1. Synaptic vesicles were isolated and fused into large structures wit
h a diameter of more than 20 mu m to characterize their ionic channels
. The 'cell'-attached and inside-out configurations of the patch clamp
technique were used. 2. Two types of ion channels were most frequentl
y observed: a low conductance chloride channel and a high conductance
non-specific channel. 3. The non-specific channel has a main conductin
g state and a substate. The main conducting state has a slope conducta
nce of 246 +/- 15 pS (+/- S.E.M., n = 15), in the presence of differen
t combinations of KCl and potassium glutamate.4. From the reversal pot
entials of the current-voltage (I-V) relation, it was concluded that t
his channel conducts both Cl- and K+. 5. The non-specific channel is h
ighly voltage dependent: under steady-state voltages it has a high ope
n probability near 0 mV and does not inactivate; when the membrane is
hyperpolarized (pipette side more positive), the open probability decr
eases dramatically. 6. Voltage pulses showed that upon hyperpolarizati
on (from holding potentials between -20 and +20 mV), the channels deac
tivated; when the membrane was stepped back to the holding potential,
the channels reactivated rapidly. 7. In a. number of experiments, when
the pipette side was made more negative than the bath, the open proba
bility also decreased. 8. Frequently, a substate with a conductance of
about 44 +/- 4% (+/- S.E.M., n = 3) of the main state was detected. 9
. We speculate that this non-specific ion channel may have different r
oles at the various stages of the life cycle of the synaptic vesicle.
When the synaptic vesicle is an intracellular structure, it might help
its transmitter-concentrating capacity by dissipating the polarizatio
n. After fusion with the surface membrane, it might constitute an addi
tional conductance pathway, taking part in frequency modulation of syn
aptic transmission.