HCECs were transfected with pZip-control, or pZip-miR-205 or pCDH-miR-205 lentiviral particles as described above. Within 24 hours after transfection, the cells were treated with TrypLE Express (Life Technologies) for 10 minutes to detach the cells. The perforated whole-cell patch-clamp experiments were carried out at room temperature. The cells were incubated with a bath solution containing 140 mM KCl, 0.5 mM MgCl
2, 1.5 mM CaCl
2, and 10 mM HEPES (pH 7.4). Borosilicate glass (1.7-mm OD) was used to make the patch-clamp pipettes that were pulled with a Narishege electrode puller (Narishege, Inc., Long Island, NY). The pipette had a resistance of 2 to 4 MΩ when filled with 140 mM KCl. The tip of the pipette was filled with pipette solution containing 140 mM KCl, 2 mM MgCl
2, 1 mM EGTA, and 5 mM HEPES (pH 7.4). The pipette was then back-filled with amphotericin B (20 μg/0.1 mL) containing pipette solution. After forming a high-resistance seal (>2 GΩ), the membrane capacitance was monitored until the whole-cell patch configuration was formed. The cell membrane capacitance was measured and compensated. The K
+ currents were measured by an Axon 200A patch-clamp amplifier (Molecular Devices, Sunnyvale, CA). The currents were low-pass filtered at 1 KHz and digitized by an Axon interface (Digidata 1200) and data were stored in an IBM-compatible computer and were analyzed using the pClamp software system 9 (Axon; Molecular Devices). K
+ currents were presented as picoamperes/25 picofarads. The same patch-clamp equipment described above was used for the single channel recording and the pipette solution contains (in mM) 140 KCl, 1.8 MgCl
2, 10 HEPES (pH = 7.4). The currents were low-pass filtered at 1 KHz and digitized by an Axon interface. Data were analyzed using the pClamp software system 9 (Axon; Molecular Devices). Channel activity defined as NP
o (a product of channel
number and open
probability) was calculated from data samples of 60 seconds' duration in the steady state as follows:
where
ti is the fractional open time spent at each of the observed current levels. The channel conductance was determined by measuring the current amplitudes over several voltages.