James W.
Beattie
ab,
Ruth C.
Rowland-Jones
c,
Monika
Farys
c,
Richard
Tran
c,
Sergei G.
Kazarian
*b and
Bernadette
Byrne
*a
aDepartment of Life Sciences, Imperial College London, South Kensington Campus, SW7 2AZ, London, UK. E-mail: b.byrne@imperial.ac.uk
bDepartment of Chemical Engineering, Imperial College London, South Kensington Campus, SW7 2AZ, London, UK. E-mail: s.kazarian@imperial.ac.uk
cBiopharm Process Development, GlaxoSmithKline, Gunnels Wood Road, Stevenage, Hertfordshire SG1 2NY, UK. E-mail: richard.x.tran@gsk.com; ruth.x.rowland-jones@gsk.com; monika.x.farys@gsk.com
First published on 16th July 2021
Therapeutic monoclonal antibodies (mAbs) are effective treatments for a range of cancers and other serious diseases, however mAb treatments cost on average ∼$100000 per year per patient, limiting their use. Currently, industry favours Protein A affinity chromatography (PrAc) as the key step in downstream processing of mAbs. This step, although highly efficient, represents a significant mAb production cost. Fouling of the Protein A column and Protein A ligand leaching contribute to the cost of mAb production by shortening the life span of the resin. In this study, we assessed the performance of used PrAc resin recovered from the middle inlet, center and outlet as well as the side inlet of a pilot-scale industrial column. We used a combination of static binding capacity (SBC) analysis and Attenuated Total Reflection-Fourier Transform Infrared (ATR-FTIR) spectroscopy to explore the used resin samples. SBC analysis demonstrated that resin from the inlet of the column had lower binding capacity than resin from the column outlet. ATR-FTIR spectroscopy with PLS (partial least square) analysis confirmed the results obtained from SBC analysis. Importantly, in situ ATR-FTIR spectroscopy also allowed both measurement of the concentration and assessment of the conformational state of the bound Protein A. Our results reveal that PrAc resin degradation after use is dependent on column location and that neither Protein A ligand leaching nor denaturation are responsible for binding capacity loss.
Various steps are employed in downstream processing of recombinantly produced mAbs in order to reduce HCP and HCDNA to safe levels as well as remove high molecular weight species (HMWS) and culture media components.5,10 Safe levels of HCP and HCDNA are recommended at below detectable limits by the FDA11 but are typically in the 1 ng mg−1 range.5 The bulk of contaminating material is removed by Protein A Affinity Chromatography (PrAc).8 Protein A reversibly binds to the CH2 and CH3 region (Fc) of mAbs through a combination of hydrogen bonding, salt bridges and hydrophobic interactions.12 PrAc is employed in a bind/elute mode with binding of IgG to Protein A performed at neutral pH. The IgG is eluted by decreasing the pH of the column, protonating both Histidine 435 of IgG and Histidine 137 of Protein A causing electrostatic repulsion and elution of the IgG from the column.13
PrAc resins have been shown to possess unrivalled purification capabilities, removing 98% of contaminants8 and giving a stepwise recovery yield of up to 99.4%.14 Protein A chromatography does, however, account for the majority of downstream processing costs, due to the high cost and lifetime degradation of the resin.15,16 Downstream processing is responsible for 80% of overall mAb production costs.15
Lifetime degradation is attributed in part to irreversible binding of contaminants which may reduce Protein A ligand accessibility. Although the precise nature of these contaminants is unclear, it has been shown that null-cell culture fluid causes less fouling than mAb containing culture fluid17 and that HCPs accumulate on the Protein A resin after repeated cycles of purification.18
An additional reported cause of lifetime degradation is the harsh alkaline cleaning in place (CIP) procedures used to remove tightly associated contaminant molecules. For every three rounds of Protein A purification performed, one CIP cycle is carried out. CIP protocols usually rely on high concentrations of NaOH (up to 0.5 M),19 with trace amounts of Protein A detected in the CIP eluant.20,21 To minimize protein A leaching and extend column lifespan, agarose-based resins using engineered Protein A ligands have been developed. MabSelect SuRe, for example, utilizes a Protein A ligand with a modified binding domain B, engineered to be more alkaline resistant.21 MabSelect SuRe retains half its binding capacity even after 10 hours of exposure to 0.16 M NaOH.20 Boulet et al. have shown that the MabSelect SuRe Protein A ligand undergoes denaturation at 1.60 M NaOH but that proteolysis only occurs in extremely harsh conditions, such as 6.46 M NaOH,20 a much higher concentration than used for column cleaning.
Whilst it is well known that PrAc resins suffer loss of binding capacity over time, one thing that is not well characterized is whether the loss in binding capacity is homogeneous throughout a Protein A column. A better understanding of this has the potential to make resin use more efficient and thus cut costs associated with mAb purification. Here we used a combination of static binding capacity (SBC) analysis and Attenuated Total Reflection-Fourier Transform Infrared (ATR-FTIR) spectroscopy to explore the performance, ligand density and secondary structure of both Protein A ligand and mAb on MabSelect SuRe samples obtained from a used Protein A column. FTIR spectroscopy is a versatile analytical tool that can analyse the chemical composition of samples in virtually any state. FTIR spectroscopy is a non-destructive, label-free method which can detect multiple components in a system simultaneously. For example, in this study agarose, Protein A ligand, solvent and IgG are all detected in an analysed sample of PrAc resin. The molecular vibrations within a sample absorb mid-infrared radiation of specific frequencies resulting in an energy change, this absorption results in spectral bands at specific wavenumbers making up an individual chemical footprint. ATR allows for the probing of a sample layer of up to 6 μm thickness adjacent to the surface of the IRE (internal reflection element) crystal22 overcoming the issue of strong water absorption in the mid-IR range beyond this depth. Previous work from our groups has applied this technique to assessment of the effects of prolonged CIP exposure by immunoaffinity resins,20 to monitoring the purification of mAbs in-column23 and mAb aggregation.24,25 In a measured mid-IR absorption spectrum, prominent spectral features such as the amide I and amide II bands found at 1600 cm−1–1700 cm−1 and 1520 cm−1–1600 cm−1 respectively are present for proteins. The exact position of peaks and shoulders within the amide bands are dependent on the protein secondary structure present,26 thus the amide bands are extremely important when characterizing proteins.24,25,27–29 Partial least squares (PLS) analysis of our spectroscopic data showcased ATR-FTIR spectroscopy as a simple and effective method of predicting performance of affinity resin for mAb capture and exhibiting additional molecular information of measured samples when compared to traditional OD280 nm based static binding capacity assays. Our findings show that the highest losses in binding capacity are experienced at the Protein A resin column inlet and there is a gradual reduction in binding capacity loss through the length of the column. The loss of binding capacity is not due to a reduction in the amount or conformation of the Protein A ligand bound to the resin in the column but is likely due to irreversible binding of mAbs or HCP fouling within the porous matrix of the Protein A resin.
The Langmuir adsorption isotherm was used to determine the mAb binding capacity of the resin samples from different locations within the pilot scale column. The measured amount of protein in the flow-through (Ceq) after loading samples of various concentrations of IgG4 (C0) was used to calculate the binding capacity (Q) of different resin samples using eqn (1):30
![]() | (1) |
Once the binding capacities of individual resin samples were calculated, the data was fitted to a Langmuir isotherm (2). This allows for prediction of maximum binding capacity (Qmax) and dissociation constant (Kd) for each resin sample.
![]() | (2) |
ATR-FTIR spectra were collected using OPUS 5.5 (Bruker, Germany). Single channel spectra were ratioed using PBS buffer background spectra and a built-in atmospheric compensation algorithm (utilized simulated vapour spectra). This ensured all background buffer liquid and vapour was removed from the spectra. The removal of spectral bands of water was confirmed by the absence of the libration + OH bending mode.31 The generated absorption spectra were then imported to Orange32 with Quasar addon.33 A rubber band baseline correction was applied to the ATR-FTIR spectra in the range 1800.0 cm−1–853.6 cm−1 using Orange. For PLS quantification, ATR-FTIR spectra were normalized at the glycosidic bending mode of the agarose base matrix at 1067 cm−1. All subsequent data analysis was performed in MATLAB (MathWorks, Natick, USA).
Sample | Q max (mg ml−1) | Local Protein A concentrationb (mg ml−1) | Average binding capacityc (mg ml−1) | Average binding capacity predictiond (mg ml−1) |
---|---|---|---|---|
a Q max values obtained from static capacity binding measurements. b Local protein A concentration values obtained from ATR-FTIR spectroscopy measurements of resin samples. Amide II band was integrated. c Average binding capacity is the average binding capacity (Q) of resin when saturated with antibodies by loading with C0 of 5, 6 and 7 mg ml−1 IgG4. d Average binding capacity prediction is the predicted binding capacity of saturated samples obtained from PLSR analysis. | ||||
MabSelect SuRe | 47.51 ± 2.07 | 31.30 ± 9.9 | 43.38 | N/A |
Middle, inlet | 35.61 ± 4.47 | 32.73 ± 12.1 | 34.41 | 25.80 |
Middle, center | 35.78 ± 1.48 | 27.63 ± 0.6 | 33.78 | 36.10 |
Middle outlet | 39.17 ± 2.6 | 20.37 ± 7.4 | 38.01 | 32.72 |
Side, inlet | 34.25 ± 2.37 | 29.04 ± 1.7 | 32.71 | 28.28 |
Overall column | 36.20 ± 2.73 | 29.77 ± 5.45 | 34.63 | 30.08 |
The Kd of mAb binding to the Protein A ligand was the same (0.1 mg ml−1) for each of the test samples as well as the MabSelect SuRe control, indicating that resin use and resin location within the column do not affect binding affinity. This lack of change in binding affinity indicates that despite 25 purification cycles of use the Protein A is not structurally altered. This finding is supported by ATR-FTIR spectroscopy, as the Protein A ligand spectral bands appear at the same wavenumber in both the unused MabSelect control and the used resin samples (Fig. 3). ATR-FTIR spectroscopy of all resin samples show the amide I band at 1654 cm−1, indicative of a primarily alpha helical protein,27 in agreement with the known crystal structure of Protein A.35
Our SBC data clearly show that the effects of repeated use on resin differs according to the location of the resin within the column, with resin at the column inlet exhibiting lower binding capacity than that at the outlet. These findings are in agreement with another study on ion exchange columns.36 Whilst SBC analysis reports on the reduction in the ability of the column to bind antibody it doesn't provide information on the changes within the column that account for this reduction.
Wavenumber (cm−1) | Band assignment |
---|---|
ν is stretching, δ is bending. | |
1688 (shoulder) | Amide I β sheets – protein A |
1654 (shoulder) | Amide I α helix – protein A27 |
1634 (main peak) | Amide I β sheets – IgG425,37 |
1545 (main peak) | Amide II unordered – IgG427 |
1540 (shoulder) | Amide II unordered – IgG427 |
1519 (shoulder) | Amide II – IgG437 |
1455 | CH3δas – IgG425,37 |
1398 | CH3δs – Valine and Alanine – IgG428 |
1375 | Glycosidic linkage – polysaccharide38 |
1238 | Amide III β sheets-IgG425,37 |
1185 | Glycosidic linkage – polysaccharide38 |
1150 | Glycosidic linkage – polysaccharide38 |
1067 | Glycosidic linkage ν – polysaccharide38 |
Partial least squared (PLS) analysis allows utilization of all bands the algorithm detects as being related to the Y value, in this case the capacity, Q (eqn (2)) of mAbs bound to the resin sample. This data contains arrays of thousands of observations representing the absorbance at different wavenumber (1800.0 cm−1–853.6 cm−1) for each resin sample with known concentrations of mAb bound. The data is broken down into components with each component representing a % of variance in the y value. The training data set utilized here was the in situ ATR-FTIR spectra of unused MabSelect SuRe Resin samples obtained from the OD280 nm static binding capacity experiments. In total there were 24 spectra used, with 1 spectrum excluded due to poor IRE contact (ESI Fig. 3†). The training data set utilized 3 components which explained 84.09% of Y variance in the training data. The test data consisted of spectra obtained from ATR-FTIR spectroscopic measurements of 36 spent resin samples saturated with mAbs, with 5 spectra excluded due to poor IRE contact (ESI Fig. 3†). The optimum number of PLS components used was chosen based on the lowest root mean squared error (RMSE) of the cross-validation set. LOOCV was used to test the model.
The loading plot spectra generated by the training data set of unused MabSelect SuRe (Fig. 5) shows the weighting of spectral peaks for each component used to quantify the amount of absorbed mAb. We found that component 1 was predominantly made up of the amide I and II bands at 1634 cm−1 and 1540 cm−1 respectively, with these peaks accounting for 72.77% variance in mAb concentration. Adding a 2nd component predominantly made up of the amide II band shoulder at 1519 cm−1 and amide III band at 1234 cm−1 accounted for a total of 80.87% of the variance in mAb concentration. The third component, representative of the amide II band as well as β sheet CH3 bending and alanine/Valine bending at 1452 cm−1 and 1400 cm−1 respectively, contributed just an extra 3.22% of variance. This component also selected two peaks represented by non mAb components; PDMS Si–CH3 at 1256 cm−1 and the C–OH Agarose peak at 1008 cm−1. The total variance provided by all three components corresponds to 84.09%.
The average binding capacity of saturated spent PrAc resins obtained from the PLS analysis shows the same trend as Qmax values with the resin obtained from the inlet of the used column having the lowest capacity and the resin obtained from the outlet retaining the highest capacity. We found that the RMSE when applying our model to the prediction of used resin was 6.14 mg ml−1 (Table 3). To compare against the traditional approach for measuring SBC, the coefficient of variation (%CV) of the RMSE of our ATR-FTIR PLS model was calculated as 18%:
![]() | (3) |
Data set | Statistic | Value |
---|---|---|
Training | R 2 | 0.84 |
RMSE | 6.08 mg ml−1 | |
LOOCV | Q 2 | 0.75 |
RMSE | 7.84 mg ml−1 | |
Test | Q 2 | 0.12 |
RMSE | 6.14 mg ml−1 |
This was then compared to the %CV calculated for the SBC assay for the overall column average binding capacity; 11%.
![]() | (4) |
Our model produces a good predication of the binding capacity of Protein A resin, meeting industry standards (<20%) and providing additional molecular information when compared to the SBC assay.
PLSR analysis of ATR-FTIR spectroscopic data allowed for the use of multiple spectral bands representing mAbs bound to used PrAc resins, ensuring an accurate prediction of the binding capacity. As expected, the PLS component explaining the most variance in mAb concentration was made up of the Amide I and Amide II bands, as these are the most informative bands for determining secondary structure from the absorption spectra of proteins.
Our data clearly demonstrate that in situ ATR-FTIR spectroscopy can be used to accurately assess the overall performance of a used column. With PLS regression analysis we predicted the overall binding capacity of the used column, when saturated with mAbs, to be 30.08 mg ml−1. This prediction is just 4.55 mg ml−1 below the SBC calculated binding capacity of 34.63 mg ml−1. Intriguingly, the side inlet exhibited the greatest reduction in binding capacity both from the SBC measurements and the ATR-FTIR spectroscopic analysis, with a slightly lower Qmax than the middle inlet. The resin at the side of the column is subjected to a phenomenon known as the wall effect, which results in resin being less packed at this location, forming a preferential route of flow in the column. A potential consequence of this is that resin at the side of the column is exposed to more contaminants/larger build-up of irreversibly bound mAb than in the centre of the column.39
The local Protein A concentration of the used resin samples did not significantly vary from each other or the unused MabSelect SuRe (Table 1), indicating that the loss in binding capacity is not due to Protein A leaching. There was no correlation between local Protein A concentration and static binding capacity (Qmax) measurements of the different resin samples. This finding, together with the spectroscopic analysis revealing no detectable changes in secondary structure of the Protein A ligand (no shift or alteration in shape of the Amide I, II and III bands, Fig. 3) in the used resin samples compared to control, indicated that Protein A ligand loss and denaturation are not causes of the reduction in binding capacity observed for the used resin samples. It is possible that the reduction in SBC is caused by fouling of the resin by either host cell proteins/DNA or the build-up of irreversibly bound mAb.18 This is supported by another study which indicated that lower binding capacity at the inlet of an ion exchange column, as seen here for a Protein A column, was the result of greater fouling due to the load material contact time being the highest here.36
Importantly we reveal that this loss of SBC is not due to Protein A ligand leaching or denaturation. Our data rather suggest that the reduction in binding capacity is due to irreversible fouling. The chemical nature of these contaminants remains to be revealed. The contaminants are not directly observable in this study, likely due in part, to these being under the limit of detection after just 25 cycles of purification. Lintern et al. reported significant contaminant build up, as detected by MS/MS, after 80 cycles of purification.18 In addition, another study reported that fouling tends to occur in the centre of PrA resin beads.36 The penetration depth of the evanescent wave used for ATR-FTIR only probes ∼5 μm of the beads, which can be up to 120 μm in diameter indicating that this technique is unlikely to detect contaminants bound to these resin samples. Since ATR-FTIR spectroscopy is more sensitive to surface layer proteins and less able to probe the interior of the MabSelect SuRe beads, further analysis using confocal Raman microscopy, which can probe further into the beads, might provide additional insights into the causes of binding capacity loss.
This study demonstrates the power inherent in in situ ATR-FTIR spectroscopy, as the molecular information gained from this approach allows quantification of mAb binding, assessment of Protein A ligand concentration and Protein A ligand conformation. Thus the use of in situ ATR-FTIR spectroscopy in this research represents a substantial advance over SBC analysis alone, providing an in-depth assessment of why resin samples exhibit reduced binding capacity. Therefore, this approach may have a significant potential in industrial mAb processing settings.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1an00985k |
This journal is © The Royal Society of Chemistry 2021 |