Patch-clamp recordings (in whole-cell or inside-out configuration) were performed by using an EPC10 amplifier (HEKA Elektronik, Germany) controlled by PATCHMASTER. Patch pipettes were made from borosilicate glass and fire-polished to a resistance of ~3 MΩ. Both the pipette and the bathing standard solution contained 140 mM NaCl, 5 mM KCl, 2 mM MgCl
2, 2 mM CaCl
2, 10 mM HEPES, and 10 mM glucose (pH 7.4, adjusted with NaOH). The different pH values of bathing solution were adjusted with HCl. To record the currents evoked by increased temperatures, the membrane potential was held at −60 mV. For bi-ionic reversal potential measurements of monovalent ions, after the whole-cell configuration was obtained in standard solution, the bathing solution was changed to 140 mM NaCl (or KCl or CsCl), 10 mM HEPES, and 10 mM glucose (adjusted to pH 6.1 with NaOH, KOH, or CsOH, respectively). For divalent cation permeability experiments, the bathing solution was changed to 110 mM MgCl
2 (or CaCl
2 or BaCl
2), 2 mM Mg(OH)
2 [or Ca(OH)
2 or Ba(OH)
2], 10 mM HEPES, and 10 mM glucose, pH 6.1 (adjusted with HCl). Given that the frequent perfusion of different bathing solutions disturbed stability of temperature control, each recorded cell experienced only one exchange of bathing solution. Therefore, currents in the presence of different bathing solutions were normalized to the value at +80 mV before liquid junction potentials were corrected. A voltage ramp was employed to indicate the reversal membrane potential. Permeability ratios for monovalent cations to (
PX/
PNa) were calculated as previously described (30 (
link)):
PX/
PNa = exp(Δ
VrevF/
RT), where
Vrev presents the reversal potential,
F represents Faraday’s constant,
R is the universal gas constant, and
T is absolute temperature. For measurements of divalent permeability,
PY/
PNa = [Na
+]
i exp(Δ
VrevF/
RT)(1 + exp(Δ
VrevF/
RT))/4[Y
2+]
o, where the bracketed terms are activities. Assumed ion activity coefficients are 0.75 for monovalents and 0.25 for divalents. To record the heat activation of BRTNaC1 in the presence of physiological solution, the bathing solution contained (in mM) 120 NaCl, 5 KCl, 4 MgCl
2, 1.5 CaCl
2,10 N-Tris-(hydroxymethyl)-methyl-2-amino-ethanesulfonic acid (TES), 25 proline, and 5 alanine. Physiological pipette solution contained (in mM) 140 K gluconate, 10 TES, 4 Mg adenosine triphosphate, 2 MgCl
2, and 0.4 Na guanosine triphosphate. For inhibitor screening, the perfusion and solution switching were carried out by a gravity-driven system (RSC-200, BioLogic). The solutions flowed through separated tubes to minimize mixing of the solutions. The patches were placed at the perfusion tube outlet.
The experimental apparatus for laser irradiation was as previously reported (31 (
link)), where the energy of laser photons was absorbed by water molecules and converted to thermal energy. Briefly, a controller (Thorlabs, maximal optic output power set at 300 mW) was used to drive a laser diode (Fitel), which generated the laser beam with an emission peak of 1,443 nm. The patch pipette tip was placed in front of the center of the optical fiber so that the cells or patches could be heated by different temperatures. To calibrate the relationship between laser driving power (indicated by voltage) and temperature (in °C), the temperature of bathing solution (room temperature, n = 5) and the recorded boiling points of pure ethanol or water (n = 5 for each) were used to fit this relationship using a two-point method. The data points were fitted to a linear equation that describes the relationship between laser driving power and temperature.
Yao Z., Yuan L., Chen X., Wang Q., Chai L., Lu X., Yang F., Wang Y, & Yang S. (2023). A thermal receptor for nonvisual sunlight detection in myriapods. Proceedings of the National Academy of Sciences of the United States of America, 120(8), e2218948120.