Introduction<\/h2>\n
Certain chemolithotrophic bacteria inhabit ore-bearing geological formations exposed to the atmosphere and obtain all of their energy for growth from the oxidation and dissolution of minerals within the ore. Energy is derived from oxidative phosphorylation coupled to respiratory electron transfer. The ability to respire aerobically on soluble ferrous ions under strongly acidic conditions is currently known to be expressed by at least 34 species in 14 genera distributed throughout the Gram-negative (Markosyan, 1972<\/a>;\u00a0Huber and Stetter, 1989<\/a>;\u00a0Kelly and Wood, 2000<\/a>;\u00a0Hallberg et al., 2010<\/a>), Gram-positive (Clark and Norris, 1996<\/a>;\u00a0Norris et al., 1996<\/a>;\u00a0Johnson et al., 2008<\/a>,\u00a02009<\/a>;\u00a0Guo et al., 2009<\/a>;\u00a0Jiang et al., 2009<\/a>), and Archaea bacteria (Segerer et al., 1986<\/a>;\u00a0Huber et al., 1989<\/a>;\u00a0Huber and Stetter, 1991<\/a>;\u00a0Karavaiko et al., 1994<\/a>;\u00a0Golyshina et al., 2000<\/a>,\u00a02009<\/a>). Given the genetic diversity within this collection of phenotypically related bacteria, it would not be surprising to learn that phylogenetically distinct groups of bacteria express different electron transfer biomolecules and pathways to accomplish aerobic respiration on soluble iron.<\/p>\n Classic reductionist studies that involve the structural and functional characterization of highly purified proteins in dilute solution have described a bewildering variety of different redox-active electron transport proteins in cell-free extracts derived from iron-grown Gram-negative (Cox and Boxer, 1978<\/a>;\u00a0Hart et al., 1991<\/a>;\u00a0Blake et al., 1992<\/a>;\u00a0Yarz\u00e1bal et al., 2002<\/a>,\u00a02004<\/a>), Gram-positive (Blake et al., 1993<\/a>;\u00a0Takai et al., 2001<\/a>;\u00a0Dinarieva et al., 2010<\/a>), and Archaea (Hettmann et al., 1998<\/a>;\u00a0Dopson et al., 2005<\/a>;\u00a0Auernik and Kelly, 2008<\/a>) bacteria. The most promising efforts to date have focused on the iron respiratory chain of\u00a0Acidithiobacillus ferrooxidans<\/i>, where an iron \u201crespirasome\u201d super complex has been defined that is comprised of 2\u00a0c<\/i>-type cytochromes, a blue copper protein called rusticyanin, and an\u00a0aa3<\/sub><\/i>-type terminal oxidase (Castelle et al., 2008<\/a>). The proteins in the aerobic iron respiratory pathway of\u00a0At. ferrooxidans<\/i>\u00a0do not appear to be expressed in many of the phylogenetically distinct bacteria that also respire on iron. Similarly, redox-active proteins expressed in other iron-grown bacteria do not appear to be expressed in iron-grown\u00a0At. ferrooxidans<\/i>. Comparative analyses conducted using those relevant bacterial genomes where partial or complete DNA sequence data is available (Chen et al., 2005<\/a>;\u00a0Ram et al., 2005<\/a>;\u00a0Valdes et al., 2008<\/a>;\u00a0Clum et al., 2009<\/a>;\u00a0Siezen and Wilson, 2009<\/a>) have not yet provided significant insight into other iron respiratory proteins or pathways. There is little information in the DNA databases to compare with because the proteins in the aerobic iron respiratory pathway of\u00a0At. ferrooxidans<\/i>\u00a0do not appear to be universal among those bacteria that respire on iron. In either case, actual respiratory electron transfer in the intact organism is not directly observed. Rather, the functional properties of the intact electron transfer chain are inferred from observations on isolated molecules.<\/p>\n This paper introduces a new means to study respiratory electron transfer reactions\u00a0in situ<\/i>\u00a0in intact bacteria under physiological conditions. The premise is that accurate UV-visible spectroscopy of electron transfer reactions among colored cytochromes can be conducted in highly turbid suspensions if the live bacteria are irradiated in an isotropic homogeneous field of incident measuring light. Under those conditions, the absorbed radiant power is independent of scattering effects (Elterman, 1970<\/a>;\u00a0Fry et al., 1992<\/a>;\u00a0Javorfi et al., 2006<\/a>;\u00a0Hodgkinson et al., 2009<\/a>). We conducted equilibrium and kinetic studies on the Fe(II)-dependent reduction and O2<\/sub>-dependent oxidation of cytochromes in intact\u00a0Leptospirillum ferrooxidans<\/i>\u00a0at pH 1.7. We used a commercial integrating cavity absorption meter (ICAM) where the cuvette comprised a reflecting cavity completely filled with the absorbing suspension.\u00a0L. ferrooxidans<\/i>\u00a0was selected because it is only known to respire on one substrate, reduced iron (Harrison, 1984<\/a>). We observed that a cytochrome with a reduced spectral peak at 579 nm is an obligatory intermediate in the aerobic iron respiratory chain of\u00a0L. ferrooxidans<\/i>.<\/p>\n <\/a><\/p>\n Leptospirillum ferrooxidans<\/i>\u00a0DSMZ 2705 was cultured autotrophically on soluble ferrous ions at 30\u00b0C in the medium described elsewhere (Tuovinen and Kelly, 1973<\/a>), adjusted to pH 1.5 and amended with 44 g\/l of FeSO4<\/sub>\u00b77H2<\/sub>O. Cells grown to stationary phase were harvested by centrifugation, washed three times with 0.02 M H2<\/sub>SO4<\/sub>, pH 1.7, and resuspended in sufficient 0.02 M H2<\/sub>SO4<\/sub>\u00a0to achieve a stock suspension of 1.5 \u00d7 1010<\/sup>\u00a0cells\/ml. The stock suspension was stored at 4\u00b0C for up to 2 weeks while spectroscopic experiments were conducted on aliquots of the cells. Previous stock suspensions of this organism have been stored in dilute sulfuric acid at 4\u00b0C for over 6 weeks before changes in the bacterium\u2019s energy metabolism could be detected.<\/p>\n Absolute numbers of\u00a0L. ferrooxidans<\/i>\u00a0cells were determined by electrical impedance measurements in a Multisizer 4 particle counter (Beckman Coulter, Inc., Brea, CA, USA) fitted with a 30-\u03bcm aperture. The instrument was programmed to siphon 50 \u03bcl of sample that contained Isoton II as the electrolyte. The current applied across the aperture was 600 \u03bcA. Voltage pulses attendant with impedance changes as particles passed through the aperture were monitored with an instrument gain of four.<\/p>\n Relative numbers of\u00a0L. ferrooxidans<\/i>\u00a0cells were determined by photon correlation scattering spectroscopy with a DelsaNano C particle size analyzer, also from Beckman Coulter, Inc. Cell densities were adjusted to 8.3 \u00d7 106<\/sup>\u00a0cells\/ml in 0.02 M sulfuric acid to give an attenuator obscuration of 47%. Determination of the relative numbers of light scattering species as a function of particle diameter was accomplished by the time domain method with operating and analysis software provided by Beckman Coulter, Inc.<\/p>\n Absorbance measurements on intact cells in suspension were conducted in an Olis<\/a> CLARiTY 1000<\/a> A spectrophotometer (On Line Instrument Systems, Inc., Bogart, GA, USA) that employed a novel ICAM. In a typical experiment, identical 4.2 ml solutions that contained ferrous sulfate in 0.02 M sulfuric acid, pH 1.7, were added to both the sample and reference observation cavities of the spectrophotometer. After recording a stable baseline from 350 to 650 nm, 140 \u03bcl were withdrawn from the sample cavity and replaced with 140 \u03bcl of the stock cell suspension of\u00a0L. ferrooxidans<\/i>. Apparent absorbance spectra (typically 6.2 s\u22121<\/sup>) were then collected until any visible absorbance changes had ceased. Raw apparent absorbance values were converted to absorbance values per cm using Fry\u2019s method (Fry et al., 2010<\/a>) as described in the text.<\/p>\n <\/a><\/p>\n The principal features of the novel CLARiTY spectrophotometer used to conduct absorbance measurements in turbid solutions are included in the schematic diagram shown in Figure\u00a01<\/a>. The sample and reference observation cells of this dual beam spectrophotometer were each comprised of a 4.2-ml spherical quartz cuvette fused with a 6-mm ID quartz tube. Each quartz chamber was surrounded by a tightly packed proprietary white powder that served to maximize diffuse reflectance of light on the exterior walls of the spherical flask. The apertures in the reflecting sphere through which the measuring light entered and the transmitted\/scattered light exited to the photomultiplier tube were positioned at a 90\u00b0 angle such that the light had to undergo many reflections and cell transversals before it was quantified using the photomultiplier tube. A white Teflon plug with a 6-mm OD was inserted into the quartz tube to minimize the loss of light out of the neck. A 1.0-cm white stir bar was included in the sample chamber to facilitate sample mixing and suspension of any particulate matter.<\/p>\n The data shown in Figure\u00a02<\/a>\u00a0illustrate how the intact cells of\u00a0L. ferrooxidans<\/i>\u00a0were quantified. The solid line in Figure\u00a02<\/a>\u00a0shows the absolute counts as a function of particle size as determined with a suspension of\u00a0L. ferrooxidans<\/i>\u00a0in the Multisizer 4. The Multisizer determined the number and size of intact bacteria suspended in an electrically conductive liquid by forcing a measured volume of the suspension to flow through a small aperture with an immersed electrode on either side. A current passing through the aperture between the two electrodes enabled the bacteria to be detected by the momentary changes in the electrical impedance as they passed through the aperture, since each bacterium displaced its own volume of electrolyte solution within the aperture itself. These changes in impedance were detected as a series of voltage pulses, for which the height and duration of each pulse were proportional to the volume of the bacterium that produced it. Each pulse was counted and allocated to 1 of 400 arbitrary size categories, or channels. Each channel encompassed a narrow range of volumes that were converted to spherical equivalents and represented by the corresponding spherical diameters on the abscissa of Figure\u00a02<\/a>. The solid line in Figure\u00a02<\/a>\u00a0shows the number of counts in each size range for spherical equivalents with diameters from 0.6 to 2.0 \u03bcm.<\/p>\n The dashed line in Figure\u00a02<\/a>\u00a0shows the relative number of\u00a0L. ferrooxidans<\/i>\u00a0cells as a function of particle size as determined by laser light diffraction. Light scattered by the bacterial suspension produced a diffraction pattern from which the relative numbers of the scattering species at each particle size were calculated. Like the Multisizer, the particle sizes determined by laser light diffraction are expressed as spherical equivalents and are also represented by the corresponding spherical diameters on the abscissa of Figure\u00a02<\/a>. Close correspondence between the electrical impedance and the light diffraction curves was observed down to 0.6 \u03bcm, indicating that the two instruments were monitoring the same population of particles. Bacteria with effective diameters less than 0.6 \u03bcm were underrepresented by the electrical impedance method, by which observations were limited to particles with effective diameters between 2 and 60% of the 30-\u03bcm aperture employed, while the light diffraction method was capable of resolving particles with effective diameters smaller than 0.1 \u03bcm. On the basis of comparisons such as that illustrated in Figure\u00a02<\/a>, it was determined that 19.8% of the bacterial cell counts were below the limit of resolution of the electrical impedance method with the 30-\u03bcm aperture. Accordingly, absolute counts of\u00a0L. ferrooxidans<\/i>\u00a0cells obtained by the electrical impedance method were multiplied by 1.23 to correct for the percentage of bacterial counts that were below the limit of resolution of the instrument.<\/p>\n Cell pellets of\u00a0L. ferrooxidans<\/i>, which were a pinkish tan color, were obtained by centrifugation of batch cultures grown to stationary phase on soluble ferrous iron. Curve\u00a0a<\/strong>\u00a0in Figure\u00a03<\/a>\u00a0shows the absorbance spectrum of oxidized\u00a0L. ferrooxidans<\/i>\u00a0that was obtained in the CLARiTY spectrophotometer in sulfuric acid, pH 1.7. Even though the cell suspension contained 5 \u00d7 108<\/sup>\u00a0cells\/ml and was roughly as turbid as non-fat milk, the resulting absorbance spectrum contained no evidence of the light scattering artifacts that one would observe by conducting the same absorbance measurements using a conventional linear spectrophotometer. The spectrum in curve\u00a0a<\/strong>\u00a0showed a clearly defined Soret peak at 422 nm and a broad \u03b1,\u03b2 band at around 520 nm.<\/p>\n The goal of the initial spectroscopic experiments was simply to determine whether the pink protein(s) in the cells changed color when the cells were suspended in sulfuric acid and subsequently exposed to excess concentrations of soluble ferrous ions under physiological conditions. Curve\u00a0b<\/strong>\u00a0in Figure\u00a03<\/a>\u00a0shows the absorbance spectrum that was obtained when the cells of oxidized\u00a0L. ferrooxidans<\/i>\u00a0were exposed to 100 mM ferrous sulfate in sulfuric acid, pH 1.7. Exposure to excess soluble iron caused the apparent Soret peak to split into two peaks with maxima at 418 and 439 nm. In addition, a new absorbance peak appeared with a maximum absorbance at 579 nm. The absorbance spectrum represented by curve\u00a0b<\/strong>\u00a0appeared immediately after mixing the bacterial suspension in the observation cell that contained the 100-mM soluble iron (\u22640.5 s). This observation indicated that the iron-dependent reduction of the cytochrome(s) in intact\u00a0L. ferrooxidans<\/i>\u00a0was essentially complete within the 0.5-s mixing time in the observation cell of the spectrophotometer. The resulting spectrum was very stable and did not vary for at least an hour after mixing. Although the live cells could respire aerobically on the soluble iron, the great molar excess of iron over molecular oxygen in the observation cell dictated that the cytochromes in the cells would remain predominantly reduced as the oxygen in the chamber was consumed. Evidence for aerobic respiration was taken from the increase in absorbance at wavelengths below 400 nm in curve\u00a0b<\/strong>. Curve\u00a0c<\/strong>\u00a0in Figure\u00a03<\/a>\u00a0shows the absorbance spectrum of 50 \u03bcM ferric sulfate in sulfuric acid, pH 1.7. The increase in the absorbance observed at low wavelengths in curve\u00a0b<\/strong>\u00a0was assumed to be due to ferric ions produced as a consequence of aerobic respiration on iron by the bacteria.<\/p>\n The goal of subsequent spectroscopic experiments was to lower the concentration of soluble iron and determine whether time-dependent changes in the cellular absorbance could be detected. Fe(II) concentrations were chosen such that the total number of electrons available for aerobic respiration was lower than the electron-accepting capacity of the >200 \u03bcM O2<\/sub>\u00a0in the air-saturated suspension. The data in Figure\u00a04<\/a>A show selected absorbance spectra that were obtained when cells of\u00a0L. ferrooxidans<\/i>\u00a0were exposed to 100 \u03bcM ferrous sulfate in sulfuric acid, pH 1.7. The seven absorbance spectra shown in the figure were selected from a data set where 6.2 complete scans from 350 to 650 nm were collected every second for 400 s. Once again, the spectrum of the bacteria produced in the presence of Fe(II) was generated within the operational dead time of mixing, roughly 0.5 s. In this case, however, subsequent aerobic respiration under the conditions of excess molecular oxygen produced time-dependent changes in the observed spectra of whole cells. The reduced peaks at 439 and 579 nm disappeared over a period of 400 s, while the oxidized Soret peak at 422 nm gradually reappeared. In addition, there was a concomitant increase in absorbance at wavelengths below 400 nm. These spectral changes were consistent with the hypothesis that the cells respired aerobically on the soluble iron until the ferrous iron was completely oxidized.<\/p>\n The primary absorbance spectra shown in Figures\u00a03<\/a>\u00a0and\u00a04<\/a>A are presented as \u201capparent absorbance\u201d because of prior reports that spectra obtained using integrated cavity absorption meters appear distorted when compared with corresponding spectra of the same materials obtained using a conventional linear spectrophotometer (Elterman, 1970<\/a>;\u00a0Fry et al., 1992<\/a>;\u00a0Javorfi et al., 2006<\/a>;\u00a0Hodgkinson et al., 2009<\/a>). Unlike single path length spectrophotometers where the Beer\u2013Lambert law governs non-linearity in the measured light intensity as a function of analyte concentration, the measuring light in an integrating sphere makes multiple random passes with different path lengths that exacerbate the apparent non-linearity with analyte concentration. While others have used semi-empirical methods to provide distortion-free spectra (Javorfi et al., 2006<\/a>), we utilized the approach suggested by Fry because it is based on derivations from first principles (Fry et al., 1992<\/a>,\u00a02010<\/a>). Fry arrived at the following exact expression for fractional absorption in an ICAM:<\/p>\nMaterials and Methods<\/h2>\n
Cell Culture<\/h3>\n
Quantification of Bacteria<\/h3>\n
Absorbance Measurements with Cell Suspensions<\/h3>\n
Results<\/h2>\n
The Redox State of Electron Transfer Proteins Can be Monitored\u00a0in situ<\/i>\u00a0in Intact Bacteria under Physiological Conditions<\/h3>\n