The effect of a potentiating drug on ion channel function is typically evaluated by comparing current responses to the control agonist in the presence and absence of the potentiator. Differences in ratios of responses are then taken as proof of distinct potentiation properties when comparing modulation by different compounds. In these experiments, the concentration of the agonist is typically kept low to generate a small fractional control response. The precise relative magnitude of the control response is, however, not standardized among labs and can range from a concentration producing a response equal to just 2% of maximal (EC2) to over EC25 in different studies. Here, we have investigated the relationship between the magnitude of the control response and the expected response ratio. As the EC value of the control response increases, the ratio of responses to agonist in the presence and absence of the potentiator decreases. We provide equations to calculate the expected response ratios at different levels of control responses and free energy changes at different response ratios. Lastly, we discuss the effect of the value of EC of the control response on the efficacy of negative allosteric inhibitors.

Drug-induced potentiation of receptor-channel function can manifest in numerous behavioral endpoints, including sedation and anesthesia (GABAA receptor), cognitive enhancement (NMDA receptor), or heightened pain sensation (TRPV channel) (Numazaki and Tominaga, 2004; Garcia et al., 2010; Collingridge et al., 2013). In electrophysiological recordings, potentiation is measured by calculating the response ratio (RR) from the ratio of amplitudes of current responses to an agonist in the presence and absence of a modulator. A difference in RR at a given modulator concentration is typically taken as evidence of distinct potentiation properties when comparing modulation by different compounds.

One issue with this approach is that it does not take into consideration the relative magnitude of the control response, i.e., the response to agonist in the absence of the modulator, which can vary considerably in different studies. As a result, the RR measured at, for example, the EC2 concentration of an agonist in one study may be, inappropriately as we show below, compared with the RR measured at, for example, the EC25 concentration of agonist in a different study (Belelli et al., 2002; Bracamontes et al., 2011; Germann et al., 2021). While it is intuitively clear that due to saturation the RR is reduced at larger fractional values of the control response, the precise relationship between the two is not obvious. Here, we have investigated how the magnitude of the response to agonist modifies the apparent potentiating effect. Essentially, we asked whether, for example, a modulator-induced tripling of an EC2 control response is energetically equivalent to tripling of an EC25 response. An alternative way to put this is whether a fixed free energy change associated with the binding of a modulator is expected to generate the same RR at different EC values.

We will consider the case of a receptor that has only two states—resting and active—using the approach first described by L. Boltzmann in his seminal 1877 paper (Sharp and Matschinsky, 2015). He proposed that the relative probabilities that a system would be in one or the other state is related to the energy difference between the states
(1)
or
(2)
where R is the universal gas constant (1.987 cal/[K × mol]), T is the absolute temperature, and the subscripts R and A denote the resting and active states, respectively. This relationship has been widely used in chemistry and biology, including in absolute rate theory to define the activation energy necessary to move from the initial state to the transition state in the reaction coordinate (Evans and Polanyi, 1935; Eyring, 1935), dissociation of salts to characterize the energy of solution (Gibbs, 1876), and the distribution of gating charges in the membrane potential during inactivation of voltage-gated channels (Hodgkin and Huxley, 1952).
For a receptor that can only be resting or active, PR = 1 − PA. Accordingly,
(3)
In the presence of a potentiating modulator
(4)
where PA+M and PR+M are the probabilities the receptor is in the active or resting state, respectively, when the agonist and modulator are co-applied. We will refer to ΔGM as the “stabilization energy” to indicate that it is the energy associated with modulator binding that reduces the energy difference between resting and active states.
Initially, we consider a case where the agonist is able to activate all receptors at a saturating concentration. That is, we have assumed equivalence between EC (ranges from 0 to 100) and PA (ranges from 0 to 1), i.e., that at EC5 PA = 0.05, at EC20 PA = 0.2, and so on. In this case, the additional energy contributed by a modulator can be calculated as
(5)
where ECagonist is the EC value of the response to agonist in the absence of modulator, and RR is the response ratio calculated as the ratio of response amplitudes in the presence and absence of the modulator.

We can now address the question about the energies required to, for example, triple an EC2 response as compared with an EC25 response. It takes −1.30 kcal/mol to triple the EC25 response and only −0.67 kcal/mol for the EC2 response. Fig. 1 A illustrates the relationship between the energy required to triple the response and ECagonist. The main inference is that the energetics of receptor function do not scale linearly with changes in current responses.

Inspection of Fig. 1 indicates that the value of ΔGM required to triple the response approaches an infinitely large negative number when the control EC value approaches 1/3.

An alternative way to demonstrate the effect of differing control activation is to calculate the RR produced by co-application of a modulator whose binding provides a constant ΔGM. Rearranging Eq. 5 gives
(6)
In Fig. 1 B, we have plotted the relationship between the RR and ECagonist assuming a ΔGM of −1 kcal/mol. The relationship shows, as expected, a steady decline as the magnitude of the control response increases. It is also clear from here that RRs measured at different levels of control activity should not be compared directly. For example, we find that the modulator whose binding is associated with a −1 kcal/mol of free energy change increases the response to agonist by fivefold (1 = no effect) at EC2 and by 2.6-fold at EC25.

In the majority of receptor–agonist combinations, the EC and PA values are not equivalent; that is even at saturating concentrations, the agonist cannot activate all receptors, and PA is less than EC/100. In addition or alternatively, a receptor may be constitutively active, in which case, and particularly at low agonist concentrations, PA exceeds EC/100. This necessitates the conversion of ECagonist to PA,agonist. In macroscopic recordings, this can be done by normalizing the amplitude of the response to a given agonist to those of a known inhibitor expected to block all receptors (PA = 0) and a high-efficacy agonist or a combination of agonists that through independent means or experiments has been shown to generate a response with a PA of 1. For example, in the case of the GABAA receptor, picrotoxin is used to reach a current response with PA of 0, and the combination of the transmitter GABA with allosteric agonists propofol or pentobarbital is employed to generate a response with PA of 1 (Chang and Weiss, 1999; Ziemba and Forman, 2016; Shin et al., 2017; Shin et al., 2019). In single-channel recordings, the PA of the response can be calculated directly from the mean open and closed time durations (Steinbach and Akk, 2001; Mortensen et al., 2004; Lema and Auerbach, 2006).

When using PA,agonist rather than ECagonist, Eq. 5 modifies to
(7)
and Eq. 6 to
(8)

Fig. 2 A shows the energy required to triple the control response for two partial agonists. Fig. 2 B shows the relationship between the RR and PA of the control response in the presence of a modulator contributing −1 kcal/mol of free energy change. The calculations were done for cases where EC100 corresponds to PA of 0.5 (a medium-efficacy agonist) and where EC100 corresponds to PA of 0.25 (a low-efficacy agonist). As in Fig. 1, the energy required increases with increasing EC (Fig. 2 A) and the RR is reduced at higher levels of control activity (Fig. 2 B). Unlike in Fig. 1 B, potentiation is observed even at EC100 because the PA at saturating concentrations of agonist remains sub-maximal.

It is also the case that the effect of a negative allosteric modulator that stabilizes the resting state shows a similar relationship to the control activity. In this case, the RR is between 0 and 1 and ΔGM >0. As shown in Fig. 3 A, as the level of control activity increases, the energy required to produce a given RR increases and approaches infinity as the control PA approaches 1. Analogously, the efficacy of the inhibitor decreases at a fixed (1 kcal/mol) ΔGM (Fig. 3 B). It is important to note that the effects of negative modulators may not conform to the two-state approach we are using (Germann et al., 2022).

Experiments have demonstrated reduction in potentiation as a function of increasing agonist concentration for a number of receptors, including potentiation of GABAA receptors by diazepam (Gielen et al., 2012) or neurosteroids (Bracamontes and Steinbach, 2009) and potentiation of neuronal nicotinic receptors by β-estradiol (Paradiso et al., 2001), CMPI (Deba et al., 2022), or calcium ions (Natarajan et al., 2020), of serotonin type 3 receptors by alcohols and anesthetics (Machu and Harris, 1994), or NMDA receptors by the synthetic compound GNE-9278 (Wang et al., 2017). Our demonstration does not require any particular hypothesized mechanism for potentiation. However, it is based on the idea that receptor function is adequately described by a simple, two-state system. This can be appropriate as long as slowly equilibrating states (desensitized, for example) can be reduced by an appropriate protocol that entails fast and standardized drug perfusion so that the measured peak response corresponds to the equilibrium response in the two-state model.

In sum, we have investigated here the relationship between the ability of a compound to potentiate the response to agonist and the relative magnitude of the control response. As ECagonist increases, the RR decreases. Accordingly, comparison of potentiation efficacy among different compounds measured at different ECagonist is inappropriate. Eq. 7 (or 5 in the case of an efficacious control agonist with high maximal PA,agonist and receptor with low constitutive PA) enables calculation of ΔG for a modulator based on the amplitudes of current responses in the presence and absence of the modulator. Eq. 8 (or 6 with high-efficacy control agonist) enables calculation of the predicted RR if the level of the control response and the ΔG for the modulator are known. Alternatively, Eqs. 6 and 8 can be used to predict potentiation RRs at fixed ΔGM at different levels of control response.

No new data were generated or analyzed in support of this study.

Eduardo Ríos served as editor.

This study was supported by the National Institutes of Health National Institute of General Medical Sciences grant R35GM140947 and funds from the Taylor Family Institute for Innovative Psychiatric Research.

Author contributions: Joe Henry Steinbach: conceptualization, formal analysis, and writing—original draft, review, and editing. Gustav Akk: conceptualization, funding acquisition, methodology, and writing—original draft.

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Author notes

Disclosures: The authors declare no competing interests exist.

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