2.1. Conceptual Framework
The relationship between the intrinsic cooperativity α and the apparent cooperativity can be compared to the relationship between mass and weight, which is why we could call weight also “apparent mass”. Mass is an absolute and intrinsic property of objects and is always the same regardless of the environment, although—like all absolute values—it is difficult to measure. Much easier to measure is weight—a relative value—which represents the effect of an object’s mass under certain experimental conditions. Similarly, the apparent cooperativity is the effect of an underlying absolute, intrinsic cooperativity α concealed by specific experimental conditions, i.e., the applied protein concentrations, more specifically, the ratio of target and chaperone protein concentrations relative to the corresponding
KC,1 and
KT,1 values (
Figure 1). Since the apparent cooperativity is the quotient of two EC
50 values and the intrinsic cooperativity α is the quotient of two
Kd values (Equation (1)), the difference between apparent and intrinsic cooperativity α is the result of the difference in EC
50 and
Kd values. The EC
50 value describes the resulting effect of the underlying absolute and intrinsic affinity of a ligand to a protein, i.e., the
Kd value adjusted by the applied protein concentration, and refers to the applied ligand concentration ([L
tot]) required to achieve 50% of this effect. For this reason, EC
50 values could also be referred to as “apparent
Kd”. In contrast, the
Kd is an absolute intrinsic property of a protein–ligand pair and, hence, independent of the experimental conditions and always refers to concentrations in free ligand, [L].
In our previous publication, we presented a simulation tool that enabled the determination of the cooperativity α by iteratively comparing the experimentally measured EC
50 value with the calculated EC
50 value of the %T
bound, ternary curve. Specifically, it was determined by matching given [L
tot] of the %T
bound, ternary curve and a numerically estimated [L
tot] constrained on [L] = [L
tot] − [CL] − [TL] − [CLT]. To calculate the concentrations of CL, TL and CLT on the basis of [L], the corresponding algebraic expressions are used [
29]. The above-mentioned general model covers ternary complex-forming compounds ranging from bifunctional compounds to pseudo molecular glues type I, which have one known binary binding affinity for one protein and an estimated weak to very weak affinity for the second protein. The model assumes that these measured (and estimated)
Kd values for
KC,1 and
KT,1 are available to calculate concentration values for CL, TL and CLT as a function of L
tot at equilibrium. The case of an infinite weak binding of the molecular glue to one of the two binding partners (molecular glue type II) and the case of an infinite weak binding to both proteins but an intrinsic and significant affinity of the two proteins to each other (molecular glue type III) requires additional mathematical constraints and will be discussed elsewhere (see [
29] for definitions of molecular glues type I–III).
Molecular glues have very different binary affinities for the chaperone (
KC,1) and the target protein (
KT,1). A typical pattern is a high affinity for the chaperone (C) and a very weak or even unmeasurable affinity for the target protein (T), which makes the measurement of the intrinsic cooperativity α a challenge and pushes the above-mentioned model to its limits. When it is possible to measure the
Kd referring to the weak affinity, the different affinities for the chaperone and the target protein result in very different apparent cooperativity values depending on whether the EC
50 shifts are measured through the weaker or the stronger binding protein, although the underlying intrinsic cooperativity α is the same for the experiments in both directions. The weaker the binary affinity of the molecular glue L to the monitoring protein (e.g., target T) and the higher the underlying cooperativity α, the greater the EC
50 shift in the %T
bound, ternary = ([TL] + [CLT])/[T
tot]·100% curve in the presence of the stronger binding counter protein C compared to the same binding experiments in the absence of the counter protein (%T
bound, binary = [TL]/[T
tot]·100%. Conversely, the stronger the intrinsic binary affinity of the molecular glue L to the monitoring chaperone protein C, the smaller the EC
50 shifts due to the presence of the weaker binding counter protein, even if the underlying intrinsic cooperativity α is very high [
29]. Consequently, the measurement of cooperativity by the stronger binding protein C can become difficult for low
KC,1 values as the binding assay cannot distinguish between the strong intrinsic binary ligand binding and the even stronger ternary binding caused by the presence of the counter protein T. In other words, the assay is bottoming out and would require lowering the concentration of the monitored protein C, which is often not possible for sensitivity reasons. Monitoring binary versus ternary binding by the weaker binding protein, therefore, results in a much better signal-to-noise ratio for the EC
50 shift, leading directly to more accurate and significant values for apparent cooperativity and, ultimately, the cooperativity α. But, as mentioned above, the challenge is often to accurately measure the weak affinity.
If the development of an binding assay for the weaker binding protein T is feasible, for instance, for values as high as 100,000 nM, the determination of a missing, very weak
KT,1 is possible from the %T
bound, ternary curve, which represents under the excess of protein C (e.g., [C
tot] = 10,000 nM)
KT,2. If the ternary complex formation has sufficient intrinsic cooperativity α, the EC
50 value of the corresponding %T
bound, ternary curve should then shift into the assay window for EC
50 values of less than 100,000 nM and be easily measurable. In such case, the developed mathematical model that requires input values for C
tot, T
tot,
KC,1,
KT,1 and α to output ternary complex concentrations [CLT] =
(C
tot, T
tot,
KC,1,
K,
T,1, α) for all cooperativity values α has to be adjusted. According to Equation (1), the missing
KT,1 has to be replaced by
KT,2·α to iteratively match the EC
50 of the %C
bound, ternary curve:
In this case, however, the EC50 shift corresponding to the stronger binding protein C derived from the %Cbound, binary to the %Cbound, ternary curve is required, which is difficult, if KC,1 is already very low. If KC,1 is sufficiently above the monitored protein C, using KT,2 instead of unmeasurable KT,1 is a feasible alternative.
Another advantage of assessing cooperativity through the weaker binding protein is that under specific conditions, the EC
50 value of the ternary binding experiment corresponds directly to the
Kd of the ternary complex formation following the corresponding CL formation (
KT,2). In such cases, assuming that the corresponding binary
KT,1 (which would be necessary to inform the mathematical model requiring both
Kd values) is available, the obtained apparent cooperativity naturally coincides with the intrinsic cooperativity α. Moreover, if such conditions can be identified and are experimentally feasible, the binding assay to the stronger binding protein C is not required and the intrinsic cooperativity α can be determined experimentally by monitoring the binding of a single binding assay only, which relaxes the previously stated requirement of measuring two binary
Kds (
KC,1,
KT,2) [
29].
The law of pathway independence states that both ternary complex-forming pathways—the one via CL and the one via TL—result in the same free energy difference between the ternary complex CLT and the sum of the three free species. Consequently, the cooperativity α is the same in both pathways and can, therefore, be derived from each pathway alone (Equation (1)). In other words, the degree to which the presence of T facilitates the ligand binding to C is the same as for the binding of ligand to T in the presence of C relative to the corresponding binary binding. The practical consequence is that the intrinsic cooperativity α can be measured by monitoring the binary and ternary ligand binding to only one of the proteins (T or C) without the use of a mathematical model. The counter protein must be present and controlled with respect to concentration, but no additional binding assay with the counter protein is required.
The problem of retrieving the cooperativity α from a single binding assay is grounded on the question under which conditions the EC50s of the %Tbound, binary and %Tbound, ternary curves correspond to KT,1 and KT,2, respectively. More generally, this question can be seen in the context of the difference between EC50 and Kd regardless of whether it is a binary or a ternary experiment.
In a binary binding experiment,
KT,1 corresponds to the concentration of free ligand L ([L]) at the binary inflection point [T] = [TL]:
Similarly, at the ternary inflection point, i.e., when [T] = [CLT],
KT,2 corresponds to the concentration of the pre-formed chaperon–ligand complex CL ([CL]):
In contrast to the Kds, the EC50 values corresponding to the inflection points of the binary and ternary %Tbound curves never coincide with the concentrations of free ligand L ([L]) nor of [CL] but match the concentrations of the total ligand [Ltot] applied. Specifically, for the binary binding, this means that the EC50 value directly corresponds to [L] only if [Ltot] is equal to [L]. Alternatively, a mathematical relationship between [Ltot] and [L], i.e., the EC50 value of the %Tbound, binary curve and the universal KT,1, which is independent of the applied total concentration of the target protein [Ttot], would need to be established such that KT,1 = EC50, Ltot, Ttot). The same applies to the ternary binding event. Either there are conditions under which the EC50 value of the %Tbound, ternary matches KT,2 so it can be directly read off the assay data, or a mathematical relationship must be established such that KT,2 can be derived from the EC50 value of the %Tbound, ternary curve, i.e., KT,2 = (EC50, Ltot, Ttot). The minimal benefit is that this mathematical relationship guides the selection of conditions under which the EC50 value matches Kd so that the cooperativity α can be derived directly from the apparent cooperativities from single binding assay data.
In our previous publication [
29], we demonstrated by simulated binding curves that apparent cooperativity values measured through the weaker binding protein are closer to the intrinsic cooperativity α than those measured by the stronger binding protein. Here, we specify the exact conditions under which apparent cooperativity measured by the weaker binding protein matches the cooperativity α. Even if only one—namely, the weaker binding protein—and not two binding assays are required, the counter protein, as such, must be available for the ternary binding experiment, but not as a binary binding assay. This can be a significant advantage in a drug discovery program. One potential obstacle to develop a binary binding assay for the stronger binding protein is the lack of a suitable position for the installation of the tag that reports the binding. Ideally, it should be close to the binding site, but not too close, which is not always possible. An alternative to monitoring binding indirectly is a competitive binding assay with a tag attached to a tracer ligand. However, if the affinity of the tracer ligand is too high, the dynamic range of the assay suffers, which often leads low signal-to-noise ratios. Finally, it is simply less time-consuming and more efficient to determine the intrinsic cooperativity α from only one binding assay than from two, even more so, if the final result is the same.
In the following sections, we discuss three experimental parameters that determine the range in which the EC50 value of a ternary binding experiment (from the %Tbound, ternary curve) coincides with the ternary Kd KT,2. If, additionally, KT,1 can be measured, the observed apparent cooperativity then coincides with the intrinsic cooperativity α. The three decisive parameters are (1) the influence of the excess concentration of the stronger binding counter protein, (2) the role of the concentration of the monitored weaker binding protein, and (3) the influence of lower KT,1 on saturation conditions.
The influence of the concentration of the stronger binding protein: Measuring ligand binding by monitoring only the changes in the protein to which the ligand binds, so-called target engagement assays, allows a direct comparison between binary and ternary binding experiments through the presence of the counter protein, which is usually unlabeled. The presence of the counter protein causes—in cooperative systems, i.e., with α > 1—additional interactions that only occur in the ternary complex, leading to enhanced ligand binding. The assay quantifies this by shifts of the EC50 value in the binding curve in the absence (%Tbound, binary) and in the presence of the counter protein (%Tbound, ternary). The underlying reason for this EC50 shift in the %Tbound, ternary curve is a lower Kd of the ligand in the presence of the counter protein. The intrinsic cooperativity α is defined as the ratio of the binary and the ternary Kd, KT,1 and KT,2, respectively. For intrinsic cooperativities greater than 1, the ligand is bound more tightly in the presence of the counter protein. In the absence of cooperativity (α = 1), the EC50 values of the binary and ternary binding curves are identical, and the ligand is not bound more tightly to the target in the presence of the chaperone (Equation (1)). This holds regardless of whether ternary complex formation takes place or not. Moreover, this means that a target engagement assay can only detect ternary complex-forming compounds that exhibit intrinsic cooperativity, i.e., α > 1 or α < 1. For non-cooperative compounds (α = 1), an assay that detects the compound-dependent induced proximity of the two proteins is required to demonstrate ternary complex formation.
If the EC50 value of a ternary binding experiment in a target engagement assay (%Tbound, ternary curve) coincides with KT,2, no binding events other than the recruitment of CL to T are expected at equilibrium (Equation (3)). In principle, with species C, T and L, three bindings with T are possible in equilibrium:
T + L ⟶ TL;
TL + C ⟶ TLC;
T + CL ⟶ CLT.
If the experimental conditions are such that contributions from the binding events of (1) and (2) are practically negligible, the measured EC50 of the %Tbound curve exclusively represents the binding event described by (3) and, thus, describes the equilibrium in Equation (3). Such conditions can be enforced by a high concentration of the stronger binding counter protein, in this example, of chaperone C. Since we assume a weak affinity of L to T and a strong affinity of L to C, all or close to all ligand L is supposed to be bound to C in the chaperone–ligand complex CL if [C] is, for instance, 100-times higher than KC,1 (referred to as “saturation conditions”).
This situation is illustrated in the following set of parameters of a typical ternary complex formation mediated by a molecular glue of type I, which still has some measurable affinity to T:
The derived parameters computed with the comprehensive mathematical model at equilibrium for [C
tot] = 10,000 nM and [L
tot] = 100 nM are as follows: [TL] = 2.48·10
−5 nM, i.e., TL represents 0.0005% of T
tot. [
29] When the excess concentration of [C
tot} is lowered to 1000 nM, the concentration of [TL] is still only 0.002 nM, which corresponds to less than 0.005% of bound target T. For [C
tot] = 100 nM, TL increases to 0.05%, which is still negligible. The 1000-fold higher affinity of L for C relative to T and a 20-fold excess of C (100 nM vs. 5 nM) is sufficient to absorb almost all ligand into CL and suppress any significant concentration of TL. At [L
tot] = 100 nM, [CL] corresponds to 37.4 nM due to the 20-fold excess of C over T; the EC
50 value of the corresponding %T
bound, ternary curve is 5000 nM, which is far away from
KT,2 = 100 nM. This means that already at an 20-fold excess of the more strongly binding counter protein C, ternary complex formation at equilibrium comprises practically only the recruitment of CL to T with no significant concentration of TL. Consequently, the concentrations of T and CLT coincide at the inflection point of the %T
bound, ternary curve. This case is represented by Equation (3) when [T] = [CLT] and, hence,
KT,2 = [CL]. Moreover, if [C] is sufficiently high, all [L
tot] is absorbed by C into CL and, hence, [CL] approaches [L
tot], and consequently, the EC
50 of the %T
bound, ternary curve approximates the ternary
Kd KT,2.
It is obvious that although a 20-fold excess of C is sufficient to suppress significant TL formation around the ternary Kd of KT,2 = 100 nM, this excess is insufficient to approximate [Ltot] to [CL] and enable the estimation of KT,2 via the EC50 of the %Tbound, ternary curve. If the concentration of C is increased to a 200-fold excess over T, i.e., [C] = 1000 nM, [CL] increases to 88 nM at [Ltot] = 100 nM. The EC50 of the %Tbound, ternary curve becomes 113 nM, which is still away from KT,2 = 100 nM. For [C] = 10,000 nM, [CL] at [Ltot] = 100 nM corresponds to 96.6 nM. The EC50 of the %Tbound, ternary curve is 103.5 nM, which is close to the theoretically possible 102.5 nM (Equation (17) below).
It is of interest to study at what excess of C “all” ligand is absorbed by C into CL, i.e., at what excess of C L
tot (to which the EC
50 refers to) corresponds to [CL]. If [C] is increased to an exorbitant 100,000 nM, [CL] approaches a value of 97.5 nM at [L
tot] = 100 nM but does not converge towards
KT,2 = 100 nM. The remaining difference is 50% of [T] = 2.5 nM. To achieve an EC
50 of the %T
bound, ternary curve of 100 nM, an [L
tot] of 102.6 nM is required. This relationship is derived algebraically below. Intuitively, at [L
tot] = 100 nM, the %T
bound, ternary curve reaches 50% of CLT formation if all [L
tot] is bound into CL and CLT and [CL] cannot exceed 97.5 nM at this [L
tot] regardless of [C]. Conversely, the EC
50 value of the %T
bound, ternary curve cannot fall below 102.5 nM regardless of the excess of C over T (
Figure 2).
In conclusion, [C] must be about 100 times the value of KC,1 for the EC50 − [Ttot]/2 of the %Tbound, ternary curve to coincide with KT,2 (see below). If these conditions are experimentally met, measured EC50 values derived from the %Tbound, ternary curve in a target engagement assay can interpreted as KT,2 and, consequently, be used to determine the cooperativity α without the use of a mathematical model.
The impact of the concentration of the monitored weaker binding protein: To understand the influence of the concentration of the monitored weaker binding protein and whether the EC50 value of the %Tbound, ternary curve and KT,2 coincide, it is necessary to relate the corresponding EC50 and Kd or Ltot and free L, respectively, to each other. We have seen in the previous section that under certain conditions, the ternary complex formation equilibria can be simplified such that only one path needs to be considered. If we focus on this case, the influence of the concentration of the monitored, weaker binding protein can be analyzed as part of a binary equilibrium in which CL binds to T and forms CLT (Equation (3)). Note that in Equation (3), the “ligand” that binds to T is CL and not L. For clarity, and because of the general nature of the topic to binary or ternary equilibria, the influence of the concentration of the monitored weaker binding protein on whether the EC50 value matches KT,2 or not is discussed below for the binary binding of L to C, but the entire concept can be applied directly to any binary equilibrium, including that of Equation (3).
In a binary equilibrium, the dissociation constant (
Kd) refers to the free ligand concentration at which 50% of the protein is bound to the ligand while the half-maximal concentration EC
50 refers to the corresponding total ligand concentration:
The Kd for protein C and ligand L (in a defined buffer and at a defined temperature) is a natural constant, i.e., it is independent of the experimental conditions and, particularly, of the selected protein C concentration. Since the determination of a Kd by measurement of the concentrations of three components of a binary equilibrium ([C], [CL] and [L]) requires non-trivial calibration of the analytical signals, scientists like to use, for practical reasons, EC50 values that refer to the required total ligand concentration Ltot at which 50% of protein binding is observed. EC50 values are well suited for the classification of compounds under the same assay conditions. However, it is mandatory for comparing compounds across assays to have the compound-specific and assay-independent Kd values.
To establish the relationship between the easily accessible EC
50 and the
Kd, we start from the simple fact that the total concentration of protein C in a binary binding experiment is the sum of free and ligand-bound protein:
Assuming constant total protein, the half-maximal effect is reached at the total ligand concentration referring to 50% binding, the EC
50 or
:
This inflection point is, hence, referring to the total ligand concentration at which bound and free C concentrations are balanced. Combining Equation (6) and the left-hand side of Equation (
), the identity of
Kd and free ligand concentration at the inflection point is established:
Using the identity for the total ligand at the inflection point, we obtain:
where
is the measured EC
50 value with respect to total ligand in the binary binding experiment. Substitution into Equation (7) yields the final result:
Alternatively, if we rearrange Equation (4) from above,
Substituting [C] in (8) with this definition, we obtain
If we expand [CL] in (9) by [L] in numerator and denominator, we obtain
After combining the two summands, the equation becomes
Rewriting (11) for [CL] gives
Equation (12) still contains [L], which is replaced in analogy to C
tot in Equation (5):
Once we substitute [L] into Equation (9) with Equation (11), we obtain
We now rearrange this equation in two steps such that
KC,1 is placed on the left:
Equation (17) finally defines the dissociation constant independent of concentrations of free ligand and of free protein C but as a function of the known [L
tot] and [C
tot]. The only unknown concentration in Equation (14) is [CL], which is [C
tot]/2 at the inflection point:
Equation (18) can be simplified to
or
Equation (20) means that the
Kd in a binary binding experiment can be obtained from the measured EC
50 by subtracting half the protein concentration used. This explains the general finding that the EC
50 is equal or close to the
Kd value when the protein concentration is well below the
Kd value but that the EC
50 and the
Kd differ significantly when the protein concentration is of the order of magnitude of the
Kd. For example, if the EC
50 = 350 nM and the protein concentration in the corresponding binding experiment is [C
tot] = 500 nM, the
Kd of this compound is 100 nM (350 nM − 500/2 nM = 100 nM). Intuitively, for a protein concentration around or greater than the
Kd, most of the compound is bound. Consequently, if in the same experimental environment, a concentration of the free ligand [L] equals
Kd, i.e., when [CL] corresponds to [C], [L
tot] needs to be well above
Kd, e.g., 350 nM in the above example (
Figure 3).
Equation (17) must now (a) be applied to Equation (3) and (b) be combined with what was discussed in the previous section.
- (a)
According to Equation (17), the EC50 of a %Tbound curve with a concentration of the monitored protein T of 5 nM and a Kd of 100 nM cannot be closer to KC,1 than = 102.5 nM.
- (b)
According to the relationship discussed above, a ternary complex-formation equilibrium can be treated as a binary equilibrium if the excess of the stronger binding protein C is about 20 times higher than that of the monitored weaker binding protein. If the excess of [Ctot] over [Ttot] is greater than 100-fold higher, [CL] coincides with , which means that the EC50 of the %Tbound, ternary curve approaches the limit of Equation (17).
To summarize, a [Ctot] 100 times higher than KC,1 allows treating the ternary equilibrium as a binary system consisting only of CL and T as reactants. Moreover, it allows considering [Ltot] as the concentration of the free ligand L that is CL, i.e., [L] = [CL], which means that the EC50 is the same as KT,2.
The influence of KT,1 on whether apparent and intrinsic cooperativity coincide: A last point of consideration is the definition of the “weaker binding protein”, i.e., at which value of KT,1 a significant TL formation starts to destroy the above discussed simplification into a binary system, despite the above-mentioned 100-fold excess of [Ctot] over KC,1., This threshold represents, then, the boundary between molecular glues of type 1 and bi-functional compounds.
The validity of the above reduction of a ternary complex-forming equilibrium into a binary equilibrium is dependent on the ratio of [Ctot] and [Ttot], as well as the ratio of the lower KC,1 and the higher KT,1. In the above-mentioned example with [Ttot] = 5 nM, [Ctot] = 10,000 nM, KC,1 = 100 nM and cooperativity α = 1000, KT,1 can be as low as 10,000 nM until the difference between the EC50 of the %Tbound, ternary curve and KT,2 becomes significantly larger than the inherent and unavoidable difference, which is 50% of [Ttot] = 2.5 nM. As discussed above, this is because the protein concentration of [Ttot] = 5 nM is too close to the corresponding KT,2 of 10 nM (=KT,1/α = 104 nM/1000). More specifically, the EC50 of the %Tbound, ternary curve is 12.6 nM, which is close to the theoretical 12.5 nM, and the EC50 deviates already 25% from the Kd. For KT,1 > 1000 nM, the relative difference falls below 25%.
Assuming the same parameters as above but with reduced α = 100,
KT,2 becomes 100 nM (=10
4 nM/100), i.e., it deviates from [T
tot] and the difference to the EC
50 value of %T
bound, ternary is further reduced. This illustrates that a lower
KT,2 only becomes relevant in combination with a high intrinsic cooperativity α and for
KT,2 approaching the typical protein concentrations, which results in larger differences between the EC
50 of the %T
bound, ternary curve and the underlying
KT,2 (
Figure 4).
In summary, the difference between the EC50 value of the %Tbound, ternary curve and the underlying KT,2 becomes less than 2.5% with respect to KT,2 for [Ttot] that is more than 20 times lower than KT,2 and [Ctot] that is more than 100 times larger than KC,1. At the inflection point of the ternary complex formation monitored by the target T, the concentration of the free target [T] is equal to the concentration of %Tbound = [TL] + [CLT]. However, if all the free ligand is bound in [CL] (due to the excess of [C] and the weak affinity of L to T), [Tbound] = [TL] + [CLT] ≈ [CLT] corresponds exclusively to [CLT], i.e., the inflection point of the %Tbound curve coincides with KT,2 = [CL] ≈ [Ltot] (see above). As soon as the affinity of L to T increases, the formation of the ternary complex is no longer the result of the binding of CL to T but also of the binding of TL to C. The same applies when the total concentration of C ([Ctot]) becomes lower and approaches KC,1. In this case, the EC50 of the %Tbound, ternary curve (i.e., in the presence of the chaperone C) is not equal to KT,2 and the corresponding shift in the binary binding curve corresponds only to the apparent cooperativity and not the intrinsic cooperativity. In this case, both paths are significantly contributing, and the intrinsic cooperativity can only be determined by a mathematical model, which requires input parameters from both binding assays with C and T as the monitoring proteins.
2.2. Experimanental Cooperativity Studies on a Small Series of FKBP12:R,S-SLF-X:MAPRE1 Ternary Complexes
MAPRE1 is a plus-end tracking protein (+TIPs) that regulates microtubule (MT) behavior and interactions between MTs and other intracellular structures during mitosis [
30]. It was identified as the recruitment complement of FKBP12 by a protein array screening of 50 macrocyclic FKBP12 ligands against 2500 randomly selected proteins. The ternary complex of FKBP12:
R,S-SLF-1a:MAPRE1 was characterized recently [
31]. The protein NMR and X-ray structure of the ternary complex reveal multiple interactions between
R,S-SLF-1a and MAPRE1 as well as interactions between FKBP12 and MAPRE1, both of which only occur in the ternary complex. The increased binding of
R,S-SLF-1a and related compounds to FKBP12 by the presence of MAPRE1 or to MARPE1 by the presence of FKBP12 enables the retrieval of the intrinsic cooperativity α. Due to the distinct binary affinities of the studied molecular glues, we expect different apparent cooperativities but the same intrinsic cooperativity α regardless of whether monitoring is through MAPRE1 or FKBP12.
TR-FRET proximity assays quantify the compound-mediated induced proximity by measuring the distance-dependent energy transfer between a donor- and an acceptor-tagged protein. It is noteworthy that ternary complex-forming compounds do not necessarily have to exhibit intrinsic cooperativity. Even in the absence of cooperativity (α = 1), ternary complexes can be formed based on the independent affinity of such compounds to either of the two proteins. While a TR-FRET proximity assay can monitor the formation of a non-cooperative ternary complex formation, i.e.,
KC,1/
KC,2 =
KT,1/
KT,2 = 1, a target engagement assay cannot as it only reports increased ligand binding caused by interactions that occur exclusively in the ternary complex (α > 1). However, if no ternary complex is formed at all, there is also no compound-dependent increase in the %A
max value of the TR-FRET assay. For this reason, we focus on those compounds from our previous publication [
31] that exhibited the highest %A
max values in the TR-FRET proximity assay when evaluating cooperativity with a target engagement assay (
Table 1).
All TR-FRET-active compounds from R,S-SLF-1a to R,--SLF-11 have the R-configuration at the α-position of the 2-amido-4-methylene-pipecolinic moiety and the S-configuration at the α-position of the second amino acid of the recruitment loop (if there is a chiral center). The compounds S,S-SLF-1d and S,S-SLF-12 are negative controls that bind strongly to FKBP12 but lack any %A
max increase, i.e., do not recruit MAPRE1 (%A
max = 0%) (
Figure 5).
As discussed in the previous section, the study of the apparent cooperativity consists of two steps: the binding characterization of a ligand to a target protein T in the absence and in the presence of a counter protein. The counter protein will (in case there is intrinsic cooperativity) lead to an increased affinity of the ligand for T, i.e., will lead to a lower KT,2 relative to the ligand alone (KT,1). Importantly, the requirement that both experiments are identical (except for the presence of the counter protein) allows labeling of only the protein by which the binding event is monitored. An alternative to this assay without protein labeling would be a competitive binding assay that measures changes in fluorescence polarization by a fluorescent tracer–ligand substitution whose fluorescence signal changes significantly when it transitions from a bound to an unbound state. However, a competitive binding assay requires chemical matter that binds to the target. Since there is no reason to expect strong binding of the FKBP12:R,S-SLF-X:MAPRE1-forming compounds to MAPRE1 alone, such a competitive binding assay was not an option.. Compared to a competitive binding assay, the monitoring of binding by structural changes on the labled protein is also independent of the binding site, which was what we prefered.
Our method of choice is the spectral shift method, which monitors binding events on the target isothermally and in equilibrium via an environment-sensitive near-infrared fluorophore [
32]. In the case of target engagement, either the proximity of the ligand towards the dye or structural changes occurring in the target as a result of binding lead to a change in the chemical environment of the fluorophore. Those changes affect the physiochemical properties of the reporter fluorophore and translate into either blue or red shifts (or peak broadening) of emission peaks upon ligand binding, which can be sensitively monitored by simultaneously recording the fluorescence at two wavelengths (i.e., at 650 nm and 670 nm). Calculating the ratio between the two fluorescence channels then allows to monitor subtle emission shifts that occur as a result of target engagement. Affinity measurements can then be performed by recording the spectral shift as a function of ligand concentration.
In the following section, the binding of each of the 10 selected compounds through MAPRE1 and FKBP12 is discussed and the resulting apparent and intrinsic cooperativities were compared in an Amax-ranked order.
Binding study through MAPRE1: MAPRE1 was labeled via lysines using an NHS-conjugated dye. The final concentration of MAPRE1
NHS (referring to [T
tot]) was 5 nM. Compounds could be titrated up to a concentration of 200 μM (referring to [L
tot]). The titration of
R,--SLF-11 up to [L
tot] = 200 μM showed a very clear well-characterized onset of the %T
bound, binary curve, which by interpolation, resulted in an estimated EC
50 of 1.8 mM. Well-defined minimal response values of the dose–response curve fitting of standard models resulted in reasonable approximations for EC
50 and derived
Kd = EC
50 − [T
tot]/2. However more accuracy could only be achieved at higher ligand concentrations—ideally at full target saturation. However, this was experimentally infeasible due to assay conditions (i.e., the requirement of maintaining a certain DMSO concentration or avoiding solubility issues of the ligand). Although the determined
KT,1 values of binding to MAPRE1 are only approximations, their relative ranking reflects the underlying differences in the affinity of the ligands L to MAPRE1. Performing these experiments in duplicates confirmed the high signal-to-noise ratio, i.e., there was no significant deviation between the two curves, indicating a high accuracy of the interpolated EC
50 values. Due to the low [T
tot] = 5 nM, this value coincides with
KT,1 (1.8 mM − 0.005 mM/2 ≈ 1.8 mM). Since FKBP12 is a well-behaved protein, an excess of [C
tot] = 10 μM could be used for
KT,2 characterization, resulting in an EC
50 value of the %T
bound, ternary curve of [L
tot] = 180 nM and an apparent cooperativity = 10,000. Since [C
tot] = 10 μM is only 41 times the
KC,1 = 234 nM instead of the recommended factor of 100 (
Figure 6a), the EC
50 value of 180 nM of the measured %T
bound, ternary curve does not exactly match the value from the general mathematical model. Iteration until the intrinsic cooperativity α matches the measured EC
50 value of [L
tot] = 180 nM (at [C
tot] = 10,000 nM, [T
tot] = 5 nM,
KC,1 = 234 nM,
KT,1 = 1,800,000 nM) results in an intrinsic cooperativity of α = 10,405 (
Figure 6b). At [L
tot] = 180 nM, the calculated corresponding “ligand” concentration of [CL] is 173 nM, which is below the upper maximum of [CL] = 180 nM − 2.5 nM = 177.5 nM. This means that with a [C
tot] of “only” 10 μM, [L
tot] = 180 nM does not achieve the maximum possible concentration of [CL] = 177.5 nM, unlike an excess of [C
tot] of 100 times
KC,1 (or higher). Consequently,
KT,2 corresponds to 173 nM and not 177.5 nM. This deviation of 2.6% between the measured EC
50 of the %T
bound, ternary curve and the underlying
KT,2 represents the difference of the measured apparent cooperativity of 10,000 and the corresponding underlying intrinsic cooperativity α = 10,405 (
Figure 6b).
Binding studies through FKBP12: To monitor the binding of
R,--SLF-11 by the stronger binding FKBP12 in the absence and in the presence of 10 μM MAPRE1 via %C
bound, binary and %C
bound, ternary, respectively, the concentration of reversibly NTA-labeled FKBP12 was limited to [C
tot] = 40 nM. The EC
50 value of the %C
bound, binary curve was 254 nM compared to 230 nM in the TR-FRET competitive binding assay from our previous work [
31]. This results in
KC,1 = 234 nM using Equation (20). Repeating this experiment in the presence of [T
tot] = 10 μM of MAPRE1 resulted in an EC
50 of the %C
bound, ternary curve of 66 nM corresponding to a relative shift or apparent cooperativity of 254 nM/66 nM = 3.8. In contrast to the experimental setup in the previous two binding experiments with monitoring through the weaker binding protein MAPRE1, where the applied protein concentrations were optimally chosen, this is not the case for the binding experiment through the stronger binder FKBP12. First of all, the applied excess of T with [T
tot] = 10 μM is roughly 20000-fold off of the proposed 100 times
KT,1 threshold, which would correspond to 180 mM. Only under such excess conditions of T can the equilibrium of forming TL under the constraint that all ligand L is bound to T be reached to ensure that [L
tot] approaches the “ligand” concentration [TL]. Moreover, the concentration of the labeled protein FKBP12
NTA with [C
tot] = 40 nM is too close to the corresponding
KC,1 = 234 nM, resulting in a high offset of 20 nM = [C
tot]/2 of the EC
50 value of the %C
bound, ternary curve and the corresponding
KC,2. If
KC,2 is sufficiently high, the 20 nM deviation to correct for the protein concentration could be neglected. However, the resulting calculated value for
KC,2 is 0.023 nM, accounting for the cooperativity α = 10,405 and
KC,1 = 234 nM as derived by the MAPRE1 experiment. This value is far below the applied protein concentration of [C
tot] = 40 nM and makes it infeasible to estimate
KC,2 from the EC
50 of the %C
bound, ternary curve. Consequently, the EC
50 shifts, meaning the apparent cooperativity, from monitoring the binding by the stronger binding protein C are diverging from the underlying intrinsic cooperativity α. Using the binary and ternary binding data to MAPRE1 with cooperativity α = 10,405 and
KT,1 = 1.8 mM and the binary binding to FKBP12 with
KC,1 = 234 nM, a resulting EC
50 = 24.2 nM is estimated for the %C
bound, ternary curve relative to the experimentally determined 66 nM. The deviation of calculated (254 nM/24.2 nM = 10.5) and measured apparent cooperativity (254 nM/66 nM = 3.8) can be explained by a negative cooperativity induced by the His6-NTA tag of FKBP12. Studies to lower [C
tot] and identify a better position for the spectral shift tag on FKBP12 are ongoing (
Figure 6a).
Binding study through MAPRE1: The compound with the second highest A
max of 255%,
R,S-SLF-6, is found to have an EC
50 value of the %T
bound, binary curve of 0.5 mM. The EC
50 value of the %T
bound, ternary curve was shifted to 114 nM in the same binding experiment but in the presence of 10 μM FKBP12, i.e., [C
tot] is 222 times the
KC,1. From the mathematical model a “ligand” concentration of [CL] = 111.5 nM at [L
tot] = 114 nM is found. This means that any applied ligand L
tot that is not bound into CLT is bound to CL, i.e., [CL] ≈ EC
50–[T
tot]/2 ≈
KT,2 ≈ 111.5 nM. Consequently, the EC
50 value of the %T
bound, ternary curve matches
KT,2 exactly for the given [T
tot] = 5 nM (0% deviation). As a result, the apparent cooperativity of 500,000 nM/114 nM = 4386 coincides with the intrinsic cooperativity α of 500,000 nM/111.5 nM = 4484 and the systematic difference due to the protein concentration becomes neglectable (
Figure 7b).
Binding study through FKBP12: The obtained results from the above binding studies via the alternative protein can be used to validate the proposed concept of retrieving the intrinsic cooperativity α from only one binding assay. For
R,S-SLF-6, the EC
50 values shift in the binary to ternary setup from 65 nM (i.e.,
KC,1 = 45 nM) to 24 nM. With a cooperativity α = 4484, obtained via MAPRE1 binding, the EC
50 value of the calculated %C
bound, ternary curve resulted in 21 nM, which is an almost perfect match and confirms the independently obtained values of the MAPRE1 binding experiment. The calculated “ternary”
Kd KC,2 =
KC,1/α = 45 nM/4484 = 0.01 nM indicates that the EC
50 value of the %C
bound, ternary curve of 21 nM is much greater than
KC,2, resulting in distinct apparent and intrinsic cooperativity values, which highlights that the information of the stronger binding protein alone is insufficient to characterize the intrinsic cooperativity α without using a comprehensive mathematical model (
Figure 7a).
Binding study through MAPRE1 R,--SLF-10: This compound, with third highest %A
max of 135%, has an interpolated EC
50 value of the %T
bound, binary curve of only 2.0 mM and, therefore, with an even weaker potency than that of
R,S-SLF-11. The same binding experiment but in presence of 10 μM FKBP12, i.e., [C
tot] = 93·
KC,1, resulted in an EC
50 shift in the %T
bound, ternary curve to [L
tot] = 377 nM. The “ligand” concentration from the mathematical model results in [CL] = 370 nM at [L
tot] = 377 nM. This is a deviation of 1.2% from the theoretical upper bound of 377 nM–2.5 nM = 374.5 nM. This also implies that
KT,2 is not 374.5 nM as hinted by the EC
50 value but 370 nM. Consequently, the apparent cooperativity of 2,000,000 nM/377 nM =5305 approaches the intrinsic cooperativity α = 2,000,000 nM/370 nM = 5405 (
Figure 8b).
Binding study through FKBP12: For
R,--SLF-10, the EC
50 of the %C
bound, binary curve shifted from 128 nM (i.e,
KC,1 = 108 nM) to the EC
50 of the %C
bound, ternary curve of 40 nM, resulting in an apparent cooperativity of 3.2. With the cooperativity α = 5405 from the MAPRE1 binding experiments, the EC
50 of the %C
bound, ternary curve is 24 nM with an apparent cooperativity of 5.3. The calculated “ternary”
Kd becomes
KC,2 =
KC,1/α = 108 nM/5405 = 0.024 nM which shows that the EC
50 value of the %C
bound, ternary curve of 40 nM is far from
KC,2 = 0.024 nM (
Figure 8a).
Binding study through MAPRE1: For
R,S-SLF-3, the compound with the fourth highest %A
max of 93%, an EC
50 value of the %T
bound, binary curve of 1.8 mM was interpolated. The same binding experiment but in the presence of 10 μM FKBP12, i.e., [C
tot] = 152·
KC,1, resulted in a shift in the EC
50 value of the %T
bound, ternary curve to [L
tot] = 827 nM. The calculated model-based “ligand” concentration is [CL] = 818 nM at [L
tot] = 827 nM. This is a rather small deviation of 0.8% from the true value of 827–2.5 nM = 824.5 nM. This means that
KT,2 is not 824.5 nM when directly reading off the EC
50 but, rather, 818 nM. Moreover, the apparent cooperativity of 1,800,000 nM/823 nM = 2177 approaches the intrinsic cooperativity α of 1,800,000 nM/818 nM = 2200 (
Figure 9b).
Binding study through FKBP12: For
R,S-SLF-3, the EC
50 of the %C
bound, binary curve shifted from 86 nM (then
KC,1 = 66 nM) to a measured EC
50 of the %C
bound, ternary curve of 49 nM, resulting in an apparent cooperativity of 1.8 relative to a calculated apparent cooperativity of 5.7. The same value estimated with the cooperativity α of 2200 from the MAPRE1 binding experiment gave an EC
50 of the interpolated %C
bound, ternary curve of 25 nM, which deviates from the measured value by a factor of only factor 2 (5.3/1.8 = 1.9). This independently confirms the accuracy of the measurement through the weak MAPRE1 binding. The calculated “ternary”
Kd of
KC,2 =
KC,1/α = 66 nM/2200 = 0.030 nM shows that the EC
50 value of the %C
bound, ternary curve is far from
KC,2, i.e., the monitoring of binding through the stronger binding protein does not allow the direct determination of
KC,2 and consequently the intrinsic cooperativity α cannot be determined through FKBP12 binding without a mathematical model describing all non-saturated conditions (
Figure 9a).
Due to a aminomethyl instead of the hydroxymethyl moiety (as R,S-SLF-6) at the second residue or the recruitment loop, R,S-SLF-7’s %Amax value drops from 255% to only 45%.
Binding study through MAPRE1: The EC
50 value of the %T
bound, binary curve of
R,S-SLF-7 was interpolated to 0.46 mM, which is slightly lower than that of the previous compounds. It has to be noted that R,S-SLF-7 showed precipitation at high concentrations. Therefore, measurements from the highest concentration samples had to be removed, which impaired the determination of the interpolation curve. Moreover, the signal is much smaller compared to the other studied ligands. In the same binding experiment but in the presence of 10 μM FKBP12 (i.e., [C
tot] = 60·
KC,1), the EC
50 of the %T
bound, ternary curve shifted to [L
tot] = 1985 nM. The model-based estimate is [CL] = 1941 nM for the “ligand” at [L
tot] = 1985 nM. This is a deviation from the theoretically found true value of 1985 nM − 2.5 nM = 1982.5 nM. The
KT,2 is 2% below the EC
50 value of the %T
bound, ternary curve. The apparent cooperativity of 460,000 nM/1985 nM = 232 is still below the cooperativity α of 460,000 nM/1941 = 237 (
Figure 10b).
Binding study through FKBP12: The EC
50 value for
R,S-SLF-7 shifted from 186 nM in the %C
bound, binary curve (resulting in
KC,1= 166 nM) to a measured EC
50 of the %C
bound, ternary curve of 110 nM, so the apparent cooperativity becomes 1.7. Using the cooperativity α = 237 from MAPRE1 binding resulted in an EC
50 value for the calculated %C
bound, ternary curve of 48 nM, which corresponds to a calculated apparent cooperativity of 3.9. The calculated “ternary”
Kd of
KC,2=
KC,1/α = 166 nM/237 = 0.7 nM shows that the EC
50 value of the %C
bound, ternary curve is, again, very distinct from
KC,2, i.e., the direct determination of
KC,2 by monitoring the binding events corresponding to the stronger binding protein does not enable the direct identification of the cooperativity α without using a mathematical model (
Figure 10a).
R,S-SLF-1a represents the only hit compound from a protein array screening against 2500 proteins. Its %Amax = 51% in the TR-FRET proximity assay was the starting point that ultimately led to the identification of a series of glues with %Amax values of up to 350%, i.e., a 7-fold improvement with respect to %Amax.
Binding study through MAPRE1: It was known from previous NMR studies that
R,S-SLF-1a has a weak (greater than 250 μM) but measurable affinity for MAPRE1. This was confirmed by the binding study using the spectral shift method. The EC
50 value of the %T
bound, binary curve of
R,S-SLF-1a was estimated as 2.0 mM. The same binding experiment, but in the presence of 10 μM FKBP12, i.e., [C
tot] = 476·[
KC,1], shifts the EC
50 of the %T
bound, ternary curve to [L
tot] = 1030 nM. The model-based estimate of the “ligand” concentration yields [CL] = 1025 nM at [L
tot] = 1030 nM. The
KT,2 = 1025 nM deviates from the true value of 1030 nM–2.5 nM = 1027.5 nM by 0.24%.
R,S-SLF-1a’s apparent cooperativity of 2,000,000 nM/1030 nM = 1942 is in great agreement with the cooperativity α = 2,000,000 nM/1025 nM = 1951) within the experimental error (
Figure 11b).
The binding study through FKBP12 R,S-SLF-1a’s EC
50 value of the %C
bound, binary curve of 41 nM (i.e.,
KC,1 = 21 nM) showed no significant shift in the EC
50 of the %C
bound, ternary curve of 45 nM, resulting in an apparent cooperativity of 0.9. Estimation using the cooperativity α = 1951 from the MAPRE1 binding resulted in an EC
50 for the calculated %C
bound, ternary curve of 22 nM, which is lower by factor 2 than the measured value. This result shows that the combination of a low
KC,1 and a high [C
tot] reaches the limit of the assay. It is not possible for
R,S-SLF-1a to detect an apparent cooperativity by monitoring the ternary binding formation by the stronger binding protein, although there is significant underlying intrinsic cooperativity α. In this case, only the binding study by the weaker binding protein revealed the significant underlying cooperativity α. It is insightful to compare to
R,S-SLF-6 with an advantageous
KC,1 of 45 nM, which is only 2.1-times higher than that of R,S-SLF-1a (21 nM). However, it is not the relative difference between the two values that is of relevance but the absolute value. The
KC,1 of
R,S-SLF-1a is exactly at the lower limit of the assay, which is
KC,2 + [C
tot]/2 = 21 nM/1951 + 20 nM = 0.011 nM + 20 nM = 20.011 nM. In other words, EC
50s of the %C
bound, ternary curve below a threshold of 20 nM cannot be detected. If the EC
50 of the %C
bound, binary curve is already at 20 nM, no shift is to be expected, which is seen in the experiment (
Figure 11a).
R,S-SLF-8 is the selected compound with the lowest %Amax value of 27% in the TR-FRET proximity assay.
Binding study through MAPRE1: The EC
50 value of the T
bound, binary curve of
R,S-SLF-8 is interpolated to 1.6 mM. The same binding experiment but in the presence of 10 μM FKBP12, i.e., [C
tot] = 92·[
KC,1], results in shifts of the EC
50 of the %T
bound, ternary curve to [L
tot] = 1074 nM. The model-based concentration of the recruited “ligand” is [CL] = 1060 nM at [L
tot] = 1074 nM. A
KT,2 of 1060 nM means a deviation of 1.1% from the true value, which is 1074 nM–2.5 nM = 1071.5 nM. This means that the apparent cooperativity of 1,600,000 nM/1074 nM = 1490 for
R,S-SLF-8 matches the intrinsic cooperativity α =1,600,000 nM/1060 nM = 1509 within the experimental error (
Figure 12b).
Binding study through FKBP12: The EC
50 of the %C
bound, binary curve of
R,S-SLF-8 is 129 nM (i.e.,
KC,1 = 109 nM) shifted to a measured EC
50 of the %C
bound, ternary curve of 65 nM, resulting in an apparent cooperativity of 2.0. Recalculating this with the intrinsic cooperativity α = 1509 obtained through MAPRE1 binding gave an EC
50 of the calculated %C
bound, ternary curve of 31 nM, which is only a factor of 2.1 off the measured value. The calculated ternary
Kd KC,2 =
KC,1/α = 109 nM/1509 = 0.7 nM shows that the EC
50 value of the %C
bound, ternary curve is different from
KC,2, i.e., monitoring the binding events through the stronger binding protein does not enable the direct determination of
KC,2 and estimation of the intrinsic cooperativity α through FKBP12 would require a mathematical model (
Figure 12a).
R,S-SLF-12 was selected as a negative control compound, which has a high affinity for FKBP12 but does not form any ternary complex according to the TR-FRET assay.
Binding study through MAPRE1: The EC
50 value of the %T
bound, binary curve of
R,S-SLF-12 showed no binding to MAPRE1 up to [L
tot] = 200 μM. This negative result indirectly confirms that the above affinities to MAPRE1 are real and required to characterize the cooperativity α of the studied ternary complex system. It also emphasizes the importance of using methods capable of accurately detecting very weak affinities (
Figure 13b).
Binding study through FKBP12: For the negative control
R,S-SLF-12, the EC
50 value of the %C
bound, binary curve of 43 nM (i.e.,
KC,1 = 13 nM) compared with a measured EC
50 value of the %C
bound, ternary curve of 30 nM results in an apparent cooperativity of 1.4. Since [C
tot] = 40 nM is even higher than the
KC,1 = 13 nM, any
KC,2 lower than
KC,1 (i.e., for α > 1) would not be measurable with the given assay setup. Without measurable binding to MAPRE1 and given the lack of a %A
max value above background (%A
max = 0%), the observed shift in %C
bound, binary of 43 nM to %C
bound, ternary of 30 nM by factor 1.4 is too small to be interpreted as proof of an underlying intrinsic cooperativity α (
Figure 13a).
S,S-SLF-1d is an epimer of R,S-SLF-1a and differs only in the stereochemistry at the α-position of the 4-methylenepiperidine-2-carboxyamide unit, which is S instead of R. In the TR-FRET proximity assay, S,S-SLF-1d showed no evidence of ternary complex formation (%Amax = 0%), indicating the high specificity of the interactions within the ternary complex FKBP12:R,S-SLF-1a:MAPRE1.
Binding study through MAPRE1: The EC
50 value of the %T
bound, binary curve of
S,S-SLF-1d is interpolated to 1.4 mM compared to 2.0 mM for
R,S-SLF-1a. The same binding experiment but in the presence of 10 μM FKBP12, i.e., [C
tot] = 1428·
KC,1, shifted the EC
50 value of the %T
bound, ternary curve to a [L
tot] higher than 1.4 mM but it was not possible to identify any
Kd. No positive cooperativity (α > 1) is observed but negative cooperativity (α < 1) cannot be excluded. This would mean that despite the presence of a high excess of FKBP12,
S,S-SLF-1d is at best bound to MAPRE1 with the same affinity as in the absence of FKBP12. This is a good example of how the strong affinity to the chaperone protein C cannot compensate for the very weak affinity of the target protein T if there is no positive cooperativity α (
Figure 14b).
Binding study through FKPB12 EC
50 of the
S,S-SLF-1d’s %C
bound, binary curve of 27 nM, i.e.,
KC,1 = 7 nM, showed a measured EC
50 of the %C
bound, ternary curve of 29 nM and no apparent cooperativity was observed, as the assay was at the bottom with this
KC,1 (
Figure 14a). This, again, emphasizes the advantage of measuring cooperativity through the weaker binding protein (
Figure 14a).
Intrinsic affinities between the two proteins C and T, i.e., without the presence of a molecular glue, add a third pathway that enables the ligand to bind to the chaperone–target complex. In this case, the ternary complex-forming equilibrium would require additional constraints in the mathematical model and impact on the determination of the intrinsic cooperativity α. Importantly, in our study, no intrinsic interactions between MAPRE1 and FKPB12 are measurable (
Figure 15) under the current experimental conditions (40 nM FKBP12 vs. 10,000 nM MARPRE1 or 5 nM MAPRE1 vs. 10,000 nM FKBP12), which confirms the observation from our NMR studies [
31] (
Figure 15).