Olfactory perireceptor and receptor events in moths: a kinetic model revised
Modelling reveals that within about 3 ms after entering the sensillum lymph, 17% of total pheromone is enzymatically degraded while 83% is bound to the pheromone-binding protein (PBP) and thereby largely protected from enzymatic degradation. The latter proceeds within minutes, 20,000-fold more slowly than with the free pheromone. In vivo the complex pheromone–PBP interacts with the receptor molecule. At weak stimulation the half-life of the active complex is 0.8 s due to the postulated pheromone deactivation. Most likely this process is enzymatically catalysed; it changes the PBP into a scavenger form, possibly by interference with the C-terminus. The indirectly determined PBP concentration (3.8 mM) is close to direct measurements. The calculated density of receptor molecules within the plasma membrane of the receptor neuron reaches up to 6,000 units per μm2. This is compared with the estimated densities of the sensory-neuron membrane protein and of ion channels. The EC50 of the model pheromone–PBP complex interacting with the receptor molecules is 6.8 μM, as compared with the EC50 = 1.5 μM of bombykol recently determined using heterologous expression. A possible mechanism widening the range of stimulus intensities covered by the dose–response curve of the receptor-potential is proposed.
KeywordsPheromone binding protein Pheromone deactivation Pheromone degradation Olfactory receptor-potential Receptor molecule density
Pheromone degrading enzyme
Sensory neuron membrane protein
- Model N
Model with pheromone deactivation by means of the hypothetical enzyme N
- Model R
Model with pheromone deactivation by the receptor molecule R as a catalyst
- Model S
Model with spontaneous pheromone deactivation
- A, Atot
A-form of PBP, with C-terminus in
B-form of PBP, with C-terminus out
Deactivated B-form of PBP, scavenger form
- E, Etot
Pheromone degrading enzyme (=PDE)
Pheromone in air
Active pheromone–PBP complex, able to bind R
Active pheromone–PBP complex
Deactivated pheromone–PBP complex
Activated pheromone–PBP–receptor complex
- N, Ntot
Hypothetical pheromone deactivating enzyme
- R, Rtot
Pheromone receptor molecule
(Concentrations of reaction partners in italics)
Cross-sectional area of the air stream equal to the outline area of the antenna, Eq. 1
Membrane area of the receptor neuron, Eq. 23
(cm−1), average catching effectiveness of the hair, Eq. 1
= 10, estimated volume ratio of neutral/low-pH zone of sensillum lymph space, Eq. 4
Density of receptor molecules in the neuron membrane, Eq. 23
= 1.5 μM, for bombykol–receptor molecule interaction, Nakagawa et al. 2005
= ln 2/t1/2FAR′fall = 0.87/s, adjusted rate constant of pheromone deactivation, chemical model, see Appendix A
Avogadro number (Eq. 22)
Number of hairs per antenna Eq. 1
Number of receptor molecules per receptor neuron, Eq. 22
= 0.83, fraction of adsorbed pheromone binding to PBP, see Appendix A
= 0.25, fraction of adsorbed pheromone activating receptor molecules, see Appendix A
= k−6/(k6 + k−6) = 0.854, Eq. 10
= 1/(K4C + 1) = 0.236, Eq. 7
= k6/(k−5 + k6 + k8R) = 0.254, Eq. 18
= Kd5NQ4K4C/Km7,8, Eq. 71
Fraction of molecules passing the area a that is adsorbed on the antenna, Eq. 1
Fraction of molecules adsorbed that is caught by the hairs, Eq. 1
= 4.5 min, half-life of 83% of pheromone in vivo (Kasang and coworkers 1971–1989)
= 0.8 s, apparent half-life of FAR′, experimental value at the adjustment uptake
= ln 2/k−4 = 29 ms, half-life of F due to reaction FA ⇒ FB, Eq. 21
= 153 ms, total lifetime of FAR and FAR′, model N, Eq. 25
= 24 ms, total lifetime of FAR and FAR′, model R, Eq. 26
(μM/s), pheromone uptake related to the volume of the olfactory hair (2.6 pl), Eq. 1
(μM/s), uptake at which the degrading enzyme is saturated, see Appendix A
Volume of one hair, Eq. 1
Air stream velocity, Eq. 1
Experimental observations together with quantitative modelling led to the suggestion that peripheral events rather than intracellular signalling govern the kinetics of the olfactory receptor-potential in the unadapted receptor neuron (Kaissling 2001). Peripheral events include the adsorptive uptake of odorant molecules from the air space by the olfactory organ, their transport towards the olfactory receptor cell and their interactions with various olfactory proteins such as extracellular odorant-binding proteins (Vogt and Riddiford 1981; Klein 1987; Steinbrecht et al. 1992, 1995), receptor molecules of the receptor neuron (Nakagawa et al. 2005), odorant degrading enzymes (Vogt et al. 1985) and a hypothetical enzyme catalyzing the postulated odorant deactivation (Kaissling 1972). The aim of this paper is to study the contribution of each of these extracellular processes to the response characteristics of the receptor neuron.
For quantitative modelling one needs to know the initial concentration of each reaction partner and the rate constant of each reaction. Until recently only a few of these model parameters had been measured, whereas others were determined indirectly or based on assumptions. Recent studies presented structural and kinetic data on the interaction of the pheromone bombykol and the pheromone-binding protein (PBP) of the silk moth Bombyx mori. From X-ray and NMR analysis it became known that this PBP undergoes conformational changes depending on pH (Sandler et al. 2000; Horst et al. 2001a, b; Klusák et al. 2003; Leal 2004) and on the presence of the ligand (Lautenschlager et al. 2005). The rate constants for pheromone binding by PBP in both conformations, the A-form and the B-form (with the C-terminus inside and outside the central binding cavity, respectively), were measured (Leal et al. 2005a). The velocities of the conformational changes of the two forms upon pH changes were determined in stop-flow experiments (ibid.).
Furthermore, the pheromone-degrading enzyme (PDE) of the moth Antheraea polyphemus, detected by Vogt and Riddiford (1981) and isolated by Vogt et al. (1985), was cloned, and its degradation kinetics were re-investigated (Ishida and Leal 2005). Finally, the receptor molecules for bombykol and bombykal were cloned, and the EC50 for bombykol interacting with the receptor molecules expressed in a heterologous system was determined (Nakagawa et al. 2005). The bombykol receptor molecule was also expressed in an “empty” olfactory neuron of Drosophila melanogaster (Syed et al. 2006).
In view of these findings, the model of perireceptor and receptor events (Kaissling 2001) needs to be updated and modified. We describe the chemical network of perireceptor events leading to the activation of receptor molecules. These processes are considered as extracellular stimulus transformation, while intracellular stimulus transduction leads from the activated receptor molecules to the depolarization of the receptor neuron, i.e. the receptor-potential. We model the kinetics of the receptor-potential following the suggestion of Kaissling (2001) that it is governed by extracellular processes, because intracellular transduction appears to be relatively rapid. This is supported by the recent analysis of intracellular signalling of Gu et al. (2009).
Modelling may help to understand the multiple functions of the PBP (Kaissling 2001), to estimate the density of receptor molecules in the receptor neuron membrane, and to distinguish the measured degradation and the postulated deactivation of the pheromone. Major attention is devoted to the unknown mechanism of odorant deactivation. Two mechanisms were discussed previously, with deactivation catalysed either by the hypothetical enzyme N (model N, Kaissling 1998a, 2001) or by the receptor molecules (model R; Kaissling 1998a, b). Here we treat both models and compare them with a model in which deactivation is a spontaneous, non-enzymatic process (model S). The experimental data were taken from studies of two insect species mainly, the silkmoth, B. mori and the saturniid moth, A. polyphemus.
We discuss the contribution of the PBP, the pheromone degrading enzyme, the pheromone deactivation process and the receptor molecules to the kinetics and the chemical specificity of the receptor-neuron response. Finally, we add in the discussion a possible explanation for the wide range of stimulus concentrations covered by the steady dose–response curve of the receptor-potential.
Description of the models
The chemical model represents a flux detector as opposed to a concentration detector (Kaissling 1998a). A flux detector adsorbs the stimulus molecules depending on both the stimulus concentration within the external medium and the relative velocity of detector and medium. Flux detectors are represented by moth antennae that adsorb pheromone molecules from an airstream. Because during the 2 s of stimulation the stimulus molecules practically do not desorb (Kanaujia and Kaissling 1985) they accumulate and must be deactivated in order to terminate the excitation. For convenience we express the stimulus uptake U and the deactivation as increase and decrease, respectively, of molecule concentrations within the olfactory sensillum per second.
Features retained from previous modelling
After adsorption from the air space at the surface of the olfactory hair, the pheromone (F) moves by random walk along the hair surface and passes through the hair wall via the pore tubules. From the pore tubules the pheromone is transported to the receptor-neuron while bound to the PBP.
Most of the pheromone entering the hair lumen (the fraction Q1) binds to the PBP. This protein solubilizes the hydrophobic stimulus molecules and carries them to the receptor-neuron (Van den Berg and Ziegelberger 1991). A minor portion of the incoming pheromone (1−Q1) encounters the pheromone-degrading enzyme (E) within the sensillum lymph, is rapidly degraded to a metabolite (M) and consequently lost as a stimulus compound.
In vivo the pheromone–PBP complex rather than the free pheromone interacts with the receptor molecules (R) (assumption B in Kaissling 2001). A single activation of the pheromone–PBP–receptor complex is thought to elicit an elementary receptor-potential (Minor and Kaissling 2003).
After the pheromone–PBP and receptor molecule form a ternary complex, the receptor molecule may become activated and induce opening of ion channels. The temporal pattern of the activation of single receptor molecules is reflected by the elementary receptor-potentials observed at weak stimulus intensities (assumption C in Kaissling 2001; Minor and Kaissling 2003).
The pheromone–PBP complex becomes deactivated, with the pheromone remaining chemically intact (cf. assumption D in Kaissling 2001). Odorant deactivation was postulated (Kaissling 1972) in order to explain the finding that the half-life of the pheromone expected from the decline of the receptor-potential after stimulus offset (in the range of 1 s) is about 300-fold smaller than the pheromone half-life measured on the living antenna (4–5 min). Consequently, there must be a process that stops the intact pheromone present within the sensillum lymph (Kanaujia and Kaissling 1985) from stimulating the receptor neuron.
While bound to the PBP the pheromone is largely protected from degradation by the enzyme (E) (assumption E in Kaissling 2001). Protection of pheromone by PBP was shown in vitro by Vogt and Riddiford (1986).
For a flux detector of the type of model R, the “steady” concentration of activated receptor molecules FAR′ increases in linear proportion to the uptake U (Kaissling 1998a). From the various possible slopes for model N we choose a linear increase (assumption F of Kaissling 2001). In both models, the steady FAR′ concentration approaches a maximum value with long-time stimulation at Usat when the deactivating enzyme is saturated. At U > Usat the fall of FAR′ after the stimulus offset is delayed due to accumulation of active stimulus molecules.
For the simulation of the receptor potential we use (as in Kaissling 1998b, 2001) the “quasi-steady” mV-amplitude measured after 2-s stimulation in A. polyphemus, for the receptor-neuron responding to the major pheromone component (E,Z)-6,11-hexadecadienyl acetate (Zack 1979) (Fig. 1a). The amplitude increases over a range of uptakes from 10−6 to 102 μM/s, with a slope much shallower than the one of a linear or the hyperbolic (logistic) function.
Following a re-evaluation of the studies of Kasang (1971, 1973) and Kasang et al. (1988, 1989a, b) on the pheromone degradation in vivo, the fraction of incoming pheromone lost by rapid enzymatic degradation is changed from the previously assumed 1% to the experimental average value of 17%. Accordingly, the fraction of pheromone molecules adsorbed that bind to PBP is Q1 = 83% (see Appendix A).
The two forms (A and B) of the PBP and their conformational changes (Leal et al. 2005a, b) now are included in the model. The new model considers the B-form as a carrier of the pheromone. The complex of the pheromone and the A-form, however, is chosen as the species that interacts with the receptor molecule because it binds the pheromone about 15 times less strongly than the B-form (Leal et al. 2005a).
- 3.In each of the three models discussed here the pheromone deactivation changes the pheromone–PBP complex to an inactive form (FB*) with B* representing the scavenger form of the PBP. In the model N the hypothetical enzyme N deactivates the complex FB (Fig. 2), whereas in the model R the receptor molecule R serves as a catalyst deactivating the complex FA (Fig. 3). For comparison, we use model S with deactivation as a spontaneous first-order reaction that changes FB to FB*.
For simulating the receptor-potential transients, we use the chemical model with a fall time of FAR′ adjusted to the experimental value of t1/2FAR′fall = 0.8 s (Fig. 1). In addition, we discuss the dependence of t1/2FAR′fall on the stimulus intensity observed by Kaissling (1998b).
The chemical model
In all models (for models N and R see Figs. 2, 3, respectively) the pheromone is adsorbed by the hair (reaction 1) and diffuses along the hair surface, through the hair wall via the pore tubules, and—carried by the pheromone-binding protein—towards the receptor neuron. Entering the hair lumen the pheromone (F) binds to one of two reaction partners dissolved in the sensillum lymph—either the pheromone-degrading enzyme (E) or the A-form of the PBP (A). When F binds to the A-form at neutral pH (reaction 2), the complex FB is produced changing the conformation of the PBP. The binding of F and A at low pH forms the complex FA (reaction 3). Upon pH-changes the complex FB may be converted into FA and back to FB (reaction 4). The complex FA is assumed to be the only species binding to the receptor molecule (R) (reaction 5). The ternary complex (FAR) may go to an activated state (FAR′) (reaction 6), which initiates excitation of the neuron via rapid cellular signal processes.
Regarding the pheromone deactivation in model N we consider a version in which the hypothetical enzyme N binds the complex FB (reaction 7). The catalytic reaction 8 produces the deactivated complex FB*, which is unable to activate receptor molecules. In model R the receptor molecule R acts as a catalyst changing the complex FA to the deactivated form FB* (reaction 8). Deactivation occurs by the spontaneous first-order reaction FB ⇒ FB* in model S.
In all of the models, the free pheromone (F) is rapidly degraded to the metabolite (M) by the enzyme (E), via forming the complex (FE) (reaction 9) and the catalytic reaction 10. Reactions 11 and 12, respectively, represent the comparatively slow enzymatic degradation of the pheromone bound to the scavenger form (B*). Finally, the intact pheromone (F) may very slowly dissociate from the deactivated complex (FB*) and serve as stimulus again. This reaction 13 is included in order to simulate the tailing of the receptor-potential observed at very strong stimuli (Kaissling 2001). Most reactions can take place in a forward and in a reversed direction, with the rate constants ki and k−i, respectively. The catalytic steps 8, 10 and 12 are considered to be irreversible.
Reaction1: Uptake of pheromone by the olfactory hairs.
The product Fair·v is the stimulus intensity expressed as molecules per cross-sectional area of the airstream and per second. The factor b depends on the outline area a of the antenna, the fraction Qads of molecules passing a cross-sectional area a of the airstream that is caught by the antenna, the fraction Qh of the molecules adsorbed on the antenna that is caught by the hairs, the volume Vh of the hairs and their number per antenna nh. For sensilla trichodea of the male antenna of A. polyphemus, we use a = 0.8 cm2, Qads = 0.3, Qh = 0.8, nh = 60,000, Vh = 2.6 pl and find b = 1,231/cm. For the shorter hairs of B. mori, we use a = 0.06 cm2, Qads = 0.27, Qh = 0.8, nh = 17,000, Vh = 0.26 pl and find b = 2,932/cm. The values of Fair, Qads, and Qh were determined using 3H-labeled pheromone applied in a turbulent air stream (Steinbrecht 1970, 1973; Kaissling 1971; Steinbrecht and Kasang 1972; Steinbrecht et al. 1989; Kanaujia and Kaissling 1985; Kaissling unpubl.).
During time intervals of a few second no desorption from the antennae was found (Kanaujia and Kaissling 1985). Because the diffusion from the hairs to other parts of the antennae is slow, the amount of pheromone adsorbed on the hairs increases during stimulus exposure. Most of the adsorbed pheromone was found to rapidly enter the hair lumen. After adsorption, the pheromone (F) moves along the hair surface (2D diffusion), through the hair wall via the pore tubules (1D diffusion) and through the sensillum lymph towards the receptor cell (3D diffusion) (Steinbrecht 1973). For modelling diffusion (see Kaissling 1987) we use a diffusion coefficient of 90 μm2/s for transport along the cuticle and pores and of 30 μm2/s within the sensillum lymph while bound to the PBP. These coefficients are based on longitudinal migration of 3H-labeled pheromone on dried and fresh hairs, respectively (Kanaujia and Kaissling 1985). With these coefficients the pheromone molecules reach the receptor-neuron inside the hair (diameter 2–3 μm) within an average time interval of about 10 ms (Kaissling 2001). Because this time is short compared with the half time of the rise of the receptor-potential, it seems adequate to assume immediate encounter of all molecular species of the reaction network. For convenience we express the amount of the membrane-bound molecular species, such as R, FAR and FAR′, as concentrations within the total hair volume (about half of which is spanned by the hair lumen).
The model concentration of PBP, A-form, is set to Atot = 3.8 mM, a value here determined indirectly (see Appendix A). The initial concentration of the B-form (existing only in the complex FB) is zero.
Reaction4: Conformational changes of PBP.
The pheromone–PBP complex (FA) binds to the receptor molecule and activates it. The rate constants are for binding k5N = 0.974/(s μM) and k−5 = 7.7/s, for activation k6 = 16.8/s and k−6 = 98/s. The rate constants k−5, k6 and k−6 resulted from the analysis of elementary receptor-potentials recorded from receptor-neurons of B. mori males stimulated with bombykal (Minor and Kaissling 2003).
After chosing the free parameters Ntot = Etot = 0.5 μM and k−7 = 300/s, we determine k8N = 49.8/s, Km7,8 = 21.9 μM, and k7 = 15.99/(s μM) (see Appendix A).
For the model we use in vitro data obtained for (E,Z)-6,11-hexadecadienyl acetate and the recombinant pheromone-degrading enzyme (PDE) of A. polyphemus (Ishida and Leal 2005):
The rate constants k9 = 300/(s μM) for association and k−9 = 230/s for dissociation of pheromone and enzyme are chosen in order to match the measured Km9,10 and to provide a rapid equilibration of substrate–enzyme binding.
Reaction13: Reactivation of the intact pheromone.
The reaction FB* ⇒ F + B* is included for simulating the tailing of the receptor-potential observed at high stimulus intensities. The experimental data may be fitted with k13 = 0.000008/s.
At first the results of the chemical model will be described. Second the simulation of the receptor potential will be introduced. Finally the influence of various parameters on the simulated receptor potential will be shown. In the analysis we had to mix model parameters obtained from the two species of moths, B. mori and A. polyphemus. Although the pheromone perception in the two species shows many similarities the values calculated here from mixed data sets are very preliminary.
The chemical model
Functions of the pheromone-binding protein
Solubilization of the pheromone
Model concentrations (μM) of free and bound pheromone at the end of 2- and 10-s stimuli with an uptake of 1 μM/s
That the PBP solubilizes the pheromone was shown by binding assays (Kaissling et al. 1985; Du and Prestwich 1995) and by partially replacing the sensillum lymph during electrophysiological recordings (Van den Berg and Ziegelberger 1991). In the latter experiments (with A. polyphemus), the pheromone, dissolved in physiological salt solution with and without PBP, was applied from a glass capillary directly to the receptor-neuron inside the hair lumen. Upon adding PBP the effectiveness of the pheromone increased by 100-fold. Apparently, the pheromone previously adsorbed to the glass capillary was now bound to the PBP and thereby solubilized. The lower increase of solubility in this experiment as compared with the above model prediction (>240-fold) could be due to a residual pheromone binding to the glass capillary.
Protection of the pheromone from enzymatic degradation
In vitro experiments with the isolated pheromone-degrading enzyme (PDE) of A. polyphemus showed that the addition of PBP effectively reduced the velocity of pheromone degradation protecting the pheromone from the enzyme (Vogt and Riddiford 1986). In vivo the pheromone degradation has a biphasic time course (Kasang and coworkers 1971–1989, see Fig. 15): 17% of the pheromone taken up by the antenna is rapidly degraded, 83% (=Q1, see Appendix A) much more slowly. According to the model (inset of Fig. 15), this striking reduction of degradation velocity results mainly from the rapid formation of the complex FB protecting the pheromone from enzymatic degradation.
With Q1 from Kasang and coworkers (1971–1989) and the parameters of degradation in vitro from Ishida and Leal (2005), we find t1/2F = 2.2 ms for A. polyphemus and t1/2F = 2.6 ms from Vogt et al. (1985).
The slow phase of pheromone degradation observed in vivo (Fig. 15) is modelled by reducing the association rate constant k11 of the deactivated pheromone–PBP complex FB* and the degrading enzyme E by 20,000-fold, as compared with k9, the association rate constant for the free pheromone and E.
For simplicity, in our models the pheromone bound to PBP upstream of the receptor activation, i.e. to the forms A and B, is fully protected from degradation. In a model without protection of FA and FB 97% of the pheromone adsorbed would be degraded before reaching the receptor neuron. If FA only is unprotected, 93% would be lost—severely impairing the sensitivity of the system.
Interaction of pheromone and receptor molecule
In conclusion, the sensitivity of the system would be smaller by several orders of magnitude if the free pheromone F alone binds and activates the receptor molecule.
In all three models the pheromone bound to PBP is deactivated by a modification of the PBP from B to the scavenger form B*, which changes FB into FB* (reaction 8). This reaction keeps the pheromone chemically intact but reduces the formation of the active pheromone–PBP complex FA and thus terminates the excitation of the neuron. In two of the models the modification of the PBP is enzymatically controlled (models N and R). In model S (Appendix B) the modification of PBP is a spontaneous and irreversible first-order process.
The number and membrane density of receptor molecules
Pheromone receptor molecules and rhodopsin
dR (% rhodopsin)
Antheraea polyphemus, receptor neuron tuned to (E,Z)-6,11-hexadecadienyl acetate
Bombyx mori, receptor neuron tuned to bombykal
For the receptor-neuron tuned to the pheromone (E,Z)-6,11-hexadecadienyl acetate of A. polyphemus, we use Vh = 2.6 pl and aM = 426 μm2 (Keil 1984b). A respective estimate for the receptor-neuron tuned to bombykal of B. mori uses Vh = 0.26 pl (from data of Steinbrecht 1973) and aM = 60 μm2 (dendrite II, Steinbrecht 1973) and considers the same Usat as for A. polyphemus. The densities of receptor molecules are compared with the density of rhodopsin in the outer disc membrane of dR = 40,000/μm2, which is set to 100% (Dratz and Hargrave 1983).
Generally, all numbers listed in Table 2 are 2.4-fold higher for model N compared with model R. The numbers of receptor molecules per neuron are tenfold higher in A. polyphemus than in B. mori, whereas the membrane densities of both species are relatively similar. They reach up to 15% of the density of rhodopsin in the outer disc membrane of vertebrates.
The temporal characteristics of the activated complex FAR′
In our analysis, we consider average fictive concentrations of FAR′. For the chemical model we determine the steady-state amplitude of FAR′ and its transients, i.e. its rise and fall upon stepwise stimulation. Because the receptor-potentials reached about a constant level with 2-s stimuli, we consider the model FAR′ concentration obtained after 2-s stimulation as quasi-steady-state amplitude. The transients of FAR′ are approximately exponential curves (Fig. 6b) and here characterized by their half-times.
For uptakes up to 1 μM/s the half-times of rise and fall of FAR′ (Fig. 1b, c) are constant and about equal to each other. (Because the steady-state amplitudes are not fully reached after 2-s stimulation, the half-times for the rise are about 20% smaller than those for the fall). At high uptakes near Usat or U1/2max, the half-times of the rise of FAR′ decrease (Fig. 1c), whereas those of its fall increase (Fig. 1b).
With k5RRtotR = 4.36/s and k5NRtotN = 1.62/s the formation of FAR is faster in model R than in models N and S. This implies a faster rise of FAR′ in model R, with half-times shorter by about 100 ms than in model N (Fig. 1c). The fall of the receptor-potential after stimulus offset is faster in model R than in model N, by the same absolute amount of time as its rise (about 100 ms). This difference, however, is hardly noticeable because the fall of the receptor-potential takes two or more seconds.
Simulating the receptor potential
Firstly, we describe the simulation with t1/2FAR′fall = 0.8 s adjusted at 10−2 μM/s (see Appendix A, kfall). While at uptakes up to 1 μM/s the transients of FAR′ after stimulus onset and offset proceed with almost similar velocity (Fig. 1b, c), the predicted receptor potential shows the typical asymmetry of the measured receptor potential. It rises relatively rapidly, with half-times from 400 ms down to less than 50 ms (Fig. 9c), and falls much more slowly, with half-times of 1.5–10 s and more (Fig. 9b). The faster rise of the model receptor-potential as compared with the rise of FAR′ is also demonstrated in Fig. 7.
While FAR′ rises with a constant half-time over a wide range of uptakes, the rise times of the model receptor-potentials decrease with higher uptakes, over the entire range of uptakes. This fits to the measured rise times (Fig. 9c). Model N produces half-times up to 100 ms larger than model R.
The model half-times of the fall of the receptor-potential amplitude (Fig. 9c, d) agree with the data—at uptakes below the “adjustment uptake” (10−2 μM/s, Fig. 1b). At higher uptakes, however, the fall times of the simulated receptor-potential are much (up to about 50%) smaller than those of the measured receptor potential. This discrepancy almost disappears if we use—instead of the adjusted t1/2FAR′fall = 0.8 s of the chemical model—the experimental values of t1/2FAR′fall of 0.5–2 s (Fig. 1b). Using the latter, however, strongly impairs the simulation of the rise times (Fig. 9c, double circles).
The typical tailing (Fig. 8) was observed in recorded receptor-potentials at high stimulus uptakes (Kaissling 1998a, b, Figs. 5, 8). As shown in Kaissling (2001), the tailing of the model response disappears with k13 = 0. Therefore, tailing could indicate a minimal dissociation of the intact pheromone (F) from the deactivated complex (FB*) (reaction 13).
Varying model parameters
Varying the concentration of the PBP
Results similar to those described for varying Atot may be obtained by varying k2 (Figs. 10, 11c, d). A decrease of the dissociation rate constants k−2 and k−3 has no effect. Their increase up to factor of one hundred has hardly visible effects (not shown).
Varying pheromone degradation and deactivation
Removing the pheromone-degrading enzyme has almost no effect on the receptor potential (Fig. 11e, f), whereas the deactivation process strongly affects the transients of the receptor potential (Fig. 11i–l). Interestingly, models N and R may differ in their responses to alterations of a specific parameter (cf. Fig. 11i, j, or k, l). For instance, the alteration of k8N in model N affects the fall of the receptor-potential strongly, but its amplitude only little (Fig. 11k). In contrast, k8R in model R strongly affects the amplitude, but to a smaller extent the fall (Fig. 11l).
The chemical specificity of the receptor-neuron response
In principle, several model parameters may contribute to the chemical specificity of the receptor-neuron response. The examples given here show that alteration of a given model parameter may cause different effects depending on the type of model. Varying the rate constant k4 causes similar but also opposite effects in the two models. A smaller k4 depresses the steady amplitude (after 2 s stimulation) in both models. It accelerates, however, the fall after stimulus offset in model N, but slows down the fall in model R (Fig. 11g, h). Similar differences between the models are seen with varying k5 and Rtot (Fig. 11i, j).
The chemical model of perireceptor and receptor events together with the assumption of relatively fast intracellular signalling describe the kinetics of the receptor potential sufficiently well except for its fall at very high-stimulus uptakes. The results of modelling agree with all experimental findings. This supports the importance in vivo of the pheromone protection from degradation and of the pheromone deactivation postulated in addition to degradation.
The roles of the PBP
There is experimental and model evidence for at least four functions of the PBP. The PBP (1) solubilizes and transports the pheromone, (2) it protects the pheromone from enzymatic degradation, (3) in vivo the pheromone interacts with the receptor molecules while bound to the PBP and (4) the PBP is most likely involved in the postulated odorant deactivation. Finally, this protein serves as an organic anion, with a surplus of nine negative charges per protein molecule. The PBP compensates for the lack of anions found by elementary analysis of the sensillum lymph (Kaissling and Thorson 1980).
The model concentration of the PBP (Atot) was indirectly determined using Eq. 41 based on the assumption that the pheromone after adsorption has two options. Its fraction 1−Q1 encounters the pheromone-degrading enzyme E, while its fraction Q1 binds to the PBP and is protected from enzymatic degradation. The calculated Atot = 3.8 mM (or 3.2 mM, Appendix A) is astonishingly close to the range directly determined in the moth A. polyphemus (5–10 mM) (Vogt et al. 1985; Vogt and Riddiford 1986; Klein 1987). This agreement supports the above assumption of two options. It excludes the previously discussed third possibility that much of the adsorbed pheromone disappears, i.e. becomes lost in a cuticular compartment (Vogt 1987).
By varying the model concentration of the PBP (Atot) it could be shown that an increase of the in vivo concentration would not provide higher steady amplitudes and a more rapid rise of the receptor-potential, and, consequently, not improve sensitivity and temporal resolution of the responses. It is, however, still unclear why the natural PBP concentrations strongly vary, e.g. in cases where several PBPs occur in the same sensilla. Thus, PBP1:PBP2:PBP3 in male moths of A. polyphemus were found in the proportions 70:<1:30 and in Antheraea pernyi in the proportions 50:50:<1, respectively (Maida et al. 2003). Each of the three PBPs binds best one of three pheromone components (compounds 1–3) detected by three cell types that coexist in the same sensilla. Compound 1, the best ligand of PBP1, is the major pheromone component of A. polyphemus and compound 2, the best ligand of PBP2, is the major pheromone component of A. pernyi. Except for the PBP of B. mori the dissociation constants of the PBPs and their pheromone components are unknown.
In male moths of B. mori, each sensillum trichodeum has one receptor neuron for bombykol and one for bombykal (Kaissling et al. 1978). Only one PBP has been found binding bombykol (Maida and Pelosi 1989; Maida et al. 1993, 2005). It mediated cell responses to bombykol only (Pophof 2004; Grosse-Wilde et al. 2006) although it also bound bombykal (after long-time incubation, Graeter et al. 2006; Zhou et al. 2009). There are further PBPs in Bombyx occurring in minute amounts (Maida et al. 1997; Forstner et al. 2006).
Pheromone protection by pheromone–PBP binding
As shown here the high concentration of PBP in vivo may be necessary for rapid binding of the incoming pheromone and hence its protection from enzymatic degradation, on its way towards the receptor neuron. Protection is very effective although not complete; it is modelled by a 20,000-fold smaller affinity of the enzyme E to the complex FB* as compared with the affinity to the free pheromone.
The rapid formation of the complex FB at neutral pH rules out the previously proposed sequential model version in which the incoming pheromone first forms the complex FA1 (at the inner hair wall). Thereafter, FA1 changes to FB for transport, and finally FB turns into FA2 (at the receptor-neuron) for the interaction with the receptor molecule (Kaissling and Leal 2004; Kaissling 2004; Lautenschlager et al. 2005). The reason to exclude this model version is that the rate constant k3 of formation of FA is about tenfold smaller than k2. The slow initial formation of FA1 in the sequential model would mean an impaired protection from pheromone degradation. This may be simulated by removing k2 from Eq. 41. The calculation reveals Q1 = 0.32, which means that 68% (instead of the measured 17%) of the incoming pheromone would be lost. Therefore, in the network discussed here the complex FB is formed (reaction 2), in parallel to FA (reaction 3).
It seems counterintuitive that the association rate constant at neutral pH (k2) is tenfold larger than at low pH (k3), and that the dissociation rate constants (k−2 and k−3) hardly depend on pH (Figs. 4, 5). At neutral pH the pheromone associating with the PBP A-form should need more time to displace the C-terminus from the inner binding cavity and to induce the change of the A-form into the B-form. At low pH, however, when the inner binding cavity is occupied by the C-terminus, the pheromone merely could bind to hydrophobic sites on the periphery of the PBP A-form.
Interestingly, bovine serum albumin was shown to be able to perform at least two functions of the PBP. The albumin solubilized the pheromone (Van den Berg and Ziegelberger 1991) and protected it from the enzymatic degradation (Vogt and Riddiford 1986), both as effectively as the PBP. It remains to be seen of whether the albumin also could fulfil other functions of the PBP as mediating the interaction with the receptor molecule or the pheromone deactivation.
Pheromone–PBP–receptor molecule interaction
A direct interaction of the free pheromone with the receptor molecules may be possible in experiments in which high pheromone concentrations were used (Syed et al. 2006). In experiments without the natural binding protein one should exclude that other proteins are present and replace its function. It seems clear, however, that in vivo, in the presence of PBP, the pheromone–PBP complex rather than the free pheromone F interacts with the receptor molecules. Modelling reveals that the concentration and life-time of the active complex FA are much larger than the one of the free pheromone F (>50-fold and >10-fold, respectively, see Appendix A). Consequently, if F instead of FA interacts with the receptor molecules, it would constitute a very ineffective system.
As proposed previously (Kaissling 2001), the pheromone in the excitatory complex FA could be associated to hydrophobic patches on the outer side of the protein possibly facilitated by the dimeric structure of the PBP. That the PBP occurs as a dimer was suggested by Kaissling et al. (1985) and finally proven by Campanacci et al. (1999) and Leal (2000). Remarkably, binding to the surface of the A-form allows the pheromone to interact with the receptor molecule but protects it from the degrading enzyme.
Experiments in A. polyphemus with direct application of PBP and pheromone components during electrophysiological recordings support the idea that PBP is involved in the pheromone–receptor molecule interaction. The receptor-neuron, type 1, tuned to the pheromone component 1 responded to the normally ineffective component 2 when the latter was offered together with PBP1. Obviously, the PBP1 mediated the interaction of neuron type 1 with the “wrong” pheromone component 2 (Pophof 2002, 2004). Applying the PBP of a different moth species (ApolPBP1 from A. polyphemus) in B. mori produced a response of the bombykol receptor-neuron even with no bombykol present (Pophof 2004). The bombykal receptor-neuron present in the same sensillum did not respond which supports the idea of a specific interaction between binding protein and receptor molecule.
The proposed mediator function of the PBP is supported by findings in Drosophila melanogaster. The pheromone-binding protein LUSH is required to activate receptor-neurons by the pheromone (Z)-11-vaccenyl acetate (Xu et al. 2005). Recently, it was shown that the pheromone induces an activated conformation in the PBP, which is recognized by the neuronal receptor molecules (Laughlin et al. 2008). If this occurs also in Bombyx it would require two A-forms of the PBP, the inactive form (A) present in the absence of the pheromone and an active form induced by binding the pheromone (FA′). In Drosophila, the LUSHD118A mutant simulating the structure of the active PBP activated the receptor neuron—in the absence of the pheromone (ibid.). For the response to LUSHD118A the neuronal receptor molecule Or67d and also sensory neuron membrane protein (SNMP) was necessary.
Model N or R?
Models R and N have been introduced by Kaissling (1998a) and further discussed by Kaissling (1998b, 2001), respectively. Model S with spontaneous deactivation as a first-order process (Appendix B) may be ruled out because it does not appropriately simulate the pronounced saturation kinetics of the receptor potential (Fig. 8). Thus, the models N and R with enzymatic deactivation remain to be discussed. Both models are based on the special physiological quantities Usat (=30 μM/s) and kfall (=0.87/s). There are a few minor differences between the two models. Model R has fewer receptor molecules, but a larger k5. In model R the receptor-potential rises faster due to a faster formation of the complex FAR. The rise times of the measured receptor-potential are simulated by model R slightly more exactly than by model N (Fig. 11c, d). Certainly a faster rise of the receptor-potential is useful to resolve repetitive stimuli of higher frequency which may be advantageous for orientation in a turbulent odour plume (Kaissling 1997). The differences in rise times, however, seem too small for favouring one of the models.
Model R is supported by recent studies showing that properties of the olfactory receptor-potential kinetics were transferred together with genes of receptor molecules expressed in an “empty” olfactory neuron (Dobritsa et al. 2003; Hallem et al. 2004; Syed et al. 2006).
Model N was preferred by Kaissling (2001) since the putative receptor molecule blocker decyl-thio-1,1,1-trifluoro-propanone (Pophof 1998; Pophof et al. 2000; Kaissling 2004) did not seem to interfere with the odorant deactivation. Thus, the application of this blocker produced smaller receptor-potentials but did not change the half-time of their fall after stimulus offset. These effects agree with model N if the blocker reduces k5 or Rtot (see Fig. 11i). In contrast, for model R a reduction of k5 or Rtot would slow down the fall of the potential (see Fig. 11j), but this has not been observed.
Because the smaller value of TcR is not compatible with the measurements of Minor and Kaissling (2003), model R appears obsolete.
In conclusion, the arguments in favour of model N seem more convincing. It should be noted that the model N would work as well if the enzymes N and E are the same protein. It seems, however, unlikely that different tasks, such as the pheromone degradation (F ⇒ M) and the modification of the PBP (FB ⇒ FB*) required for deactivation are done by the same enzyme.
It is common to all three models discussed that the mechanism of deactivation must involve a modification of the PBP to the scavenger form B* while the pheromone bound to B* remains chemically intact. In the previous model N (Kaissling 2001), odorant deactivation was achieved by a transformation of the PBP molecule from a reduced “transport” form (Bred) into an oxidized “scavenger” form (Box). This mechanism was suggested by the apparent redox shift of the pheromone–PBP complex observed in vitro (Ziegelberger 1995). The redox shift was shown to occur in the presence of a catalyst contained within the olfactory hairs, represented in our models by the hypothetical enzyme (N) or the receptor molecules (R). The redox-shift became questionable when Leal (2003) did not find the expected reduction of mass units. A final judgement about this phenomenon appears premature because there is other experimental evidence in favour of a redox shift (Ziegelberger 1995). In the present paper we leave the redox shift aside but keep hold of the models N and R, with the deactivated (or scavenger) form (B*) of the PBP.
A possible mechanism of forming a scavenger PBP (form B*) may be proposed for model N. In this model the postulated enzyme N is able to distinguish between the pheromone–PBP complex FA and those PBP molecules carrying a stimulus molecule inside the inner binding cavity, the complex FB. We propose—as a result of a discussion with F. Damberger and W. Leal—that the enzyme N might be able to recognize the exposed hydrophobic C-terminal tail of the B-form and to discriminate it from the exposed hydrophilic N-terminal tail of the A-form. The enzyme N could remove or block the C-terminal tail of FB and thus prevent FA from being formed.
This idea is supported by experimental removal of the C-terminus, which eliminated the FB ⇒ FA transformation at low pH. The pheromone was irreversibly locked inside the binding cavity of the truncated PBP (Leal et al. 2005a). This way the pheromone could be made “invisible” to the receptor molecule. Furthermore, the PBP-pheromone binding at low pH was maintained by one-point mutation of the C-terminus (Xu and Leal 2008). Apparently, the formation of a C-terminal alpha-helix—necessary for the repulsion of the pheromone from the inner binding cavity—was blocked.
Numbers of receptor molecules, ion channels and SNMP
The estimated densities of olfactory receptor molecules are by far higher than the presumed density of ion channels in the plasma membrane of the olfactory receptor-neuron. Attempts to estimate the latter revealed a minimum of 10,000 ion channels per receptor neuron of A. polyphemus with a conductance per channel of 30 pS (Kaissling and Thorson 1980). This corresponds to a channel density of 23 per μm2 and fits to the number of about 20 putative ion channels per μm2 estimated from atomic-force microscopy of dendritic membranes (Kaissling and Kumar 1997; Eschrich et al. 1998).
Thus, the numbers of receptor molecules per ion channel would amount to roughly 4,000/20 = 200. This ratio would imply a large average distance between receptor molecules and ion channels, much higher than expected from a direct coupling of receptor molecules and adjacent ion channels. From geometrical reasons, for direct coupling a ratio below ten receptor molecules per ion channel seems more likely (Wicher et al. 2008; Sato et al. 2008). This small ratio could be reached either by a smaller number of receptor molecules, or a larger number of ion channels, perhaps with a smaller conductance per channel. The large numbers of receptor molecules are required for the wide range of stimulus intensities covered by the dose–response curves of the receptor-potential.
Recently it has been found in Drosophila that the receptor molecules are associated with the SNMP (Benton et al. 2007) and that this protein is required for pheromone sensitivity (Jin et al. 2008). The density of SNMP molecules may be roughly estimated from electron-micrographs showing gold-labelled antibodies against SNMP in olfactory sensilla of A. polyphemus. From the micrographs in Rogers et al. (2001) 300 gold particles/μm2 of the membrane of pheromone receptor-neurons may be counted. This figure corresponds to a minimum of about 5% of the density of receptor molecules in A. polyphemus calculated for model N. The density of SNMP could, however, well be higher if only a small fraction of the SNMP molecules carried a gold particle.
EC50 of the pheromone–receptor molecule interaction
Nakagawa et al. (2005) determined the EC50 = 1.5 μM for bombykol and the heterologously expressed bombykol receptor molecule. The EC50 provides a maximum estimate of the dissociation constant of the pheromone and receptor molecule interaction and may be compared with the model EC50 of the complex FA and the receptor molecule. For both models we find EC50 = 6.8 μM (EC50 = Kd5NQ4 for model N, or EC50 = Km5,8Q4 for model R). Considering that our model uses data from two species of moths, and it yields an EC50 for binding the pheromone–PBP complex rather than the free pheromone, a closer agreement with the results of Nakagawa et al. is not expected.
The receptor-potential kinetics differs from the one of FAR′ because it depends—in addition to FAR′—on other factors such as the electrical circuit of the sensillum and on intracellular transduction processes. While in models N and R the steady FAR′ concentration rises in linear proportion to the uptake, the dependence of the “steady” amplitude of the receptor-potential on the uptake—and on FAR′—is highly nonlinear (Fig. 1a).
For our simulation of the receptor-potential transients, we used the method of FAR′–mV conversion. The underlying assumption of very fast intracellular signalling is supported by the recent analysis of Gu et al. (2009). For a theoretical, stepwise onset of FAR′ they found that the half-time of the rise of the receptor-potential would be 16 ms only. Our measured half-times were much longer, 400 ms at weak, and 50 ms at strong stimulation (Fig. 11e, f). The half-time of the receptor-potential fall would be—according to these authors—about 1 s at weak and 2.2 s at strong stimulation, whereas the measured half-time in A. polyphemus was 1.5 and 17 s, respectively (Fig. 9c, d). A fast signalling may also be expected from the direct coupling of receptor molecules and ion channels (Wicher et al. 2008; Sato et al. 2008). Thus, our assumption of fast intracellular signalling seems to be correct and justifies our method of simulating receptor potential by the FAR′–mV conversion (see “Simulating the receptor potential”).
As described in “Results”, the simulation of the rise of the receptor-potential was satisfactory if we use the chemical model with the adjusted value of t1/2FAR′fall = 0.8 s, the half-time of the fall of FAR′, the concentration of activated receptor molecules. The simulation of the fall of FAR′ was, however, incorrect at higher stimulus uptakes. This discrepancy was shown to be due to the measured increase of t1/2FAR′fall occurring at uptakes far below saturation (Kaissling 1998b; Fig. 1b). Since the increase of t1/2FAR′fall is not explained by the chemical model, we conclude that it is due to intracellular processes developing during the 2 s of stimulation. The rise of the receptor potential, however, is apparently governed by the extracellular processes. Besides the measured values of t1/2FAR′fall of 0.5–2 s for A. polyphemus there is available only the value of 0.34 s estimated for a receptor-neuron of B. mori very weakly stimulated with bombykal (Fig. 23 in Kaissling 1987).
In our models the delayed fall of FAR′ and the receptor-potential after offset of strong stimuli (near to, or above Usat) is due to a saturation of the deactivation mechanism causing accumulation of mainly FB and the active stimulus complex FA within the sensillum. The delayed fall of the receptor potential has been frequently observed in pheromone–receptor neurons (Kaissling 1971, 1987, 2001). As shown by Kaissling (1971), the delayed fall even occurs with pheromone derivatives that produce smaller maximum receptor-potential amplitudes than the pheromone. Smaller maximum amplitudes of the receptor potential may be produced by the chemical model, e.g. if the pheromone derivative induces a smaller activation of the receptor molecule by an increased rate constant k−6.
The tailing of the receptor potential after offset of strong stimuli disappears if reaction 13 is omitted. This suggests that deactivation is, to some degree, reversible, and that stimulus molecules may activate receptor molecules for a second time.
In summary, the simulation shows that the saturation effects and the tailing of the response may be produced by perireceptor events.
The shallow dose–response curve
The asymmetric shape, i.e. the fast rise and the much slower fall of the receptor potential, is a consequence of the nonlinear slope of the steady dose–response curve covering a range of stimulus intensities much wider than covered by the standard hyperbolic binding or logistic curve. Part of the shallow slope may be due to shortening the electrical length constant of a long dendrite with increasing stimulation and increasing electrical membrane conductance of the neuron (Kaissling 1971; Vermeulen et al. 1997). As suggested by Gu et al. (2009) this slope may in addition be produced, if elements of the intracellular signalling cascade or specific types of ion channels become active at different stimulus intensities.
An additional explanation so far not considered is the varying effectiveness of molecule capture along the length of the olfactory hairs. Thus, the distal half of the long hairs of A. polyphemus caught 70% of the radiolabeled pheromone molecules caught by the entire hairs (Kanaujia and Kaissling 1985). This could mean that receptor molecules located near the hair base receive far fewer stimulus molecules than those near the hair tip.
The chemical specificity of the receptor-neuron response
Certainly a specific detector must be bound to each receptor neuron since usually two or more neurons tuned to different pheromone components innervate the same sensillum and share the same sensillum lymph space. For example, the receptor neuron of B. mori tuned to bombykol responds to bombykal if the latter is offered at a 10,000- to 100,000-fold higher concentration (Kaissling et al. 1978). As shown in “Results” several model reactions may contribute to the specificity of the receptor-neuron response. The alteration of a single model parameter such as an increase of k−6 may strongly change the receptor-potential kinetics. In fact, the described alterations of the steady dose–response curve upon stimulation with pheromone derivatives (Fig. 12) were observed together with an additional effect: a smoother, less fluctuating time course of the receptor potential (Kaissling 1974, 1977, 1987, 1998a). The latter effect may as well be explained by an increased k−6. With a larger k−6, the single receptor molecule activations—reflected by the elementary receptor potentials (“bumps”)—last a smaller time, too small to be resolved due to low-pass filtering by capacitances of the sensillum circuit (Kaissling and Thorson 1980; Minor and Kaissling 2003). The example of varying k−6 supports the assumption that the specificity of the receptor-neuron response largely depends on the specificity of the stimulus–receptor molecule interaction, more on receptor activation rather than binding alone. It should be noted that adaptation after strong stimuli may cause similar alterations of the steady dose–response curves (Zack 1979; Kaissling 1987) as observed with pheromone derivatives (Fig. 12). This could indicate that adaptation affects the activation of the receptor molecule.
Our models show that interactions of the stimulus compound with extracellular proteins other than the receptor molecules, such as PBPs and enzymes, may contribute to the chemical specificity of the receptor-neuron response, but apparently to a smaller extent (Steinbrecht 1996). Varying Atot merely shifts the dose–response curves along the stimulus axis (Fig. 10). Thus, the specificity of the response might indeed depend more on the interaction with the receptor molecule than with the PBP even if the affinity to the receptor molecule is weaker than to the PBP (Kd5N > Kd2, Kd30). In vitro studies with isolated PBP and pheromone derivatives reveal that the specificity of binding to PBP is considerably smaller than of the neuron response, as, e.g. in A. polyphemus (De Kramer and Hemberger 1987; Meng et al. 1989; Prestwich et al. 1995; Oldham et al. 2000; Maida et al. 2003; Mohl et al. 2002), Lymantria dispar (Hansen 1984; Plettner et al. 2000; Kowcun et al. 2001), or B. mori (Zhou et al. 2009). The only case known so far of a noticeable specificity of pheromone–PBP binding is the major PBP of B. mori males which bound bombykol, but did not bind bombykal (A. Svatos, personal communication. Cf. “The roles of the PBP”).
Almost no effects on the response are produced by altering the pheromone degrading enzyme. Removal of the pheromone degradation in the model, e.g. by using E = 0, hardly changes the time course of the receptor-potential within a range of a few seconds after stimulation (Fig. 11e, f). This was concluded also from the finding that normal electrophysiological responses were recorded from antennae showing no activity of the pheromone degrading enzyme (Maida et al. 1995). Thus, it seems clear that the fall of the receptor potential after stimulus offset is not caused by pheromone degradation and that pheromone deactivation must occur.
Pheromone degradation seems to be little specific. Hexadecanol, a compound ineffective to the receptor-neuron, and bombykol were enzymatically degraded in vivo with similar velocity (Kasang and Kaissling 1972). In vitro studies revealed little differences between the degradation of the pheromone component (E,Z)-6,11-hexadecadienyl acetate and 2-naphthyl acetate by the isolated sensillar esterase (Vogt et al. 1985).
An example of impaired enzymatic degradation might be the case of (E,Z)-4,6-hexadecadiene that produced almost normal receptor potentials if applied at concentrations about 100-fold higher than bombykol. The potential ceased after stimulus offset indicating the deactivation of the alkene. The nerve-impulse response, however, lasted for many minutes at a low level (Kaissling et al. 1989). This means that the deactivation did not completely remove the stimulant. Obviously, the alkene was not degraded by dehydrogenation as found for bombykol (Kasang et al. 1989b). This experiment shows the significance of enzymatic pheromone degradation: the total removal of active pheromone that is necessary to recover the high sensitivity of the receptor-neuron.
According to the model, stronger effects on the neuron response are expected from altering the hypothetical pheromone deactivation responsible for the fall of the receptor potential after stimulus offset (Fig. 11i). Pheromone deactivation, however, seems much less specific than the receptor-neuron response. The fall observed with less effective bombykol derivatives is sometimes slowed down, but for most test compounds accelerated. The half-life of the fall may be reduced to about 10% of the value with bombykol stimulation (Kaissling 1974, 1977, 1998a). As shown above, however, the fall may also depend on model parameters (e.g. k−6) other than those of the deactivation process.
Summary of the temporal model characteristics
The modelling demonstrates the gaps of our knowledge and may help to find strategies for further work. Certainly it would be most desirable to have a complete set of biochemical, electrophysiological and fine-structural data for one animal species. Quantitative data on the interaction of binding protein, SNMP, receptor molecule and ion channel are needed. The process of pheromone deactivation is an essential postulate that needs to be experimentally verified; the proposed mechanism needs to be tested. An alternative model without pheromone deactivation has not been published. How PBP and bovine serum albumin protect the pheromone from enzymatic degradation seems an interesting question of molecular biophysics.
The computer program was supplied by John Thorson (described in Kaissling 2001) who passed away in June 2008. I have much to thank him not only for his cooperation over the years and his painstaking, uncompromising criticism but also for his generous and humorous discussion. Much gratitude for the help for clarity and linguistic improvement goes to Ann Biederman-Thorson, also for checking an earlier version of this manuscript. Thanks for discussion and help to many colleagues, among them Walter S. Leal, Jean-Pierre Rospars, John G. Hildebrand, one unknown referee, and last but not least Friedrich Barth for invaluable advice to improve the structure of the paper.
This article is distributed under the terms of the Creative Commons Attribution Noncommercial License which permits any noncommercial use, distribution, and reproduction in any medium, provided the original author(s) and source are credited.
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