Open Access Article
Shane D.
Curry
a,
Bryce M.
Bower
a,
Sven A.
Saemundsson
a,
Andrew P.
Goodwin
*ab and
Jennifer N.
Cha
*abc
aDepartment of Chemical and Biological Engineering, University of Colorado, Boulder, 596 UCB, Boulder, CO 80303, USA. E-mail: Jennifer.Cha@colorado.edu; Andrew.Goodwin@colorado.edu
bMaterials Science and Engineering Program, University of Colorado, Boulder, 596 UCB, Boulder, CO 80303, USA
cBiomedical Engineering Program, University of Colorado, Boulder, 596 UCB, Boulder, CO 80303, USA
First published on 24th February 2025
Nanoparticle accumulation at tumor sites has been well reported in vivo, where targeting typically shows increased retention, but challenges remain for clinical translation. This work examines the effect of targeting ligand binding affinities and nanoparticle size on retention and transport through a solid tumor. We first show using cell affinity assays that modifying a wildtype (WT) anti-epidermal growth factor receptor (EGFR) affibody-enzyme fusion protein into a UV-photocrosslinkable (N23BP) version led to a significant decrease in affinity, whether as a free protein or as a conjugate to silica nanoparticles. Despite the reduced EGFR affinity, all protein conjugated nanoparticles showed binding and uptake to EGFR-overexpressing HTB9 bladder cancer cells as detected by confocal microscopy and flow cytometry. Next, transport studies of the protein conjugated nanoparticles using monoculture spheroids revealed that spheroid binding was higher for 17 nm particles bound with the WT proteins than N23BP, which was expected based on their respective KD values. However, the 17 nm particles conjugated with the photocrosslinkable N23BP affibody-enzymes showed an altered distribution profile that peaked further into the spheroid than the WT nanoparticle conjugates or in the absence of UV treatment. We correlate this finding with increased transport and retention of the photocrosslinked N23BP-nanoparticle conjugates in 3D spheroids to both the lower binding affinity of the affibodies for EGFR and the ability to introduce covalent linkages between the affibody and cell receptor. The larger 40 nm protein-conjugated nanoparticles showed limited penetration regardless of affinity or photocrosslinking on a 12 h timescale but did show overall increased transport after 24 h.
We previously demonstrated that photocrosslinking affibody-enzyme-nanoparticle complexes to CaCo2 colorectal cancer xenografts in mice led to inhibited tumor growth in the presence of prodrug administration.23 In said studies, ∼18 nm upconverting nanoparticles (UCNPs) were used to initiate crosslinking at clinically relevant wavelengths and the enzyme cytosine deaminase (CodA) was used for prodrug conversion. Despite the inhibited tumor growth, little information is known about the distribution of photocrosslinked, low affinity nanoparticle-affibody conjugates within the tumor. For the studies shown here, we first demonstrate methods to conjugate the EGFR binding affibody and affibody-enzyme fusions to ∼40 nm and ∼17 nm silica nanoparticles. Silica nanoparticles (SiNPs) were used in this study as a model for common silica-based functionalization of more complex nanoparticles like UCNPs. 17 nm SiNPs were chosen to have a size similar to the previous studies, while 40 nm particles were chosen as a larger group to analyze the impact of affinity alongside size. First, SiNPs were synthesized and bound with the wildtype (WT) and photocrosslinkable (N23BP) affibody-enzyme fusion proteins. Cell affinity assays were next run using the protein conjugated nanoparticles which showed highly disparate KD values ranging from the high nM for the WT-conjugated particles versus mid-to high μM for the N23BP affibody bound SiNPs. In comparing the protein conjugated 17 and 40 nm particles, a decrease in binding affinity was observed with the increase in particle size which may be due in part to the number of proteins bound to the differently sized SiNPs. The protein conjugated particles were next tested for 2D cell uptake against HTB9 bladder cancer cells by confocal microscopy, which showed significant binding and uptake regardless of affinity or particle size. Next, to measure transport in a tumor model, 3D HTB9 bladder cancer spheroids were formulated and reacted with the 17 and 40 nm WT and N23BP-affibody-enzyme modified SiNPs over 12–24 h. Analysis of confocal microscopy images was used to measure the binding and transport into the 3D spheroids. These conjugates demonstrated much higher binding for the 17 nm particles bound with the WT proteins as compared to N23BP, as expected based on their respective KD values. However, the 17 nm particles conjugated with the photocrosslinkable affibodies showed an altered diffusion profile upon UV irradiation, displaying greater distribution of retained particles within the spheroid. In studying the protein conjugated 40 nm SiNPs, the size barrier of the larger particles inhibited spheroid penetration regardless of affinity after 12 h of incubation, and there was minimal particle accumulation after 24 h compared to the 17 nm particles. All together, these results show the importance of optimizing particle size and affinity to enable maximum tumor penetration and accumulation in addition to the effects of photocrosslinking on nanoparticle diffusion profiles.
To study cellular interactions with nanoparticles conjugated with either the WT-CodA or N23BP-CodA, silica nanoparticles (SiNPs) were synthesized. As mentioned above, SiNPs were used due to the ease of large-scale synthesis and as a model for silica shell chemistry on nanoparticles such as UCNPs for use in vivo. For this, solid silica nanoparticles were synthesized using a sol gel process with an average particle diameter of ∼40 and ∼17 nm by TEM (Fig. 2a). The SiNPs were next modified with a functional polyethylene glycol (PEG) layer by reacting with a 1
:
5 ratio of PEG-silane-2k to DBCO-PEG-silane-2k in anhydrous toluene followed by a slow centrifuge to remove aggregates. After reaction, zeta potential measurements of the particles showed a substantial increase in surface potential toward the positive as compared to silica nanoparticles alone (Table S1†). To orient the affibody-enzyme from the particle surface, the SiNPs were further reacted with nitrilotriacetic acid-PEG-azide (NTA-PEG-azide-3.4k) followed by the addition of 10 mM Ni2+ and the C-terminal His-tagged WT-CodA or N23BP-CodA (Fig. 2b). To remove any weakly bound protein, the particles were washed with 5–20 mM imidazole to yield protein–particle conjugates that showed minimal protein release at pH values 5–7 (Fig. S2†). While dynamic light scattering (DLS) measurements indicated particle aggregation, results showed particles remained on the nanoscale at each modification step (Table S1†). The final conjugation yield for the ∼40 nm SiNPs were ∼4–5 proteins per particle whereas ∼17 nm SiNP had ∼1–2 proteins per particle.
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| Fig. 2 (Top) TEM images of as synthesized 40 nm (A) and 17 nm (B) SiNPs. (Bottom) SiNP modification and conjugation to affibody-CodA process. | ||
Next, cell affinity measurements were run to determine the binding of each affibody-CodA protein to EGFR-overexpressing HTB9 human bladder cancer cells to measure the affinity to cells.25,26 For this, 15
000 HTB9 cells were treated with the affibody enzymes alone at various concentrations ranging from 0.5–250 nM for 1 h followed by centrifugation to collect the cells and remove unbound protein. Flow cytometry was then used to determine the median fluorescence intensity, which was analyzed and fit to a one site binding model to determine the apparent dissociation constant KD (Fig. S3†). This procedure yielded a KD of ∼6 nM for WT-CodA and in the millimolar range for N23BP-CodA against HTB9 cells, suggesting the actual KD was greater than what could be accurately measured by this method.
In order to determine the apparent affinity of the affibody-CodA-SiNPs after particle conjugation, a similar procedure was done with the protein conjugated nanoparticles. Fluorescence analysis was used to determine the affibody-CodA loading on each particle sample, which were then incubated with HTB9 cells at protein concentrations that ranged from 0.1 to 50 nM and 0.1 to 400 nM for the 17 and 40 nm particles, respectively. These protein concentrations corresponded to ∼0.67–333 μg mL−1 and 1 μg mL−1–3.8 mg mL−1 particle mass concentrations, respectively. 50 nM protein was chosen as a cutoff for the smaller particles as the presence of aggregates began to skew flow cytometry readings beyond this concentration. As shown in Fig. 3, for the 17 and 40 nm WT-CodA-SiNP, taking the median fluorescence intensity for each concentration yielded a KD of ∼112 and ∼517 nM, respectively. It should be noted though that, as with many particle systems, aggregation occurs which can skew the absolute values obtained. In the data obtained, both the 17 nm and 40 nm SiNPs modified with N23BP-CodA showed weak affinity to cells in comparison to the 17 and 40 nm WT-CodA-SiNPs, again yielding KD values in the millimolar and beyond range. Based on the obtained values, it appears that the photocrosslinkable proteins conjugated to nanoparticles do not show stronger binding to EGFR expressing cells even though multivalency often increases association.27 As a comparison, dye labeled, PEGylated, SiNPs were used to analyze the binding profile of particles with no affinity. As shown in Fig. S4,† the non-targeted particles demonstrate a sharp uptick after 125 μg mL−1, which would correlate with ∼19 and ∼13 nM protein for the 17 and 40 nm affibody-CodA-SiNPs, respectively. This uptick is not present with the targeted nanoparticles. Instead, the targeted particles resemble either the early part of a binding curve in which receptor saturation has not yet significantly affected the curve (N23BP-CodA-SiNPs) or after receptor saturation begins to show (WT-CodA-SiNPs). It is important to note that, due to the differences in dye loading, the median fluorescence intensity values cannot be compared directly.
Next, particle uptake by HTB9 cells was verified via fluorescence microscopy using 2D cell cultures. HTB9 cells were treated with each affibody-CodA-SiNP conjugate for 24 h at 100 nM protein equivalent concentration before washing, nuclear staining, and imaging. As shown in Fig. 4, each protein-NP conjugate type was shown to associate and be uptaken by the HTB9 cells. Not unexpectedly, the 17 nm WT-CodA particles at the same concentration added to cells as the 40 nm showed larger amounts of particles bound (Fig. S5†). Despite the high KD values of the N23BP affibodies for the EGFR expressing cells, a significant number of the particles bound to cells could be detected, as further confirmed by analyzing the proportion of particle fluorescent area in comparison to total nuclear area as a proxy for cell count (Fig. S5†). Additionally, when incorporating DiI membrane stain, the particles appear to be associated with the cells (either by internalization or on the cell membrane) (Fig. S6†). This was irrespective of the fact that only 100 nM protein were added to cells although the roughly measured KD values for the N23BP proteins were in the micromolar range.
The ability of the WT and N23BP conjugated SiNPs to accumulate and diffuse in tumor microenvironments was determined next. For this, monoculture 3D spheroids were formed by incubating 20
000 HTB9 cells in polyHEMA coated 96 well plates for 72–96 h followed by characterization by widefield microscopy (Fig. S7†). Concurrently, the WT-CodA and N23BP-CodA proteins were modified with the Alexa Fluor 555 (AF555) dye prior to SiNP conjugation to track particle movement into the spheroids. AF555 was chosen to limit background autofluorescence often observed in cell imaging and to allow for greater spheroid light penetration. Spheroids were incubated with 250 nM of the AF555 labeled WT-CodA-SiNP and N23BP-CodA-SiNP for 12 h and 24 h, with UV irradiation occurring 4 h post particle treatment. They were then transferred to flat bottom imaging plates and fixed before nuclear staining and imaging. To analyze particle transport into spheroids, the Hoechst nuclear stain was used to create a mask around the entire spheroid. This mask was then eroded by 10 μm using the “imerode” MATLAB function to create a second mask which was subtracted from the first, creating a 10 μm slice on the outside of the spheroid. This process was continued to create a mask for every 10 μm slice until the center of the spheroid. For each slice, excessively bright aggregates were removed and the mean AF555 intensity was plotted against depth to yield a distribution profile.
As shown in Fig. 5, the 40 and 17 nm particles showed very different spheroid binding and penetration profiles as determined by tracking AF555 fluorescence. In each case, at 12 h post treatment, the WT-CodA-SiNPs showed overall higher binding throughout the spheroid in comparison to the photocrosslinkable affibody-nanoparticles, although this effect was only statistically significant for the 17 nm particles. Since the measured KD values of two different protein nanoparticle conjugates show multifold differences, an overall lower spheroid binding with the N23BP-CodA-SiNP conjugates is expected. Importantly, the 17 nm WT-CodA-SiNPs were able to accumulate past 70 μm from the edge of the spheroid, as shown by fluorescence detectable above background, suggesting that the high nM affinity was weak enough to still allow spheroid penetration at this particle size. Additionally, the WT-CodA-SiNPs showed greater accumulation for each depth up to 30 μm into the spheroid when compared to the crosslinked N23BP-CodA-SiNPs and up to 40 μm compared to the non-crosslinked N23BP-CodA-SiNPs (p < 0.05). For the N23BP-CodA-SiNPs, no statistical significance was obtained between the crosslinked and non-crosslinked groups. However, an altered penetration depth distribution profile was observed, as discussed further in Fig. 6 below. Regardless of affinity, the 40 nm protein conjugated nanoparticles showed little spheroid penetration, accumulating mostly on the periphery or having low overall binding, in comparison to the 17 nm particles (Fig. 5A and B). This result suggests that the size barrier of the 40 nm particles was enough to limit penetration on the 12 h timescale independent of affinity, while the 17 nm particles transported further after 12 h.
Incubating the spheroids with the affibody-enzyme-SiNP conjugates for 24 h revealed different trends (Fig. 5C and D). For the 40 nm particles, each particle set had traveled slightly deeper into the spheroids but showed low overall binding, even with the WT affibody. In the case of the 17 nm particles, the WT-CodA-SiNPs showed higher accumulation throughout the spheroid than the N23BP-CodA-SiNPs did (p < 0.1 at 30 and 80 μm depths). Similar to 12 h incubation, this result could be caused by the fact that the affinity is low enough where it serves to increase overall binding while still allowing some transportation into the spheroid.1 The 17 nm WT-CodA-SiNPs displayed their peak fluorescence closer to the edge of the spheroid as compared to the N23BP-CodA-SiNPs, which encouraged further observation of the distribution transport profiles.
Upon normalization of each group to its maximum fluorescence intensity, differences in transport became more evident for the 17 nm protein conjugated nanoparticles (WT-CodA-SiNP, N23BP-CodA-SiNP + UV, N23BP-CodA-SiNP − UV) (Fig. 6). First, at 12 h post treatment, the WT-CodA-SiNPs and the N23BP-CodA-SiNPs without UV irradiation showed similar trends. In both cases the mean fluorescence intensity peaked around 10 μm into the spheroid and decreased with further distance into the spheroid. However, with the photocrosslinked N23BP-CodA-SiNPs, the mean fluorescence intensity peaked around 20–40 μm into the spheroid, displaying a broader peak with a slower decline as depth increased. This unique profile was attributed to photocrosslinked particles being unable to exit the spheroid, leading to increased retention. As mentioned above, by 24 h post-treatment the low affinity N23BP-CodA-SiNPs had a distribution profile that peaked further into the spheroid than the WT-CodA-SiNPs did. This trend was evident with both the UV-treated and untreated particles and attributed to the lower affinity of the N23BP affibody reducing the binding site barrier impact. For the larger 40 nm protein-conjugated nanoparticles with 12 h of incubation, the WT-CodA-SiNPs peaked on the spheroid surface and the photocrosslinked particles peaked about 10 μm into the spheroid. In comparison, the non-crosslinked N23BP-CodA-SiNPs displayed a more uniform distribution profile, although this may be due to having a lower peak before normalization. Additionally, the 40 nm particles all showed peaks further into the spheroids after 24 h of incubation with limited surface bound particles. Only the particles with the strongest affinity (17 nm WT-CodA-SiNPs), had the fluorescence peak near the periphery of the spheroid.
500 rcf for 15 min and washed twice in ethanol. For smaller particle production, the temperature was increased to 70 °C and centrifugation was done for 1 h. Isolated particles were characterized by transmission electron microscopy, dynamic light scattering spectroscopy, and zeta potential measurements.
:
7.5 molar ratio overnight at 4 °C. Excess dye was removed with Pierce Dye Removal Columns. Degree of labeling was calculated following UV-vis spectroscopy.
000 HTB9 cells for 1 h at room temperature in PBS supplemented with 1% BSA and 0.1% sodium azide. The cells were then centrifuged at 150 rcf for 5 min and washed twice with ice cold BSA and sodium azide supplemented PBS. Cells were immediately analyzed via flow cytometry and characterized using median fluorescence intensity. The binding curve was used to calculate the apparent dissociation constant (KD) using a one site binding model using 0.1–400 nM for the 40 nm particles and 0.1–50 nM for the 17 nm particles. A similar process was used for the free affibody-enzymes using 0.5–250 nM protein. For the dye labeled SiNPs without affibody-enzymes, the same process was used with a 0.1–1000 μg mL−1 concentration range.
000 cells per well in 96 well flat bottom imaging plates and grown for 48 h. Cells were then treated with 100 nM affibody-enzyme-SiNP for 24 h. Following this, cells were washed 2× with DPBS, stained with 5 μM Hoechst nuclear stain and 3 μM DiI membrane stain for 20 min, washed 2×, and imaged in DPBS. ImageJ was used for analysis by determining total fluorescent area of Hoechst and Alexa Fluor 488.
000 cells per well and grown for 4 days. Following this, spheroids were treated with 250 nM of affibody-enzyme-SiNPs for 12 or 24 h. After 4 h of incubation, photocrosslinked samples were irradiated for 30 min with UV light to initiate crosslinking of the benzophenone group. After protein treatment, spheroids were transferred to 96 well flat bottom imaging plates, washed 1× with DPBS, and fixed with 4% paraformaldehyde for 30 min. They were then washed 1×, stained with 10 μM Hoechst nuclear stain for 30 min, washed 1×, and imaged in DPBS.
Image analysis was performed using a MATLAB script derived from Saemundsson et al.29 Briefly, TIF images were read and the nuclear channel was used to create a mask of the entire spheroid. This mask was then eroded by 10 μm using the “imerode” function to create a second mask which was subtracted from the first. This created a 10 μm slice on the outside of the spheroid. This process was continued to create a mask for every 10 μm slice until the center of the spheroid. For each slice, excessively bright aggregates were removed, background values were subtracted, and the mean Alexa Fluor 555 intensity was read and plotted against depth to yield a distribution profile. Student's t-test was used to determine statistical significance.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4na00823e |
| This journal is © The Royal Society of Chemistry 2025 |