Methods
We prepared a library of sixty-six complexes using the progesterone receptor (PR) ligand binding domain (LBD) obtained from PDB 1A28 . 21 Thirty-two steroidal ligands with potency ranging from inactive to high potency (Table S1) were inserted into the PR pocket in the same orientation as progesterone. Ligands and EC 50 values were identified from published literature. 30–32 An unliganded PR complex was also generated without ligand. All complexes were solvated in an octahedral box using TIP3P water with a 10-Å buffer around the protein complex. Na + and Cl − ions were introduced to neutralize the protein and achieve physiological conditions of 150 mM. All systems were set up using tleap in AmberTools20, part of Amber 2020 41 with the protein.ff14SB forcefield. 42,43 Parameters for the different ligands were obtained using Antechamber and the Generalized Amber ForceField GAFF) 44–46 in AmberTools 20. All minimizations and simulations were performed using Amber20 with GPU acceleration. 47,48 Complexes were minimized with 5000 steps of steepest decent followed by 5000 steps of conjugate gradient minimization with 100 kcal mol −1 Å −2 restraints on all atoms. Restraints were removed from all atoms excluding ligand atoms and the previous minimization was repeated. A final round of minimizations was performed with no restraints on any atoms. The complexes were heated from 0 to 300 K using a 100-ps run with constant volume periodic boundaries and 5 kcal mol −1 Å −2 restraints on all protein and ligand atoms. Equilibration was performed using a 10 ns-MD run with 10 kcal mol −1 Å −2 restraints on protein and ligand atoms using the NPT ensemble. A second 10-ns run was performed with weaker restraints of 1 kcal mol −1 Å −2 on both protein and ligand atoms, followed by a third 10-ns run with 1 kcal mol −1 Å −2 weak restraints kept only on ligand atoms. Finally, all restraints were removed, and triplicate 500 ns production simulations were obtained for each complex. A 2-fs timestep was used and all bonds between heavy atoms and hydrogens were fixed with the SHAKE algorithm. 49 A Langevin thermostat was used with a collision frequency of 1.0 ps −1 to control temperature, while the Berendsen barostat is used to maintain constant pressure. A cut-off distance of 10 Å was used to evaluate van der Waals forces and long-range electrostatics with Particle Mesh Ewald (PME).
Root mean square deviation (RMSD) values were calculated over all combined trajectories to assess stability and equilibration (Fig. S8, ESI † ). The ‘strip’ and ‘trajout’ commands of the CPPTRAJ module 50 were used to remove solvent atoms and extract 25 000 evenly spaced frames from each 500-ns simulation for analysis. For each complex, the three simulations were combined to generate 75 000 frames for analysis. Root mean square fluctuations (RMSF) analysis was performed using Cα atoms of protein residues, computed for each frame in the trajectory relative to the initial structure. The ‘hbond’ command in CPPTRAJ was used to identify and quantify all hydrogen bonds in trajectories. The ‘surf’ command was used to calculate the solvent-accessible surface area (SASA) of amino acids in the binding pocket. The ‘dist’ command was used to calculate the distances between all pairs of Cα atoms. To calculate binding free energies of ligands to PR, the MM-PBSA and MM-GBSA methods were utilized. 51 For SASA, distances and free energy analyses, we partitioned data by ligand class ( i.e. inactive, weak, moderate and high potency ligands) and used t -tests to determine whether the values for any given ligand class were significantly different (in both directions) from those of the other ligands.
The Network View plugin 52 in VMD 53 and the Carma program 54 were used to analyze contacts and produce dynamic networks for each system. 55 Residue contact maps were used to determine how dynamic contacts are altered across various complexes. To generate contact maps, protein residues are defined as nodes and edges (or contacts) are created between two non-neighboring nodes if the heavy atoms of the two residues are within 4.5 Å of each other for 75% of the trajectory. To produce dynamic networks, edges in residue contact maps were weighted by covariances calculated from MD simulations (following the protocol described in ref. 55 . Edge weights inversely proportional to the calculated pairwise correlation between the nodes. To identify groups of nodes with correlated motions, communities were generated from dynamic networks using the Girvan–Newman algorithm. 56 The ligand community was defined as the community containing the ligand.
Communication between the pairs of residues ( e.g. ligand and helix 12, ligand and binding pocket residues) was described by quantifying the shortest distance between these sites using the Floyd–Warshall algorithm. 57 For distant residues, a communication path is drawn as a chain comprised of nodes and edges that connect the two residues. Due to the inverse correlation between correlation and edge weights, the sum of edges along the path between two distant nodes becomes lower as the strength of communication ( i.e. , correlation) increases. Among all possible paths between the two residues, the shortest distance refers to the path for which the sum of edge weights is the lowest. Shortest distance is a unitless parameter that quantifies the sum of the edge weights. For closely located residues within contact of one another, the shortest distance is simply calculated as the length of the edge connecting the two nodes.
Results
Triplicate MD trajectories were obtained for each complex. Representative structures for simulations reveal that all ligands retain the same relative orientation and position within the PR binding pocket (Fig. S2, ESI † ). To reveal a relationship between dynamic traits observed in MD simulations and structural features of ligands, we ordered the ligand library by EC 50 and identified the most defining characteristics of each, focusing on the C3, C11, and C17 substituents on each steroid ( Fig. 1A and B ). Where applicable, C20 and C21 attached to the C17-β substituent were also considered. C17 substitutions are designated as ‘bulky’ if they have a minimum of two carbons, the only exception being promegestone (P0M) with a C17-α methyl, labeled ‘m’. Further, bulky substituents are labeled ‘c’ if they contain the C20-ketone and C21-hydroxyl group that is characteristic of corticosteroids. Also labeled are ligands containing an esterified substitution at C17-α (‘e’). This SAR quickly grouped our library into 3 classes designated ‘inactive’, ‘weak’ and ‘potent’ ligands, with distinguishing features consistent with previous reports. 33,34
Four of seven inactive ligands are C21 steroids, possessing the C17-β substituent with C20-ketone and C21-hydroxyl groups that is typical of corticosteroids. Glucocorticoids are known to not activate PR. 33 C17-α hydroxy substituents are also a trait of inactive ligands, found in five of seven ( Fig. 1A ). The last two inactive ligands are the only ones in our library with a C11-oxo substitution which may explain their inactivity. Weak ligands exhibit a less distinctive SAR. The weak class has the highest number of ligands with a C17-β hydroxyl (5/10). All ligands without a C17-β hydroxyl contain a bulky C17-β substituent and a C11–OH, with one exception: spironolactone (SNL). The defining feature of potent agonists is a bulky substituent at C17-α and/or C17-β positions with 15/15 having at least one and 8/15 possessing both. This SAR is consistent with reports that PR affinity and activity is optimized in ligands with bulky C17 substituents. 18,25
To compare how different ligands affect communication and coupling in PR complexes, we measured the ‘shortest distance’ between: (i) ligand and the activation function surface/AF-2, (ii) ligand and binding pocket residues. This metric uses covariances calculated between proximal amino acids to approximate the strength of communication (see Methods). Calculated from MD trajectories, shortest distance is inversely proportional to strength of communication between two residues.
First, we quantified communication between ligands and AF-2. The activation surface, i.e. , the coregulator binding site on the LBD, contains helix 12 ( Fig. 1C ). Helix 12 (H12) contains Glu911, a conserved residue that serves as a ‘charge clamp’, providing electrostatic stabilization for the LXXLL peptide fragment of coregulators bound at AF-2 ( Fig. 1C ). To quantify communication between ligands and AF-2, we measured the ‘shortest distance’ between the ligand and Glu911. In comparing shortest distances between active and inactive ligand classes, we did not observe significant differences ( Fig. 1D ). We further split active ligands into ‘weak’ and ‘high’ potency agonists, which also did not yield statistically significant differences. However, a close analysis revealed that the high potency class of agonists splits into two subgroups, subsequently designated as moderate and high potency ligands. Moderate potency agonists display significantly stronger coupling ( i.e. , lower shortest distance) with AF-2 ( Fig. 1E ). The five ligands in the moderate potency class all possess a hydroxyl group at C11 which is not observed in the majority of high potency ligands.
Next, we calculated shortest distances between ligands and the surrounding amino acids that comprise the binding pocket (subsequently referred to as binding pocket residues) ( Fig. 1F ), including residues on helices 3, 5, 7, 10, 12 as well as the loop between H11 and H12 (L11-12) and S1 β-strand. We observed that moderate potency ligands show significantly weaker communication (higher shortest distance) with H5 residues compared to high potency agonists. These moderate potency agonists also show stronger communication with H10 compared to other ligands. No significant differences were seen in shortest distances between ligands and other helices ( Fig. 1G ). This analysis suggests that moderate and high potency agonists induce different patterns of coupling within PR, possibly equating to distinct activation mechanisms between the two classes. Furthermore, the findings indicate that the distinction between the two classes involves varying modulation of H5 and/or H10.
To quantify the interaction between ligands and PR, we used MM-PBSA and MM-GBSA methods to calculate the binding energy of ligand binding from our trajectories. Because only interaction energies are calculated and entropy is not included, these values are not true free energies. Grouped by class, energies reveal a trend with potency, as inactive ligands have the highest binding energy while high potency agonists have the lowest energy ( Fig. 2A and Fig. S3, ESI † ). This result suggests that the potency of PR ligands is correlated with the strength of their interaction with PR. To further investigate this pattern, we performed solvent-accessible surface area (SASA) calculations to determine how ligands alter the local environment within the PR binding pocket. Simultaneously, we used energy decomposition to calculate the energetic contributions of the binding pocket residues to the energy of ligand binding. Binding energies are calculated using the MM-PBSA and MM-GBSA methods, followed by per-residue energy decomposition. We examined residues near the D-ring and A-ring ends of the steroids to determine how structural features of the four ligand classes influence SASA and binding energy contributions. All SASA values and binding energies are presented in table (Tables S2 and S3, ESI † ) and graph form (Fig. S4 and S5, ESI † ).
On the D-ring end, we examine Phe794, Leu797, Leu887, Cys891, Thr894, Val903, Phe905, Met909, Ile913 and Asn719 ( Fig. 2B ). Phe794 is the most exposed in weak agonists, with significantly higher SASA values (*, p < 0.05 by two-tailed, unpaired t -test) compared to moderate/high potency agonists ( Fig. 2C ). This results from the lower tendency of weak agonists to have substituents in the C17-α position ( Fig. 2A ). Conversely Phe794 is most buried in high potency agonists ( Fig. 2G ), resulting from the presence of bulky C17-α substituents. We then analyzed exposure of Asn719 on H3 which is physically close to L11–12 residues Val903 and Phe905. Asn719 is conserved in all oxosteroid receptors and forms hydrogen bonds with C21 and C17 and C11 hydroxyl groups. We observe lower SASA ( i.e. more buried) with weak agonists ( Fig. 3B ), suggesting that weak ligands induce a buried conformation around this H3 region and are most likely to interact with Asn719 via hydrogen bonding with C17 groups. We note that 8 of 10 weak ligands have a C17–OH (5 β, 3 α).
Non-polar L11–12 residues Val903 and Phe905 are positioned close to the C17-α and/or C17-β substituent, and reveal significantly higher SASA, more exposed, in moderate potency agonists ( Fig. 2D ). Interestingly, Ile913 located on H12, more distant from the D-ring, shows similar SASA trends to Val903/Phe905, suggesting that these residues form fewer contacts with surrounding residues in moderate potency ligand complexes. This exposure of Val903, Phe905, and Ile913 stabilizes ligand binding, as two of these residues (Val903, Ile913) make higher binding energy contributions in moderate potency agonist complexes than other ligands ( Fig. 2E and F ). We observed that Thr894 (H10) and Leu797 (H7) also contribute significantly to stabilizing moderate agonist complexes ( Fig. 2E ). These combined results suggest that moderate potency agonists are uniquely stabilized by the AF-2 and pre-AF-2 regions of PR.
On the A-ring end, we examine Met756, Leu763, Arg766 (all on H5), and Phe778 (S1/S2), with sidechains close to the A/B steroidal rings. Met756 has the highest SASA in moderate potency agonist complexes ( Fig. 2D ). It is difficult to identify a structural rationale for this observation as Met756 is close to the C19 methyl group which is present in 24 of 33 ligands. However, this observation suggests that separate events may cause a repositioning of moderate agonists in the binding pocket, contributing to a less hydrophobic environment on the β face. Forming a cavity around the A-ring, Leu763 and Phe778 have significantly higher SASA in moderate agonists but are buried in high potency agonists.
Arg766 (H5) is conserved in steroid receptors and positioned to interact with the C3 atom of the A-ring. We observe lower SASA for Arg766 in high potency ligand complexes ( Fig. 2G ) and higher SASA in weak agonist complexes ( Fig. 2C ). In addition, Arg766 contributes favorably to the binding energy of high potency ligands ( Fig. 2H ), suggesting a direct interaction that confers stabilization to the potent agonists. In summary, the SASA and energy decomposition produces some expected findings, such as a clear distinction around the D-ring between high potency and weak agonists based on C17-α substitution. Moreover, four unexpected predictions emerge from this analysis: (i) moderate agonists are uniquely stabilized by the AF-2 and L11–12 region, (ii) weak agonists have higher burial of Asn719 (H3), possibly equating to stronger interaction with this conserved residue, and (iii) moderate agonists appear to be repositioned in the pocket, evidenced by distinct H5 interactions, and (iv) high potency ligands are uniquely stabilized around the A-ring. A comparison of representative structures from each ligand class reveals a reorientation in the moderate potency ligand (BUD) that is absent with other classes ( Fig. 2I ), providing support for the observations made from binding pocket environment analysis.
To determine whether functional profiles of ligands influence specific inter-residue interactions across the receptor, we calculated the average distance between every pair of Cα atoms. Distances between residues 705–716 (Loop1–3 and H3) and 890–904 (H10, H11, Loop11–12) are significantly longer in moderate agonists and shorter in weak complexes ( Fig. 3A and B ). This result is particularly striking because the distance between H11 and H3 was previously identified in GR 35 and ERα 36 as a predictor of functional effects of ligands.
To understand the origin of the trends observed in H11–H3 distances, we identified all hydrogen bonds and compared their occupancies between PR complexes. We identified 8 hydrogen bonds that show significant differences in occupancy between ligand classes (Table S4, ESI † ). Of these, the highest occupancy is between Glu904–Asn719, present in weak agonist complexes ( Fig. 3C ). We also observe a hydrogen bond between Leu901–Ser712 in weak agonist complexes ( Fig. 3D ). Both hydrogen bonds link H3 to the H11/Loop11–12 region of PR, consistent with the shorter Cα–Cα distances observed between H3 and H11 residues in weak complexes ( Fig. 3C ). Both display significantly reduced occupancy in moderate potency complexes.
This Asn719–Glu904 hydrogen bond is observed in the PR crystal structure, hypothesized to be important for correctly positioning of H12. 26 A similar role is proposed for the equivalent Asn residues in AR, MR and GR. 27,28,37 This stabilization is believed to play a role in activation of steroid receptors but may be less relevant in PR due to the reduced importance of Asn719. Thus, our simulations suggest that weak ligands (with C17-α OH group) are most likely to coopt this vestigealized mechanism to mediate the stabilizing interaction between Asn719 on H3 and L11–12. This conclusion is consistent with the low SASA observed in Asn719 in weak agonists ( Fig. 2C ), suggesting higher levels of Asn719 hydrogen bonding. To further investigate the behavior of Asn719 in PR complexes, we examined the interactions between Asn719 and residues within van der Waals contact. We determined that interactions between Asn719 and H11/H12 tend to be highest in weak potency ligands, supporting the notion that weak ligands pull H3 and H11/H12 closer ( Fig. 3E ).
Conversely, the opposite effect is observed in moderate potency ligands. These ligands reduce interactions between Asn719 and H11/H12, measured by distances ( Fig. 3A ), hydrogen bond occupancy (Table S4, ESI † ) and van der Waals interactions ( Fig. 3E ). We hypothesize that this unexpected behavior may result from the C11–OH group and which is a characteristic of this ligand class. To test this hypothesis that the C11 hydroxyl group forms unique interactions, we characterized hydrogen bonding between all ligands and Asn719, specifically C11, C17 (α and β) or C21 hydroxyl groups ( Fig. 3F ). Of all ligands, moderate potency ligands have the highest hydrogen bonding levels (50% and higher) between C11 and Asn719. While some inactive and weak ligands also use the C11–OH for Asn719 hydrogen bonding, these interactions are less frequent (25% and lower). Instead, weak agonists have a higher propensity to interact with Asn719 via C17–OH (50% and higher), while inactive and high potency ligands form C17–OH hydrogen bonds to a lesser extent. These patterns indicate that Asn719 will preferentially interact with C17–OH of PR ligands and in their absence, with the C11–OH. The hydrogen bond with C11–OH is suboptimal and is unable to stabilize the interaction between H3 and H11/H12. Thus, our findings suggest that the unique behavior of moderately potent agonists with Asn719 can be attributed to both the presence of the C11–OH and absence of a C17–OH. We summarize the hydrogen bonding behavior of each class using representative ligands ZK5, DHT, BUD and P0M respectively ( Fig. 3G ).
Finally, our studies draw a strong distinction between high potency PR agonists and the moderate/weak agonists. High potency agonists function independently of Asn719, as the receptor has evolved a new optimal method for ligand recognition. Conversely, moderate and weak ligand classes both function in relation to Asn719. Moderate ligands have bulky D-ring substitutions that allow for potent PR activation, but display weaker activity than high potency ligands because of the C11–OH, which introduces evolutionary pressure on ligands to revert to the ancient Asn719-dependent activation. Weak ligands generally lack bulky C17-α substituents which makes them incapable of potently activating PR. Their weak activity results from the presence of a C17-β OH group which recognizes Asn719 and stimulates the ancestral steroid receptor activation mechanism. For the handful of weak ligands without a C17-β OH ( e.g. HCY, BLX, BM0, Fig. 2A ), we note that these tend to also have a C11–OH and/or C17α-OH without a bulky C17-α substituent, suggesting that their weak activity also can be directly linked to activation via Asn719.
Analyses of our MD simulations suggest that mechanisms of PR modulation differ among the ligand classes proposed in this study. To clarify the role of specific amino acids in mediating ligand activity, we combined mutagenesis studies with luciferase reporter-based transactivation assays ( Fig. 3H and I , full data is shown in Fig. S6 and S7, ESI † ). We tested the effect of reducing the hydrophobicity around C17 by individually mutating H3 residues Leu715 and Leu718 to both alanine and serine in vitro . We also tested the effect of mutating Met756 (H5), Phe778 (S1/S2), Thr894 (H10) and Met909 (H12) to alanine. All residues are in the binding pocket and from our MD analyses determined to be important in mediating activity profiles of the various ligand classes. Thus, we hypothesized that responses to PR mutations would differ by ligand class. While we observe some patterns within classes, an unexpected result was that ligands tended to display the same effects across all mutations. This was observed at both low and high ligand concentrations.
In inactive ligands prednisone (PDN) and dexamethasone (DEX), the response was lowered below DMSO control by most mutations as compared to wild-type PR. At higher concentrations, prednisone displayed additional reduction. Weak ligands showed a more variable response. At 1 μM ligand, three out of four ligands showed no significant change in activity for most mutants. At 10 μM, cortisol (HCY), dihydrotestosterone (DHT), and aldosterone (AS4) tended to show reduced activity while estradiol (EST) shows an increase for 5 out of 8 mutations studied. Moderate potency agonist triamcinolone acetonide (1TA) showed increased activity for all mutations while budesonide (BUD) showed either increased or diminished responses. Activity of high potency agonists progesterone (STR) and medroxyprogesterone (MP0) were lowered in all mutants while mometasone furoate (MOF) had more variable responses. Overall, ligand classes reveal similarities, particularly at the low dose, that support our general hypothesis that structural features common to a ligand class will drive similar functional responses to mutations. However, the mutagenesis studies do not provide strong support for the notion of specific amino acids differentially mediating activity of these ligand classes. Instead, by reducing hydrophobicity in the pocket, all mutations regardless of identity tend to confer a similar, ligand-dependent effect resulting in increase, decrease or no change in response.
Conclusion
Ligands targeting PR have therapeutic potential for several women's health ailments. By understanding the molecular features that drive or inhibit potency in PR ligands, we may gain insight that enables the design of new ligands. In this work, we have focused on using MD simulations to learn how steroidal ligands of varying activity levels modulate PR dynamics. We assembled a group of inactive, weak, and potent PR agonists and examined dynamics, intra-receptor communication, binding pocket environment and energetics in PR complexes. Using correlations calculated from MD trajectories, we predicted the strength of communication between ligands, surrounding residues, and AF-2. Patterns observed in our analysis split the group of potent agonists into moderate and high potency ligands, generating four ligand classes.
Steroidal ligands were modeled into the agonist-bound PR conformation where H12 is docked against H3 and H4, allowing the formation of a coactivator binding site. Conventional models of nuclear receptor activation suggest that this conformation is not supported in an unliganded or antagonist-bound state. 38 As such, the inactive ligand complexes in this study may not represent conformational states that are physiologically plausible. This observation may explain why our MD simulations reveal very few dynamic features that accompany and/or explain the phenotype of the inactive ligand class. Two observations of note were made. First, calculated binding free energies were significantly higher in inactive ligands than other agonists, consistent with published findings that bulky C17-α substituents increase both binding affinity and activity over the C17-α OH substitution that characterizes 5 out of 7 inactive ligands in this study. Second, we do not observe any conformational effects ( e.g. , unfolding, or increased fluctuations) at AF-2, even in inactive ligand complexes on the timescales of these simulations. This is consistent with prior simulation studies which observed large AF-2 fluctuations only when the antagonistic X-ray structure was modeled. 24
Our simulations reveal that weak ligands activate PR by coopting a defunct steroid receptor mechanism involving conserved H3 residue, Asn719 ( Fig. 4 ). Along with Val903 and Met909 on L11–12 and H12 respectively, Asn719 was most buried in weak complexes, suggesting that these ligands push H3 and L11–12 close together. This claim is supported by both interhelical distances and hydrogen bond analyses. Weak agonists also tend to contain a hydroxyl at C17 which is ideally positioned to engage the C
Created by potrace 1.16, written by Peter Selinger 2001-2019
O of the Asn719 sidechain in a hydrogen bond ( Fig. 3F ). Concurrently, the amide N interacts with and stabilizes the pre-H12 loop and the AF-2 by extension. This mechanism is observed in other oxosteroid receptors and likely existed in their ancestor, but was lost during PR evolution (summarized in Fig. 4 ).
Instead, the hydrophobic nature of the PR pocket favors ligands with bulky substituents at C17, which characterizes the majority of moderate and high potency ligands in this study. However these two classes reveal dynamic differences which appear to be meditated by the presence of a C11 hydroxyl group that attenuates activity of moderate ligands. Specifically, because they tend to lack an OH group at C17, moderate potency ligands engage in hydrogen bonding with Asn719 via the C11–OH, causing a reorientation of the steroids in the ligand binding pocket, and several effects observed in simulations, including destabilizing the interaction between H3 and H11/H12. High potency ligands are also less likely to form hydrogen bonds with Asn719, confirming that evolution has shaped PR to prefer nonpolar interactions over polar contacts with Asn719. Interestingly, while the Asn719 hydrogen bond with C11–OH is deleterious for PR activity, this interaction improves activity in MR ligands. 39 Additionally, GR and MR ligands ( i.e. corticosteroids) which are all C11-hydroxylated strongly activate the oxosteroid ancestor, 29 suggesting that C11–OH was historically beneficial for steroid receptor activation ( Fig. 4 ). Evolution altered this relationship in the PR/AR lineage, making the C11–OH in steroids detrimental for activity.
In summary, our simulation study reveals that steroidal ligands bound to PR trigger different activation mechanisms, which we unravel by monitoring dynamic signatures. We show that while PR has evolved new preferences for responding to ligand signals, it retains vestiges of a defunct activation mechanism that can be turned on by ligands with the appropriate molecular structure, i.e. a C17 (preferentially β) hydroxyl group that can hydrogen bond with Asn719. Because this mechanism is evolutionarily obsolete, this activity is weak at best. Additionally, when ligand structures enable them to incorporate both the ancestral and extant PR mechanisms, frustration arises leading to attenuated activation, as in the case of moderate potency ligands compared to high potency ligands. We note that the conclusions achieved here would not be possibly by crystallographic studies alone. While they might show the existence of a hydrogen bond in a structure, X-ray structures are limited for quantifying the occupancy of these interactions, which is one of the key results for distinguishing the between PR dynamics of weak and moderate agonists. These results may inform rational drug design strategies, as PR agonism can be modulated by designing ligands to target specific activation mechanisms. Because several aspects of nuclear receptor activation are conserved, it is possible that similar mechanistic features observed in PR might apply to other receptors.
Finally, we note that evolution does not explain all PR activation differences observed in these ligand classes, such as the effect of the A-ring. We observe that our ligand classes exhibit differences around the A-ring which clearly influence activity. Indeed, PR activation studies show that a double bond added into the A-ring of 11β-hydroxydihydroprogesterone (11βOHDHP4) significantly increases activity. 40 Additionally, we have not accounted for full versus partial agonistic activity of the ligands here, as we have focused solely on EC 50 values. Further work will be required to determine whether there is an evolutionary basis for partial agonistic activity reported for steroidal PR ligands.
Experimental
The plasmid containing full-length PR-B receptor (pcDNA3.0-PRB) was purchased from Addgene, USA. The DNA encoding PR hinge and LBD region (632–933) (UniProt ID: P06401 ) was PCR amplified using a combination of primers: 5′TATAGAATTCATGGTCCTTGGAGGTCGA-3′ and 5′-TATAAGATCTTCACTTTTTATGAAAGAGAAGG-3′ with 5′- E coRI and 3′- B glII restriction enzyme sites, respectively. The enzyme-digested PCR insert was cloned in-frame with DBD of pSG5-Gal4-DBD vector with the same restriction sites. This vector (pSG5-Gal4-DBD-PR) was used later as a template to generate different LBD mutants by PCR-based site-directed mutagenesis.
The following primers used for the mutagenesis reactions:
All mutants were confirmed by DNA sequencing. The hormone-dependent transcription activity of wild-type progesterone receptor and its mutants was assayed in the luciferase reporter system. HeLa cells were grown and maintained in phenol red-free medium MEM-α supplemented with 10% charcoal-dextran stripped FBS. The cells were seeded in 96-well plates at 90% confluency (8000–10 000 cells per well) and co-transfected with 50 ng 9x-UAS firefly luciferase reporter, 1 ng Renilla (pRL-SV40), and 5 ng wild-type progesterone receptor (pSG5-Gal4-DBD-PR) or mutant receptor plasmids using FuGene HD (Promega). Twenty-four hours after transfection, cells were treated with DMSO or selected ligands at two different concentrations (1 μM and 10 μM). Firefly and Renilla luciferase activities were measured 24 hours after ligand treatment using the Dual-Glo kit (Promega) using Spectramax iD5 plate reader. Firefly readings normalized over renilla for transfection efficiency check. The graphs were plotted as mutant versus wild type which were already normalized over DMSO.
Introduction
The progesterone receptor (PR) belongs to the nuclear receptor superfamily of ligand-regulated transcription factors which regulates a plethora of biological processes such as development, metabolism, reproduction, and inflammation upon binding of cognate ligands. 1–5 In association with estrogen receptor (ER), PR functions as a primary regulator of female development and reproduction. 6,7 Target genes of PR are important in normal breast development, 8,9 embryo attachment, and uterine decidualization in pregnancy 10,11 as well as other functions related to menstruation and the endometrium. 12,13 In addition to direct roles in breast cancer, 8,14 PR signaling is implicated in uterine diseases such as endometrial cancer, endometriosis, and leiomyoma. 15–17 Therefore, targeting PR transcriptional activity and signaling is a widely accepted and promising therapeutic approach for many diseases.
The transcriptional function of PR is initiated by progesterone binding in the hydrophobic binding pocket of the moderately conserved ligand binding domain (LBD). The binding of progesterone and other steroidal ligands is mediated by substituents on the four-ring steroid scaffold. These pharmacophores lead to distinct interactions with surrounding amino acid residues, allowing for diverse and ligand-specific functional modulation of PR. For example, a small modification to steroid hormones, such as C17-α acetylation or 19 nor-substitution, increases both ligand binding affinity and transcriptional activity in PR. 12,18,19 C11-β substituents permit selective PR modulation by differential stabilization of helix 12 (H12); 20 this mechanism is observed in ulipristal acetate, a selective PR modulator with a bulky dimethyl-amino phenyl group at C11. 19
Previous PR studies identify several LBD residues that are crucial for ligand recognition, including Arg766 on H5 which is conserved across steroid receptors, as well as Gln725 on H3, Met908 and Met909 on H12, and Cys891 and Thr894 on H10 (ref. 20–25 ). A unique feature of PR is the behavior of Asn719, a conserved helix 3 (H3) residue. In all other oxosteroid receptors ( i.e. androgen, glucocorticoid and mineralocorticoid receptors), Asn719 forms hydrogen bonds with the cognate ligands which have been shown by mutagenesis to be crucial for activation (ref. 26 and 27 ). This interaction is missing in the PR-progesterone complex, and mutation of Asn719 only has a minor effect on progesterone activity, indicating its lesser role in PR. 26 Conversely, introducing N705A into AR causes the receptor to behave like PR, increasing its preference for progestins. 28 The interaction between ligand and Asn719 also exists in the oxosteroid ancestor AncSR2, 29 which suggests that PR diverged from its ancestor, evolving a mechanism to exclude Asn719 in steroid hormone activation. In this work, we aim to gain a mechanistic understanding of how diverse steroidal ligands activate PR by investigating how they impact PR dynamics.
While the plasticity of the PR binding pocket and its ability to accommodate ligands of various sizes is documented, 18 there is poor understanding of how ligands modulate PR dynamics to achieve distinct transcriptional profiles. Molecular dynamics (MD) simulations are a valuable tool for studying ligand effects on the conformational dynamics of proteins. Here, we use MD simulations to investigate the dynamic behavior of ligand-bound PR complexes. We have assembled a library of 33 steroidal ligands (Fig. S1 and Table S1, ESI † ) with reported EC 50 values ranging from 0.1 nM–1000 μM. 30–32 Ligands were classified by potency as inactive (EC 50 > 10 μM), weak (10 μM to 1 nM) or high (<1 nM). All reported EC 50 values are obtained from cellular transcriptional assays in dose–response format. Our structure–activity relationship (SAR) analysis revealed that C11-hydroxylation of high potency agonists weakens EC 50 , defining a 4th class of ‘moderate’ potency ligands ( i.e. 1 nM–10 nM vs. <1 nM). We analyzed dynamics, protein–ligand interactions, binding free energies and solvent accessibility within the binding pocket. Our studies reveal that while high potency PR ligands activate independently of Asn719, this residue drives the activity of both weak and moderate potency ligands via two distinct mechanisms. By forming a hydrogen bond with C17–OH substituents, weak ligands coopt the ancestral steroid receptor mechanism to achieve weak activity in PR. Conversely, hydrogen-bonding between C11-hydroxyl and Asn719 repositions ligands in the pocket, reducing the activity of moderate-potency ligands relative to high potency steroids. Our research demonstrates multiple activation mechanisms in PR, including a residual, diminished mode of activation triggered by C17-hydroxylated steroids. We also reveal the dual role of Asn719 in facilitating and impeding activation, underscoring its pivotal significance in the design of PR ligands.
Coi Statement
There are no conflicts to declare.
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