Extraction of PE545
Cells of R. salina grew well with obvious accumulation of PE545 (Fig. 1). The purity ratio of crude extract following repeated freeze-thawing was 1.46 (Fig. 2a). In order to facilitate the binding and dissociation of PE545 with the medium under appropriate conditions in the next step of hydrophobic chromatography, the sample needs to be treated with high salt. On the basis of a large number of experiments in the early stage, ammonium sulfate with 50% saturation was selected for sample treatment. After adding an appropriate amount of ammonium sulfate to the crude extract and centrifuging, the purity of PE545 in the supernatant increased slightly to 1.69 (Fig. 2a), and the recovery of PE545 reached 81.35%.
Hydrophobic interaction chromatography
In the next essential step, an FPLC instrument equipped with a Butyl-S Sepharose 6 Fast Flow column was employed for further purification, following preliminary purification via 50% saturated ammonium sulphate fractionation. A change in ionic strength of the mobile phase alters the polarity of proteins, and impurities and PE545 were eluted at different times depending on their differential interactions with the n-butyl groups of the resin (Fig. 2c). The elution volumes of the three different mobile phases were 100 mL, 100 mL and 50 mL.
Absorbance at 545 nm was used for real-time surveillance of PE545 elution. All PE545 was bound to the column in starting buffer containing 2.5 M ammonium sulphate, while a large amount of impurities accounting for ~ 47% of total protein was eluted (A280, peak 1 in Fig. 2c). Following the passage of 20 mM phosphate buffer containing 2.0 M (NH4)2SO4 through the column, more impurities (~ 9% of total protein) were eluted (A280, peak 2 in Fig. 2c). During this process, the absorption value at 545 nm remained zero, and no red component was observed, which indicated that the target protein was still bound to the column material (Fig. 2d). When the mobile phase was changed to 20 mM phosphate buffer, the increase in absorption value at 545 nm and the appearance of a red component in the eluate indicated that PE545 was eluted (Fig. 2d). The results of 545 nm absorption curve integration showed that more than 99% of PE545 was eluted. After PE545 collection in multiple fractions, the fraction with the highest purity (A545/A280 = 13.66) was collected separately, and this accounted for around half of all collected target protein. The final recovery of PE545 was 78.63% (Table 1). Moreover, alongside the improvement in protein purity, there were no significant changes in the characteristics of visible light absorption spectra and fluorescence emission spectra for all three samples (Fig. 2a, b), which indicates that this purification process did not significantly affect the biological properties of PE545. Experimental results showed that the purification effects were superior to others (Doust et al. 2004).
Table 1
Purification efficiency of PE545 from Rhodomonas salina
Purification step
|
Amounts of PE545 (mg)
|
PE545 yield (%)
|
Purity ratio (A545/A280)
|
Purification fold
|
Crude extracts
|
63.08 ± 3.09
|
100
|
1.46 ± 0.15
|
1
|
After n-butyl hydrophobic chromatography
|
49.60 ± 1.98
|
78.63
|
13.66 ± 0.52
|
9.4
|
Data are expressed as the mean ± SD (n = 3). |
The amounts of PE545 were determined with equation system by measures of absorbances at 545 nm. |
Previous studies demonstrated that Butyl-S Sepharose 6 Fast Flow resin is a relatively mild hydrophobic medium that selectively adsorbs PE545 without altering its structural conformation (Hjerten et al. 1974). This type of hydrophobic attraction between PE545 and the n-butyl matrix is due to a net increase in entropy of the environment, which enhances the thermodynamic stability by releasing ordered water molecules surrounding non-polar protein groups into the surrounding solutions, and reducing the non-polar surface area exposed to water. Although hydrophobic forces are affected by many factors, the primary factor here is the amino acid sequence composition of PE545, especially the hydrophobic amino acid distribution on the surface of PE545 (Novoderezhkin et al. 2010).
Gel electrophoresis
Following SDS-PAGE, Coomassie Brilliant Blue staining and Zn2+-enhanced UV-fluorescence autoradiography revealed three bands at the expected positions (α1 and α2 subunits around 10 kDa, and β subunit around 20 kDa) (Fig. 3). Because each α subunit contains only one DBV, its autofluorescence is weaker than that of the β subunit (Scholes et al. 2011). Coomassie Brilliant Blue staining revealed additional impurity protein bands following freeze-thawing extraction of PE545 (lane 4 in Fig. 3), and were absent in the final PE545 (lane 3 in Fig. 3), consistent with the UV-Vis absorption spectra.
Spectral analyses of PE545
Although PE545 with high purity and high yield was obtained using the above-mentioned optimised purification process, we wished to ensure that the purified protein maintained its spectral properties before follow-up studies on energy transfer.
The characteristics of light-harvesting and energy transfer were monitored by absorption spectroscopy and fluorescence spectroscopy. The purified PE545 in the study has a visible light absorption range from 450 nm to 650 nm, with a strong absorption peak at 545 nm and a shoulder peak at 564 nm (Fig. 4a). A fluorescence emission peak of purified PE545 was observed at 587 nm following excitation at 545 nm (Fig. 4b). Comparing the absorption and fluorescence emission spectra showed that the α1α2 ββ heterodimer of PE545 has a 42 nm red shift from 545 nm to 587 nm. These spectra revealed that the purified protein retained its complete energy transfer properties, consistent with previous reports for purified PE545 (Novoderezhkin et al. 2010; Tong et al. 2020). As the basis of the energy transfer function of PE545, the main absorption band of PE545 is due to the PEB chromophore, and the main fluorescence emission peak at 587 nm is derived from the DBV chromophore, consistent with the results of previous studies (Wilk et al. 1999; Doust et al. 2004). Meanwhile, the fluorescence spectrum can also identify the quantum state of specific chromophore molecules, in addition to reflecting the internal energy transfer ability. The fluorescence properties were similar to those reported previously, indicating that the energy transfer function of PE545 purified by the new method was unchanged (Marrone 1999). Again, because the function of PE545 is closely related to its structure, these results also proved that the protein microenvironment and quantum states of the chromophore in PE545 were not altered, which further confirms the reliability of the new purification method.
CD spectroscopy is associated with the absorbance of a target substance, and it is also affected by molecular asymmetry or conformational asymmetry. In the visible region (450–750 nm), the main contribution to the CD spectrum is from the chromophore, hence it is very sensitive for reflecting the structure of the chromophore. Thus, CD spectra are suitable for in-depth confirmatory testing of the integrity of chromophore conformation, chromophore structure, and chromophore function. As can be seen from Fig. 4c, the CD spectra of purified PE545 had a pronounced positive peak at 536 nm and a negative peak at 569 nm, with the positive and negative peaks intersecting at 554 nm, consistent with literature reports (Maccoll et al. 1994; Doust et al. 2006). Furthermore, the intersecting point at 554 nm suggests a strongly coupled chromophore pair with exciton splitting and excitation delocalisation. These results agree well with the absorbance of two double-bound PEB groups (β50/β61) at the central interface of the PE545 dimer, which further demonstrates the retained spatial conformation of the chromophores (Maccoll et al. 1994). This verifies that the purified PE545 had good structural and functional integrity, and the complete energy transfer function was maintained.
To verify these results in more depth, the second-order derivative Gauss formula was used to deconvolute the absorption spectrum, the fluorescence emission spectrum, and the CD spectrum of the final high purity PE545 (Fig. 4). In the absorption spectrum, two spectral components at 545 nm and 569 nm were obtained by Gaussian deconvolution with R2 = 0.99256 (Fig. 4a). In the fluorescence emission spectrum following excitation at 545 nm, two peaks (582 nm and 609 nm) were also obtained with R2 = 0.99898 (Fig. 4b). Deconvolution of the CD spectrum yielded three peaks at 516 nm, 536 nm and 569 nm, with an R2 value of 0.96767 (Fig. 4c). All deconvolution data were also in good agreement with reported spectral components (Maccoll et al. 1994), and the results further confirmed that the optical activity was not altered by the purification method.