Abstract
The temperature dependence of the transport kinetics of flounder Na+-coupled inorganic phosphate (Pi) cotransporters (NaPi-IIb) expressed in Xenopus oocytes was investigated using radiotracer and electrophysiological assays. 32Pi uptake was strongly temperature-dependent and decreased by ∼80% at a temperature change from 25°C to 5°C. The corresponding activation energy (E a) was ∼14 kcal mol−1 for the cotransport mode. The temperature dependence of the cotransport and leak modes was determined from electrogenic responses to 1 mM Pi and phosphonoformic acid (PFA), respectively, under voltage clamp. The magnitude of the Pi- and PFA-induced changes in holding current decreased with temperature. E a at −100 mV for the cotransport and leak modes was ∼16 kcal mol−1 and ∼11 kcal mol−1, respectively, which suggested that the leak is mediated by a carrier, rather than a channel, mechanism. Moreover, E a for cotransport was voltage-independent, suggesting that a major conformational change in the transport cycle is electroneutral. To identify partial reactions that confer temperature dependence, we acquired presteady-state currents at different temperatures with 0 mM Pi over a range of external Na+. The relaxation time constants increased, and the peak time constant shifted toward more positive potentials with decreasing temperature. Likewise, there was a depolarizing shift of the charge distribution, whereas the total available charge and apparent valency predicted from single Boltzmann fits were temperature-independent. These effects were explained by an increased temperature sensitivity of the Na+-debinding rate compared with the other voltage-dependent rate constants.
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Notes
The dependence of z on [Na+] is a consequence of fitting a single Boltzmann function to the Q-V data. The valence estimated from the single fit is a weighted value that depends on the relative contributions from the empty carrier and Na+ binding partial reactions. Similar behavior was observed by fitting a single Boltzmann to presteady-state data generated by a three-state model that simulates the empty carrier and one voltage-dependent Na+ binding step (I. C. Forster, unpublished data).
In applying this model to NaPi-IIb, we have lumped the empty carrier transition (1–8, Fig. 6A) and Na+ binding transitions (1–2a, 2a–2b) into a single transition. A more accurate description of the presteady-state kinetics would require fitting the presteady-state relaxations to >2 exponentials and using at least a two Boltzmann fit to the data. We were unable to extract more than one component of nonendogenous presteady-state charge movement by exponential curve fitting with confidence. Moreover, attempts to fit a double Boltzmann function to our Q-V data (e.g., as undertaken by Krofchick, Huntley and Silverman [2004] for SGLT1) were equally unsuccessful because of fit uncertainties with the larger number of free parameters.
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Acknowledgement
This work was supported by grants to H. M. from the Swiss National Science Foundation and the Gebert Rüf Foundation (http://www.grstiftung.ch).
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Bacconi, A., Ravera, S., Virkki, L.V. et al. Temperature Dependence of Steady-State and Presteady-State Kinetics of a Type IIb Na+/Pi Cotransporter. J Membrane Biol 215, 81–92 (2007). https://doi.org/10.1007/s00232-007-9008-1
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DOI: https://doi.org/10.1007/s00232-007-9008-1