A method for exceptionally low noise single channel recordings

Summary We present a method whereby, with integrating electronics, quartz patch electrodes and a novel use of silicone oil, background noise levels as low as .083 pA RMS in a 5 kHz bandwidth (4-pole Butterworth filter) have been achieved in single channel patch clamp recordings. These approaches result in much higher signal to noise ratios for single channel recording than have previously been reported and should allow many investigators to significantly reduce noise at a constant bandwidth or to increase their recording bandwidths by several kHz.     

Isolated perfused rabbit colon crypts: stimulation of Cl− secretion by forskolin

The aim of this study was to characterize ion conductances and carrier mechanisms of isolated in vitro perfused rabbit colonic crypts. Crypts were isolated from rabbit colon mucosa and mounted on a pipette system which allowed controlled perfusion of the lumen. In non-stimulated conditions basolateral membrane voltage (V _b1) was –65±1 mV (n=240). Bath Ba²⁺ (1 mmol/ l) and verapamil (0.1 mmol/l) depolarized V _b1 by 21±2 mV (n=7) and 31±1 (n=4), respectively. Lowering of bath Cl^– concentration hyperpolarized V _b1 from –69±3 to –75±3 mV (n=9). Lowering of luminal Cl^– concentration did not change V _b1. Basolateral application of loop diuretics (furosemide, piretanide, bumetanide) had no influence on V _b1 in non-stimulated crypts. Forskolin (10^–6 mol/l) in the bath depolarized V _b1 by 29±2 mV (n=54) and decreased luminal membrane resistance. In one-third of the experiments a spontaneous partial repolarization of V _b1 was seen in the presence of forskolin. During forskolin-induced depolarization basolateral application of loop diuretics hyperpolarized V _b1 significantly and concentration dependently with a potency sequence of bumetanide > piretanide furosemide. Lowering bath Cl^– concentration hyperpolarized V _b1. Lowering of luminal Cl^– concentration from 120 to 32 mmol/l during forskolin-induced depolarization led to a further depolarization of V_b1 by 7±2 mV (n=10). We conclude that V_b1 of rabbit colonic crypt cells is dominated by a K⁺ conductance. Stimulation of the cells by forskolin opens a luminal Cl^– conductance. Basolateral uptake of Cl^– occurs via a basolateral Na⁺ : 2Cl^– : K⁺ cotransport system.     

Regulation and possible physiological role of the Ca2-dependent K+ channel of cortical collecting ducts of the rat

In the luminal membrane of rat cortical collecting duct (CCD) a big Ca²⁺-dependent and a small Ca²⁺-independent K⁺ channel have been described. Whereas the latter most likely is responsible for the K⁺ secretion in this nephron segment, the function of the large-conductance K⁺ channel is unknown. The regulation of this channel and its possible physiological role were examined with the conventional cell-free and the cell-attached nystatin patch-clamp techniques. Patch-clamp recordings were obtained from the luminal membrane of isolated perfused CCD segments and from freshly isolated CCD cells. Intracellular calcium was measured using the calcium-sensitive dye fura-2. The large-conductance K⁺ channel was strongly voltage- and calcium-dependent. At 3 mol/l cytosolic Ca²⁺ activity it was half-maximally activated. At 1 mmol/l it was neither regulated by cytosolic pH nor by ATP. At 1 mol/l Ca²⁺ activity the open probability (P _o) of this channel was pH-dependent. At pH 7.0 P _o was decreased to 4±2% (n=9) and at pH 8.5 it was increased to 425±52% (n=9) of the control. At this low Ca²⁺ activity the P _o of the channel was reduced by 1 mmol/l ATP to 8±4% (n=6). Cell swelling activated the large-conductance K⁺ channel (n=14) and hyperpolarized the membrane potential of the cells by 9±1 mV (n=23). Intracellular Ca²⁺ activity increased after hypotonic stress. This increase depended on the extracellular Ca²⁺ activity. A possible physiological function of the large-conductance K⁺ channel in rat CCD cells may be the reduction of the intracellular K⁺ concentration after cell swelling. Once this channel is activated by increases in the cytosolic Ca²⁺ activity it can be regulated by changes in cellular pH and ATP.Supported by DFG Schl 277/2-3     

Properties of voltage-gated currents of microglia developed using macrophage colony-stimulating factor

Microglia were isolated from a murine neonatal brain cell culture in which their development had been stimulated by supplementation with the macrophage/microglial growth factor macrophage colony-stimulating factor (M-CSF). Using the whole-cell configuration of the patch-clamp technique, voltage-gated membrane currents were recorded from these microglial cells. Hyperpolarization induced inward rectifying K⁺ currents, as described for microglia from untreated cultures. These currents activated negative to the K⁺ equilibrium potential and, with a strong hyperpolarization, displayed time-dependent inactivation. The inactivation was abolished when extracellular NaCl was replaced by N-methyl-d-glucamine (NMG), thereby indicating a partial block of this K⁺ conductance by Na⁺. Inward rectifying currents were also blocked by extracellularly applied Cs⁺ or Ba²⁺. They were slightly diminished following treatment with extracellular tetraethylammonium chloride (TEA) but were not affected by 4-aminopyridine (4-AP). Upon long lasting depolarizing voltage pulses to potentials positive to 0 mV, the cells exhibited a slowly activating H⁺ current which could be reduced by application of inorganic polyvalent cations (Ba²⁺, Cd²⁺, Co²⁺, La³⁺, Ni²⁺, Zn²⁺) as well as by 4-AP or TEA. Based on their kinetics and pharmacological characteristics, both currents detected on M-CSF-grown microglia are suggested to correspond to the inward rectifier and the H⁺ current of macrophages.     

Development and testing of a simple algorithm for a glucose clamp

The glucose clamp technique is widely used in clinical research studies to maintain a constant blood glucose (BG) level during metabolic perturbation. An algorithm is used to set the rate of an intravenous glucose infusion according to measured BG concentrations. Currently used clamp algorithms are unnecessarily complex. This paper describes the development and use of a new algorithm which is simpler to implement. The algorithm employs proportional and differential feedback control. Discrete BG sampling with a sampling period of 5 min is used. Computer simulation with a two-compartment model of glucose dynamics was used to refine the algorithm. A Monte Carlo approach was adopted to examine the effects of random variations in measured BG concentrations and the elapsed time between blood sampling and adjustment of the glucose infusion rate. A coefficient of variation in BG concentration of less than 4 per cent was predicted for a euglycemic clamp. This was confirmed when the algorithm was applied in clinical research studies. This degree of BG control compares well with other published algorithms.     

Effect of C-peptide administration on whole body glucose utilization in STZ-induced diabetic rats

Recent studies suggest that C-peptide stimulates glucose transport in isolated skeletal muscle. In order to determine the effect of C-peptide on whole body glucose utilization, streptozotocin (60 mg kg^-1) (STZ)-induced diabetic and normal rats were studied using the euglycaemic clamp procedure and continuous infusion of somatostatin (1.0 μg kg^-1 min^-1) in pentobarbital-anaesthetized rats. Plasma insulin levels during the 6.0- and 30.0-mU kg^-1 min^-1 insulin infusions rose to 70–90 μU mL^-1 and 500–700 μU mL^-1, respectively. Blood glucose concentrations were clamped at 7.5–7.9 mmol L^-1 in the diabetic rats and at basal levels or 7.7 mmol L^-1 in the non-diabetic (normal) rats. Biosynthetic human C-peptide (0.5 nmol kg^-1 min^-1) was infused in 12 diabetic and 11 normal rats, resulting in concentrations of 26–41 nmol L^-1. The metabolic clearance rate of glucose (MCR) for the diabetic rats receiving C-peptide (12.0±1.0 mL kg^-1 min^-1) was significantly (P<0.01) higher than that in the diabetic rats given saline (6.3±0.7 mL kg^-1 min^-1) or a randomly scrambled C-peptide (7.8±1.3 mL kg^-1 min^-1) at low-dose insulin infusion but not at the high-dose insulin infusion. In normal rats C-peptide did not significantly increase the MCR for glucose. These results thus demonstrate that C-peptide has the capacity to increase glucose utilization in STZ-induced diabetic rats.     

Prediction models for insulin resistance in the polycystic ovary syndrome

Women with the polycystic ovary syndrome (PCOS) have a high prevalence of insulin resistance, with consequent increased risk of metabolic diseases later in life. An early metabolic screening would therefore be of clinical relevance. By using stepwise regression analysis on several variables obtained in 72 women with PCOS, we constructed simple and reliable mathematical models predicting insulin sensitivity, as measured by the euglycaemic hyperinsulinaemic clamp. The normal ranges of insulin sensitivity were calculated from 81 non-hirsute, normally menstruating women with normal ovaries, and similar body mass index (BMI) and age as the women with PCOS. Measured variables included BMI, waist and hip circumferences, truncal-abdominal skin folds, circulating concentrations of gonadotrophins, androgens, sex hormone-binding globulin (SHBG), triglycerides, total cholesterol and cholesterol subfractions, fasting insulin, C-peptide and free fatty acids. The three best prediction models included waist circumference, together with insulin (model I: R(2) = 0.77), serum triglycerides (model II: R(2) = 0.65), and the subscapularis skin fold (model III: R(2) = 0. 64). Using reference limits for insulin sensitivity obtained in the 81 normal pre-menopausal women, the models identify insulin resistant women with PCOS. These simple and inexpensive models are potentially useful in clinical practice as an early screening in women with PCOS.     

End-plate currents evoked by paired stimuli in frog muscle fibres

Using voltage-clamp techniques spontaneously occuring miniature end-plate currents (mepc) and nerve-evoked end-plate currents (epc) were recorded in frog glycerol-treated or cut muscle preparations. Epcs were induced by pairs of stimuli (the delay of the 2nd stimulus, t being 6 ms–30 s; one pair was delivered every 60–90 s). The decay time constant of the epc (_epc) was longer, the larger its quantal content despite the presence of active acetylcholinesterase (AChE). After treatment with anticholinesterases (prostigmine or armin, an irreversible inhibitor) this increase in _epc became more pronounced. When AChE was fully active the decay of the 1st epc ₁ was slightly faster than the decay of the 2nd epc ₂ only when the interstimulus interval was rather short (t<20 ms). Following treatment with anticholinesterases this difference between ₂ and ₁ could be determined even when t was as long as 30 s. In anticholinesterase-treated preparations was found to be inversely proportional to log t: a 50% increase in the decay time-constant of the 2nd epc occurred with t=120 ms. During continuous stimulation (10 impulses/s) _epc increased from the 1st to the 5–6th responses, but then decreased in parallel with the fall in the epc amplidude. The phenomenon of postsynaptic potentiation we observed could be readily abolished when quantal content was decreased by the presence of magnesium ions, but it was relatively unaffected when the receptor density was decreased by -bungarotoxin (-BuTX).The possible existence is discussed of two kinds of repetitive binding of ACh molecules, first, to free cholinoreceptors (a process which could be inhibited by -BuTX) and, second, to a complex of the cholinoreceptor plus one molecule of ACh (a process which is less sensitive to -BuTX blocking action).     

A reappraisal of frog muscle chloride conductance-voltage relations at pH 9

Voltage clamp experiments in muscle show that the steady state chloride conductance at pH 9 remains rather independent of [Cl^–]_o, for [Cl^–]_o in the range 165–265 mM. The steady state conductance-voltage relation has a maximum near V _rest — 20 mV. The initial-conductance — voltage relation obtained when the voltage is stepped away from a constant conditioning value (e.g. the resting potential) approaches an asymptotic maximum for hyperpolarizing steps and a minimum for depolarizing steps. The conductance declines with time if the test voltage is more negative than the resting potential, but remains constant if it is more positive. When the conditioning voltage is varied and the test kept constant the initial conductance at the step is also seen to be sigmoidal, if the test step is hyperpolarizing: for large negative conditioning steps the conductance at the test potential approaches the same asymptotic value as does the steady state relation, independent of the test voltage. At positive conditioning voltages it approaches a maximum asymptote which is dependent on the test voltage. When the test step is positive-going the initial conductance at the step is weakly dependent on the conditioning voltage and for large negative conditioning potentials is larger than predicted from the steady state relation. In summary, during hyperpolarizing voltage steps the chloride conductance seems to decline due to a gating phenomenon, but openstate conductance seems to be voltage-dependent, and at membrane potentials more positive than the resting it rapidly (within the settling time of the clamp) assumes a value almost independent of any preceding (conditioning) voltage.     

Kinetic mode switch of rat brain IIA Na channels in Xenopus oocytes excised macropatches

Na currents recorded from inside-out macropatches excised from Xenopus oocytes expressing the subunit of the rat brain Na channel IIA show at least two distinguishable components in their inactivation time course, with time constants differing about tenfold ( _h1 = approx. 150 s and _h2 = approx. 2 ms). In excised patches, the inactivation properties of Na currents changed with time, favoring the faster inactivation kinetics. Analysis of the fast and slow current kinetics shows that only the relative magnitudes of _h1 and _h2 components are altered without significant changes in the time constants of activation or inactivation. In addition, voltage dependence of both activation and steady-state inactivation of Na currents are shifted to more negative potentials in patches with predominantly fast inactivation, although reversal potentials and valences remained unaltered. We conclude that the two inactivation modes discerned in this study are conferred by two states of Na channel the interconversion of which are regulated by an as yet unknown mechanism that seems to involve cytosolic factors.