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PLoS One
2010 Oct 26;510:e13611. doi: 10.1371/journal.pone.0013611.
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Human α3β4 neuronal nicotinic receptors show different stoichiometry if they are expressed in Xenopus oocytes or mammalian HEK293 cells.
Krashia P
,
Moroni M
,
Broadbent S
,
Hofmann G
,
Kracun S
,
Beato M
,
Groot-Kormelink PJ
,
Sivilotti LG
.
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BACKGROUND: The neuronal nicotinic receptors that mediate excitatory transmission in autonomic ganglia are thought to be formed mainly by the α3 and β4 subunits. Expressing this composition in oocytes fails to reproduce the properties of ganglionic receptors, which may also incorporate the α5 and/or β2 subunits. We compared the properties of human α3β4 neuronal nicotinic receptors expressed in Human embryonic kidney cells (HEK293) and in Xenopus oocytes, to examine the effect of the expression system and α:β subunit ratio.
METHODOLOGY/PRINCIPAL FINDINGS: Two distinct channel forms were observed: these are likely to correspond to different stoichiometries of the receptor, with two or three copies of the α subunit, as reported for α4β2 channels. This interpretation is supported by the pattern of change in acetylcholine (ACh) sensitivity observed when a hydrophilic Leu to Thr mutation was inserted in position 9' of the second transmembrane domain, as the effect of mutating the more abundant subunit is greater. Unlike α4β2 channels, for α3β4 receptors the putative two-α form is the predominant one in oocytes (at 1:1 α:β cRNA ratio). This two-α form has a slightly higher ACh sensitivity (about 3-fold in oocytes), and displays potentiation by zinc. The putative three-α form is the predominant one in HEK cells transfected with a 1:1 α:β DNA ratio or in oocytes at 9:1 α:β RNA ratio, and is more sensitive to dimethylphenylpiperazinium (DMPP) than to ACh. In outside-out single-channel recordings, the putative two-α form opened to distinctive long bursts (100 ms or more) with low conductance (26 pS), whereas the three-α form gave rise to short bursts (14 ms) of high conductance (39 pS).
CONCLUSIONS/SIGNIFICANCE: Like other neuronal nicotinic receptors, the α3β4 receptor can exist in two different stoichiometries, depending on whether it is expressed in oocytes or in mammalian cell lines and on the ratio of subunits transfected.
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21049012
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Figure 1. In HEK-expressed α3β4 receptors, the 9â²LT mutation has a greater effect if inserted in α3.Traces in (A) are whole cell inward currents elicited by different ACh concentrations applied to cells expressing wild type (top), α3β4LT (middle) or α3LTβ4 (bottom) channels. The bars above the traces show the duration of the agonist applications and the agonist concentration (in µM). Cells were transfected with an α3 to β4 ratio of 1â¶1 and held at â30 mV. Dose-response curves are shown in (B) for each receptor combination. The data were averaged after normalisation to the fitted maximum for each experiment. The lines show Hill equation fits (see Methods) to the pooled normalised data (nâ=â6â8).
Figure 2. The effect of the 9â² LT mutation in oocytes depends on the α3â¶Î²4 subunit ratio.Traces in (A) represent inward currents elicited by different concentrations of ACh (in µM) bath applied (duration shown as a solid bar). Cells were held at â70 mV. Pooled normalised dose-response curves, fitted with the Hill equation with free parameters are shown in (B) for oocytes injected with 1â¶9 (left) or 9â¶1 (right) α3 to β4 cRNA ratio. The 1â¶9 subunit ratio produces wild-type receptors that are more sensitive to ACh. The effect of the mutation is greater when it is carried by the β4 subunit if β4 is overexpressed (1â¶9) and when the α3 subunit is mutated if the α3 subunit is overexpressed (9â¶1).
Figure 3. Relationship between the average EC50 values and the presumed number of 9â² LT mutations.Each point is plotted according to the stoichiometry we suggest for each cell type and subunit ratio. The assumed stoichiometry is stated on the plot. The linear relationship between the EC50 values and the number of mutated subunits confirms that the stoichiometry we assume is plausible.
Figure 4. The two different receptor stoichiometries expressed in oocytes differ in their DMPP sensitivity.The traces in (A) are examples of inward currents elicited by low agonist concentrations (in µM) and recorded from oocytes injected with a subunit ratio of 1â¶9 (top traces) and 9â¶1 (bottom). The duration of each agonist application is shown above each trace (solid bar). All agonists (CCh, carbachol; EPB epibatidine; Nic, nicotine; DMPP, dimethylphenylpiperazinium; Cyt, cytisine; LOB, lobeline) were tested on the same oocyte (held at â70 mV), with the exception of lobeline (shown on the right, recorded from a different cell but with similar initial ACh current as the cell on the left, for both subunit ratios). The log-log plots in (B) are partial dose-response curves for the experiments shown in A (left). Note the increase in the potency of DMPP (10-fold leftward shift of the dose-response curve) in the 9â¶1 ratio.
Figure 5. The two-α and three-α form of the α3β4 receptor differ in their response to Zn2+ modulation.Traces in (A) are typical currents activated by an EC20 concentration of ACh on the two-α receptor (left, 1â¶9 αâ¶Î² ratio) and the three-α receptor (right, 9â¶1 ratio) in the presence of increasing concentrations of Zn2+. Zn2+ was pre-applied to oocytes for 30 s before it was applied together with ACh. (B) Zn2+ concentration-response curves for the three-α receptor (filled squares) and the two-α receptor (filled circles). Curves from different cells were pooled and fitted to the Hill equation and to the sum of two Hill equations, respectively. Note that Zn2+ potentiated only the ACh responses of oocytes expressing the two-α stoichiometry.
Figure 6. Single-channel properties of α3β4 receptors expressed from extreme ratios in HEK293 cells.(A) Examples of outside-out currents elicited by 5 µM ACh, from cells transfected with an α3 to β4 cDNA ratio of 1â¶9 (left) and 9â¶1 (right). Patches were held at â100 mV. The histograms of fitted amplitudes corresponding to these recordings are shown in (B). These are fitted with Gaussian curves to give the peak current amplitudes and the areas under each curve (for these two patches the values are 2.7±0.3 pA, area 100% for 1â¶9; 2.6±0.5 pA, area 27% and 3.9±0.4 pA, area 73% for 9â¶1). The histogram on the left (C) shows the proportion of bursts (as % of the total number of bursts from all experiments, pooled) at each chord conductance for the two subunit ratios. The histogram on the right (D) shows the difference in the duration of the bursts to different conductances for the two ratios.
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