol, benzene/methanol, or ethanol before incorporation into membranes, it tends to adopt a nonchannel conformation. Upon sonication and incubation at 65°C, this is converted to the characteristic channel conformation. On the other hand, if gramicidin is dissolved in solvents such as trifluoroethanol before membrane incorporation, it appears to adopt the channel conformation even without sonication and incubation at elevated temperature. Gramicidin conformation in membranes therefore appears to be dependent on its "solvent history" (LoGrasso et al., 1988
). The channel conformation of gramicidin in membranes has been characterized in molecular detail by solid-state NMR (Ketchem et al., 1993
; Kovacs et al., 1999
). However, the nonchannel forms in membranes have not been characterized well although various crystal structures of the nonchannel conformations adopted by gramicidin in organic solvents have been deduced (Wallace and Ravikumar, 1988
; Langs, 1988
; Langs et al., 1991
). Interestingly, the crystal structure of the membrane-bound channel form has not yet been solved.
In membranes, the single-stranded ß6.3 dimer channel conformation is the most preferred (thermodynamically stable) conformation (Killian et al., 1988
), and this conformation has been shown to be maintained in membranes with a range of acyl chain lengths (Cornell et al., 1989
) and upon ion occupation (Smith et al., 1990
). The rate of interconversion from the nonchannel to the channel form can be modulated by sonication and prolonged incubation at elevated temperatures (LoGrasso et al., 1988
; Killian et al., 1988
). The membrane-interface-seeking property of tryptophan is implicated in the thermodynamic stability of the single-stranded channel form in membranes (Arumugam et al., 1996
; Wimley and White, 1996
; Chattopadhyay et al., 1997
; Yau et al., 1998
).
Spectroscopic methods provide valuable information about the peptide conformation in membranes in absence of x-ray crystallographic data. Moreover, information obtained from spectroscopic measurements inherently contains useful dynamic aspects, often missing from static crystallographic structures. For gramicidin, CD spectroscopy has served as a valuable tool to distinguish the channel conformation from other forms (LoGrasso et al., 1988
; Killian et al., 1988
; Woolley and Wallace, 1994
). Furthermore, size exclusion chromatography has provided information about the equilibrium ratio of single-stranded and double-stranded conformation existing in various environments (Bañó et al., 1991
; Salom et al., 1998
). However, none of these techniques provide information about the dynamics and the molecular properties such as polarity and viscosity of the immediate microenvironment of the peptide.
In this article, we have investigated the organization and dynamics of the functionally important tryptophan residues of gramicidin in the channel and nonchannel conformations utilizing a combination of red-edge excitation shift (REES) and other fluorescence approaches including membrane penetration depth analysis using the parallax method (Chattopadhyay and London, 1987
), and CD spectroscopy. A shift in the wavelength of maximum fluorescence emission toward higher wavelengths, caused by a shift in the excitation wavelength toward the red edge of the absorption band, is termed REES. This effect is mostly observed with polar fluorophores in motionally restricted media such as very viscous solutions or condensed phases where the dipolar relaxation time for the solvent shell around a fluorophore is comparable to or longer than its fluorescence lifetime (Demchenko, 1988
, 2002
; Mukherjee and Chattopadhyay, 1995
; Chattopadhyay, 2003
; Raghuraman et al., 2003
). REES arises from slow rates of solvent relaxation (reorientation) around an excited-state fluorophore which depends on the motional restriction imposed on the solvent molecules in the immediate vicinity of the fluorophore. Utilizing this approach, it becomes possible to probe the mobility parameters of the environment itself (which is represented by the relaxing solvent molecules) using the fluorophore merely as a reporter group. Further, since the ubiquitous solvent for biological systems is water, the information obtained in such cases will come from the otherwise "optically silent" water molecules.
The unique feature about REES is that whereas all other fluorescence techniques (such as fluorescence quenching, energy transfer, and polarization measurements) yield information about the fluorophore (either intrinsic or extrinsic) itself, REES provides information about the relative rates of solvent (water in biological systems) relaxation dynamics which is not possible to obtain by other techniques. This makes REES extremely useful since hydration plays a crucial modulatory role in a large number of important cellular events including protein folding, lipid-protein interactions, and ion transport (Mentré, 2001
; Kouyama et al., 2004
). An in-depth discussion of the photophysical framework for REES is provided in recent reviews (Chattopadhyay, 2003
; Raghuraman et al., 2003
).
We have previously shown that REES and related techniques (wavelength-selective fluorescence approach) serve as a powerful tool to monitor the organization and dynamics of probes and peptides bound to membranes (Chattopadhyay and Mukherjee, 1993
, 1999a
,b
; Mukherjee and Chattopadhyay, 1994
; Ghosh et al., 1997
; Kelkar et al., 2003
; Mukherjee et al., 2004
) and membrane-mimetic media such as micelles and reverse micelles (Rawat et al., 1997
; Rawat and Chattopadhyay, 1999
; Chattopadhyay et al., 2002
; Raghuraman and Chattopadhyay, 2003
, 2004
; Raghuraman et al., 2004
). In addition, we have previously used the wavelength-selective fluorescence approach to analyze the organization and dynamics of tryptophans in the soluble hemolytic protein
-toxin (Raja et al., 1999
) and the cytoskeletal proteins tubulin (Guha et al., 1996
) and spectrin (Chattopadhyay et al., 2003
).
| MATERIALS AND METHODS |
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) of 0.23 M1 cm1 at 295 nm and optical transparency beyond 310 nm (Eftink, 1991a
Sample preparation
All experiments were done using unilamellar vesicles (ULV) of POPC containing 2% (mol/mol) gramicidin A'. The channel conformation of gramicidin was generated essentially as described earlier (Mukherjee and Chattopadhyay, 1994
). To generate the nonchannel conformation of gramicidin in membranes, ULVs were prepared by the ethanol injection method (Kremer et al., 1977
). In general, 1280 nmol of POPC (640 nmol for the nonchannel form) in chloroform/methanol was mixed with 25.6 nmol of gramicidin (12.8 nmol for the nonchannel form) in methanol. A few drops of chloroform were added to this solution. The solution was mixed well and dried under a stream of nitrogen while warming gently (
40°C) and dried further under a high vacuum for at least 12 h. To prepare the channel form, the dried film was swelled in 1.5 ml of 10 mM sodium phosphate, 150 mM sodium chloride, pH 7.2 buffer, and samples were vortexed for 3 min to uniformly disperse the lipids. The samples were sonicated to clarity under argon (
30 min in short bursts while being cooled in an ice/water mixture) using a Branson model 250 sonifier (Branson Ultrasonics, Danbury, CT) fitted with a microtip. The sonicated samples were centrifuged at 15,000 rpm for 15 min to remove any titanium particles shed from the microtip during sonication, and incubated for 12 h at 65°C with continuous shaking to completely convert to the channel conformation (Killian et al., 1988
; LoGrasso et al., 1988
). For the nonchannel conformation, the dried film was dissolved in ethanol to give a final concentration of 40 mM lipid in ethanol. The ethanolic solution was then injected into 1.5 ml of 10 mM sodium phosphate, 150 mM sodium chloride, pH 7.2 buffer, and samples were vortexed to uniformly disperse the lipids.
Two sets of samples were prepared to monitor the conformational transition of the nonchannel form to the channel form. In one set, nonchannel samples prepared by the above protocol were incubated at 65°C for 12 h. Alternatively, sonication has been suggested to accelerate the conformational transformation (LoGrasso et al., 1988
). A separate set of samples were therefore prepared by sonicating the ULVs formed by the ethanol injection method. The samples were sonicated for 30 min, followed by centrifugation and overnight incubation at 65°C as described above.
All samples were incubated in dark at room temperature for 1 h before fluorescence or CD measurements. Background samples were prepared the same way except that gramicidin was omitted. All experiments were done with multiple sets of samples at 25°C.
Depth measurements using the parallax method
The actual spin (nitroxide) content of the spin-labeled phospholipids (5- and 12-PC) was assayed using fluorescence quenching of anthroyloxy-labeled fatty acids (2- and 12-AS) as described earlier (Abrams and London, 1993
). For depth measurements using the parallax method, ULVs were prepared by sonication followed by incubation at 65°C for 12 h (channel conformation) and by the ethanol injection method (nonchannel conformation) as described above. These samples were made by drying 160 nmol of POPC containing 15 mol % spin-labeled phospholipid (5- or 12-PC) and 3.2 nmol of gramicidin under a stream of nitrogen while being warmed gently (35°C) and then under a high vacuum for at least 3 h. Duplicate samples were prepared in each case except for samples lacking the quencher (5- or 12-PC) where triplicates were prepared. Background samples lacking the fluorophore (gramicidin) were prepared in all experiments, and their fluorescence intensity was subtracted from the respective sample fluorescence intensity.
Steady-state fluorescence measurements
Steady-state fluorescence measurements were performed with a Hitachi F-4010 steady-state spectrofluorometer (Tokyo, Japan) using 1-cm-pathlength quartz cuvettes. Excitation and emission slits with a nominal bandpass of 5 nm were used. Background intensities of samples in which gramicidin was omitted were subtracted from each sample spectrum to cancel out any contribution due to the solvent Raman peak and other scattering artifacts. The spectral shifts obtained with different sets of samples were identical in most cases. In other cases, the values were within ±1 nm of the ones reported. Fluorescence polarization measurements were performed using a Hitachi polarization accessory. Polarization values were calculated from the equation (Lakowicz, 1999
)
![]() | (1) |
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![]() | (2) |
![]() | (3) |
o where kq is the bimolecular quenching constant and
o is the lifetime of the fluorophore in the absence of quencher.
N-Bromosuccinimide modification
Gramicidin in the channel or nonchannel conformation was subjected to NBS modification by serial addition of small aliquots from a freshly prepared 2 mM stock solution of NBS in water to a stirred solution of the sample. The sample was incubated in the sample compartment of the fluorimeter in dark (shutters closed) for 5 min before measurement of fluorescence intensity. The background-subtracted fluorescence intensity was corrected for dilution. The excitation wavelength used was 280 nm and emission was monitored at 331 nm for gramicidin in the channel conformation and at 335 nm for the nonchannel conformation. The fluorescence intensity of gramicidin in absence of NBS served as a control. All experiments were done with multiple sets of samples and average values are shown in Fig. 7.
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![]() | (4) |
i is a pre-exponential factor representing the fractional contribution to the time-resolved decay of the component with a lifetime
i such that
i
i = 1. The decay parameters were recovered using a nonlinear least-squares iterative fitting procedure based on the Marquardt algorithm (Bevington, 1969
2 ratio, the weighted residuals (Lampert et al., 1983
2 value (generally not >1.2). Mean (average) lifetimes 

for biexponential decays of fluorescence were calculated from the decay times and pre-exponential factors using the equation (Lakowicz, 1999
![]() | (5) |
Circular dichroism measurements
CD measurements were carried out at room temperature (25°C) on a JASCO J-715 spectropolarimeter (Tokyo, Japan) which was calibrated with (+)-10-camphorsulfonic acid (Chen and Yang, 1977
). The spectra were scanned in a quartz optical cell with a path length of 0.1 cm. All spectra were recorded in 0.5 nm wavelength increments with a 4-s response and a band width of 1 nm. For monitoring changes in secondary structure, spectra were scanned in the far-UV range from 200 to 280 nm at a scan rate of 100 nm/min. Each spectrum is the average of 12 scans with a full scale sensitivity of 10 mdeg. All spectra were corrected for background by subtraction of appropriate blanks and were smoothed making sure that the overall shape of the spectrum remains unaltered. Data are represented as mean residue ellipticities and were calculated using the formula
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obs is the observed ellipticity in mdeg, l is the pathlength in cm, and C is the concentration of peptide bonds in mol/L. | RESULTS |
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218 and 235 nm, a valley at
230 nm, and negative ellipticity below 208 nm. These are characteristic of the single-stranded ß6.3 conformation. The nonchannel form, on the other hand, is characterized by a large negative peak at 229 nm, a weaker positive peak at 218 nm, and positive ellipticity below 208 nm. As shown in Fig. 1, the CD spectrum of the gramicidin conformation induced by sonication followed by prolonged heat incubation at 65°C, is representative of the channel conformation and that induced by ethanol injection resembles the nonchannel form (Killian et al., 1988
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Red-edge excitation shift of tryptophans as an indicator of gramicidin conformation
The fluorescence emission spectra of various conformations of gramicidin are shown in Fig. 2. Tryptophans in the channel form of gramicidin exhibit an emission maximum of 333 nm, when excited at 280 nm. The emission maximum of the nonchannel form, however, displays a slight red shift and is at 335 nm, in agreement with previous literature (Cox et al., 1992
). Fig. 2 also shows the emission spectra of intermediates I and II. The emission maximum of intermediates I and II are 335 and 334 nm, respectively. It is apparent from the figure that the conversion from the nonchannel to the channel form via intermediates I and II is accompanied by a progressive decrease in fluorescence intensity. The shift in the maxima of fluorescence emission of the tryptophan residues of gramicidin in the channel conformation as a function of excitation wavelength is shown in Fig. 3. (We have used the term maximum of fluorescence emission in a somewhat wider sense here. In every case, we have monitored the wavelength corresponding to maximum fluorescence intensity, as well as the center of mass of the fluorescence emission. In most cases, both these methods yielded the same wavelength. In cases where minor discrepancies were found, the center of mass of emission has been reported as the fluorescence maximum.) As the excitation wavelength is changed from 280 to 310 nm, the emission maximum is shifted from 333 to 340 nm which corresponds to a REES of 7 nm. It is possible that there could be further red shift if excitation is carried out beyond 310 nm. We found it difficult to work in this wavelength range due to low signal/noise ratio and artifacts due to the solvent Raman peak that sometimes remained even after background subtraction. Such dependence of the emission maximum on excitation wavelength is characteristic of the red-edge excitation shift. This implies that the tryptophans in the gramicidin channel conformation are localized in a motionally restricted region of the membrane. This is consistent with the interfacial localization of the channel tryptophans in the membrane (O'Connell et al., 1990
; Cox et al., 1992
; Ketchem et al., 1993
; Mukherjee and Chattopadhyay, 1994
). The membrane interface is characterized by unique motional and dielectric characteristics distinct from both the bulk aqueous phase and the more isotropic hydrocarbon-like deeper regions of the membrane (Ashcroft et al., 1981
; Perochon et al., 1992
; Slater et al., 1993
; White and Wimley, 1994
). This specific region of the membrane exhibits slow rates of solvent relaxation and is also known to participate in intermolecular charge interactions (Yeagle, 1987
) and hydrogen bonding through the polar headgroup (Boggs, 1987
). These structural features which slow down the rate of solvent reorientation have previously been recognized as typical features of microenvironments giving rise to significant REES effects. It is therefore the membrane interface which is most likely to display red-edge effects (Chattopadhyay, 2003
).
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Fluorescence lifetime serves as a sensitive indicator of the local environment and polarity in which a given fluorophore is placed (Prendergast, 1991
). A typical decay profile of gramicidin tryptophans with its biexponential fitting and the statistical parameters used to check the goodness of the fit is shown in Fig. 5. Table 1 shows the gramicidin tryptophan lifetimes in various conformations. As can be seen from the table, all the fluorescence decays could be fitted well with a biexponential function. The mean fluorescence lifetimes of gramicidin tryptophans were calculated using Eq. 5 and are shown in Table 1. The mean fluorescence lifetime for gramicidin tryptophans are found to be longer in the nonchannel form (2.76 ns) than the channel form (1.72 ns). Table 1 also shows the mean fluorescence lifetime for the tryptophans in the intermediates I and II. An increase in polarity of the tryptophan environment is known to reduce the lifetime of tryptophans due to fast deactivating processes in polar environments (Kirby and Steiner, 1970
; Ho and Stubbs, 1992
). The reduction in mean fluorescence lifetime of the tryptophans in the channel conformation can be attributed to the polarity of the interfacial region where the channel tryptophans are localized.
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![]() | (7) |


is the mean fluorescence lifetime taken from Table 1. The values of the apparent rotational correlation times, calculated this way using a value of r0 of 0.09 (Weber, 1960
Acrylamide quenching and N-bromosuccinimide modification of gramicidin tryptophan fluorescence
Acrylamide quenching of tryptophan fluorescence is widely used to monitor tryptophan environments in proteins (Eftink, 1991b
). Fig. 6 shows a representative Stern-Volmer plot of acrylamide quenching of gramicidin tryptophans in the channel and nonchannel conformations. The slope (KSV) of such a plot is related to the accessibility (degree of exposure) of the tryptophans to the quencher. The quenching parameter obtained by analyzing the Stern-Volmer plot is shown in Table 2. The Stern-Volmer constant (KSV) for acrylamide quenching of the nonchannel form of gramicidin was found to be 1.41 M1 whereas the value for the channel form was found to be 0.95 M1. However, interpretation of the Stern-Volmer constant is complicated this way due to its intrinsic dependence on fluorescence lifetime (see Eq. 3). The bimolecular quenching constant (kq) for acrylamide quenching is therefore a more accurate measure of the degree of exposure since kq takes into account differences in fluorescence lifetime. The bimolecular quenching constants, calculated using Eq. 3, are shown in Table 2. The kq values show that the tryptophans in the channel conformation are relatively more accessible to acrylamide although the difference is small. In case of membrane-bound peptides with a heterogenous distribution of tryptophans such as found in the nonchannel conformation of gramicidin, if acrylamide preferentially quenched the exposed tryptophans, a blue shift (i.e., toward lower wavelength) of the residual fluorescence emission maximum would be expected (Caputo and London, 2003
). Interestingly, Fig. 6 shows that the fluorescence emission maximum of gramicidin in either conformation remains invariant and does not exhibit any blue shift of the emission maximum upon quenching by acrylamide.
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The accessibility of the gramicidin tryptophans was further explored by chemical modification using NBS as an oxidant. NBS oxidation of the indole moiety of tryptophan to the nonfluorescent oxindole (Spande and Witkop, 1967
) can be used to assess the relative accessibility of tryptophan residues in proteins and peptides (Raja et al., 1999
; Verza and Bakás, 2000
; Schibli et al., 2002
). Fig. 7 shows the residual fluorescence intensity of gramicidin after NBS modification of tryptophans plotted as a function of molar ratio of NBS to gramicidin tryptophan in the channel and nonchannel conformations. It is apparent from the figure that the tryptophans in the nonchannel conformation are more sensitive to NBS modification than those in the channel conformation. For example, at a molar ratio of NBS to gramicidin tryptophan of 0.2, fluorescence intensity was reduced to 50% in the nonchannel conformation. The corresponding value in the case of the channel conformation was 0.7.
In case of soluble proteins, NBS is unable to modify tryptophan residues that are deeply buried (Raja et al., 1999
; Verza and Bakás, 2000
). Fig. 7 shows that all the tryptophans of gramicidin in either conformation are susceptible to NBS modification and it is possible to completely abolish tryptophan fluorescence with
3 molar excess of NBS (less for the nonchannel conformation). This implies that the membrane bilayer does not act as a barrier to NBS modification and resistance to modification may arise due to decreased accessibility of the tryptophan residues due to packing constraints. Interestingly, the location, depth, orientation, and distribution of the tryptophan residues of gramicidin are markedly different in the channel and nonchannel conformations. In the channel conformation, the gramicidin tryptophans are clustered at the membrane-water interface and Trp-9 and Trp-15 are involved in stacking (aromatic-aromatic) interaction (Hu et al., 1993
; Ketchem et al., 1993
; Mukherjee and Chattopadhyay, 1994
; Separovic et al., 1999
). In the nonchannel conformation, however, there is a distribution of tryptophans along the membrane axis (Arumugam et al., 1996
; see Fig. 8). The increased accessibility of tryptophans in the nonchannel conformation to NBS may be attributed to the relatively shallow location of Trp-15 and Trp-13 in the membrane as opposed to the interfacial location of the tryptophans in the channel conformation. The absence of stacking interaction in the nonchannel conformation may also play a role in the increased accessibility to NBS.
Membrane penetration depths of gramicidin tryptophans
Membrane penetration depth is an important parameter in the study of membrane structure and organization (Chattopadhyay, 1992
; London and Ladokhin, 2002
). Knowledge of the precise depth of a membrane-embedded group or molecule often helps define the conformation and topology of membrane probes and proteins. In addition, properties such as polarity, fluidity, segmental motion, ability to form hydrogen bonds, and the extent of solvent penetration are known to vary in a depth-dependent manner. To gain a better insight of gramicidin conformations in membranes, especially in terms of the localization of the tryptophan residues, average penetration depths of the gramicidin tryptophan residues were determined in the channel and nonchannel conformations. Average depths of the tryptophan residues in membrane-bound gramicidin were calculated by the parallax method (Chattopadhyay and London, 1987
) using the equation
![]() | (8) |
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| DISCUSSION |
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The tryptophan residues in gramicidin channels are believed to be crucial for maintaining the structure and function of the channel (Hu et al., 1993
; Salom et al., 1998
; Andersen et al., 1998
). The importance of the tryptophans has been demonstrated by the observation that the cation conductivity of the channel decreases upon substitution of one or all of the tryptophan residues by phenylalanine, tyrosine, or naphthylalanine (Prasad et al., 1983
; Daumas et al., 1989
; Becker et al., 1991
; Fonseca et al., 1992
), and also upon ultraviolet irradiation or chemical modification of the tryptophan side chains (Barth and Stark, 1991
; Andersen et al., 1998
). In fact, it has been proposed that the tryptophans increase ion permeability by electrostatic interactions (Andersen et al., 1998
; Busath, 1993
).
The distributions and depths of the gramicidin tryptophans represent major differences between the two forms (shown in Fig. 8). The reason that the nonchannel conformation is not the thermodynamically stable form in membranes is due to the fact that in this form some of the tryptophan residues are buried in the low dielectric nonpolar region of the membrane which is energetically unfavorable (Wimley and White, 1996
). The preferred localization of the tryptophan residues at the membrane interface has been ascribed to the ability of the tryptophan-NH groups to form hydrogen bonds with the hydrogen bond acceptors near the lipid headgroups, one of the strongest candidates for such acceptors being the lipid carbonyls (Ippolito et al., 1990
). Interfacial water molecules present near the lipid headgroup region also form a distinct class of possible hydrogen bond acceptors and could give rise to REES effects due to suitable timescale of reorientation. The proposition that the tryptophan residues of membrane-bound gramicidin channels are indeed hydrogen-bonded to the neighboring hydrogen bond acceptors is further supported by the fact that the gramicidin analog in which all the four tryptophan residues are replaced by phenylalanines, which are more hydrophobic and cannot act as hydrogen bond donors, appears to preferentially adopt the alternate antiparallel double-stranded helical dimer conformation (Cotten et al., 1997
; Salom et al., 1998
), and exhibits drastically reduced channel activity (Fonseca et al., 1992
). In the absence of any tryptophan residues, the double-stranded helical dimer nonchannel conformation becomes the energetically favored state in the membrane.
The solvent history dependence of gramicidin conformations in membranes has been previously studied by nuclear magnetic resonance (Zhang et al., 1992
; Arumugam et al., 1996
; Abdul-Manan and Hinton, 1994
; Bouchard et al., 1995
), circular dichroism (LoGrasso et al., 1988
; Killian et al., 1988
), high performance liquid chromatography (Bañó et al., 1991
), and vibrational spectroscopy (Bouchard and Auger, 1993
). In this work, we have utilized red-edge excitation shift (REES), and related fluorescence parameters to distinguish the membrane-bound channel and nonchannel conformations of gramicidin. More specifically, we have used fluorescence lifetime, polarization, quenching, chemical modification, and membrane penetration depth analysis, in addition to REES measurements to address this issue. Our results show that REES, which is sensitive to rate of solvent reorientation and hence a good reporter of the fluorophore environment (rather than the fluorophore itself), can detect gramicidin conformation and could potentially be used to distinguish these two conformations. We have previously shown, using anthroyloxy and NBD-labeled membrane probes, that depth-dependent solvent relaxation in membranes can be used as a "dipstick" (Chattopadhyay and Mukherjee, 1999a
,b
). We show here that this approach can also be used to distinguish conformations of a membrane-bound peptide that differ in the distributions and depths of the tryptophan residues. In summary, we report here novel fluorescence-based approaches to monitor conformations of this important ion channel peptide. Our results offer vital information on the organization and dynamics of the functionally important tryptophan residues in gramicidin.
| ACKNOWLEDGEMENTS |
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S.S.R. thanks the Council of Scientific and Industrial Research, and D.A.K. thanks the University Grants Commission for the award of Senior Research Fellowships. This work was supported by the Department of Science and Technology, and the Council of Scientific and Industrial Research, Government of India.
| FOOTNOTES |
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Satinder S. Rawat's present address is Room 211, Building 469, Laboratory of Experimental and Computational Biology, NCI-FCRDC, National Institutes of Health, Frederick, MD 21702-1201 USA.
Submitted on February 19, 2004; accepted for publication April 12, 2004.
| REFERENCES |
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Abrams, F. S., and E. London. 1993. Extension of the parallax analysis of membrane penetration depth to the polar region of model membranes: use of fluorescence quenching by a spin-label attached to the phospholipid polar headgroup. Biochemistry. 32:1082610831.[CrossRef][Medline]
Andersen, O. S., G. Saberwal, D. V. Greathouse, and R. E. Koeppe. 1996. Gramicidin channelsa solvable membrane "protein" folding problem. Ind. J. Biochem. Biophys. 33:331342.
Andersen, O. S., C. Nielsen, A. M. Maer, J. A. Lundbæk, M. Goulian, and R. E. Koeppe. 1999. Ion channels as tools to monitor lipid bilayer-membrane protein interactions: gramicidin channels as molecular force transducers. Methods Enzymol. 294:208224.[Medline]
Andersen, O. S., D. V. Greathouse, L. L. Providence, M. D. Becker, and R. E. Koeppe. 1998. Importance of tryptophan dipoles for protein function: 5-fluorination of tryptophans in gramicidin A channels. J. Am. Chem. Soc. 120:51425146.[CrossRef]
Arseniev, A. S., I. L. Barsukov, V. F. Bystrov, A. L. Lomize, and Y. A. Ovchinnikov. 1985. 1H-NMR study of gramicidin A transmembrane ion channel. Head-to-head right-handed, single-stranded helices. FEBS Lett. 186:168174.[CrossRef][Medline]
Arumugam, S., S. Pascal, C. L. North, W. Hu, K.-C. Lee, M. Cotten, R. R. Ketchem, F. Xu, M. Brenneman, F. Kovacs, F. Tian, A. Wang, S. Huo, and T. A. Cross. 1996. Conformational trapping in a membrane environment: a regulatory mechanism for protein activity? Proc. Natl. Acad. Sci. USA. 93:58725876.
Ashcroft, R. G., H. G. L. Coster, and J. R. Smith. 1981. The molecular organisation of bimolecular lipid membranes: the dielectric structure of the hydrophilic/hydrophobic interface. Biochim. Biophys. Acta. 643:191204.[Medline]
Bañó, M. C., L. Braco, and C. Abad. 1991. Conformational transitions of gramicidin A in phospholipid model membranes. A high-performance liquid chromatography assessment. Biochemistry. 30:886894.[CrossRef][Medline]
Barth, C., and G. Stark. 1991. Radiation inactivation of ion channels formed by gramicidin A. Protection by lipid double bonds and by
-tocopherol. Biochim. Biophys. Acta. 1066:5458.[Medline]
Becker, M. D., D. V. Greathouse, R. E. Koeppe, and O. S. Andersen. 1991. Amino acid sequence modulation of gramicidin channel function: effects of tryptophan-to-phenylalanine substitutions on the single-channel conductance and duration. Biochemistry. 30:88308839.[CrossRef][Medline]
Bevington, P. R. 1969. Data Reduction and Error Analysis for the Physical Sciences. McGraw-Hill, New York.
Boggs, J. M. 1987. Lipid intermolecular hydrogen bonding: influence on structural organization and membrane function. Biochim. Biophys. Acta. 906:353404.[Medline]
Bouchard, M., and M. Auger. 1993. Solvent history dependence of gramicidin-lipid interactions: a Raman and infrared spectroscopic study. Biophys. J. 65:24842492.
Bouchard, M., J. H. Davis, and M. Auger. 1995. High-speed magic angle spinning solid-state 1H nuclear magnetic resonance study of the conformation of gramicidin A in lipid bilayers. Biophys. J. 69:19331938.
Busath, D. D. 1993. The use of physical methods in determining gramicidin channel structure and function. Annu. Rev. Physiol. 55:473501.[CrossRef][Medline]
Caputo, G. A., and E. London. 2003. Using a novel dual fluorescence quenching assay for measurement of tryptophan depth within lipid bilayers to determine hydrophobic
-helix locations within membranes. Biochemistry. 42:32653274.[CrossRef][Medline]
Chattopadhyay, A. 1992. Membrane penetration depth analysis using fluorescence quenching: a critical review. In Biomembranes Structure & Function: The State of the Art. B. P. Gaber, and K. R. K. Easwaran, editors. Adenine Press, Schenectady, New York. 153163.
Chattopadhyay, A. 2003. Exploring membrane organization and dynamics by the wavelength-selective fluorescence approach. Chem. Phys. Lipids. 122:317.[CrossRef][Medline]
Chattopadhyay, A., and E. London. 1987. Parallax method for direct measurement of membrane penetration depth utilizing fluorescence quenching by spin-labeled phospholipids. Biochemistry. 26:3945.[CrossRef][Medline]