• The Journal of Korean Physical Therapy
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• v.14 no.2
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• pp.1-15
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• 2002

Excitation-contraction coupling in skeletal muscle is process by which depolarization of the muscle fiber membrane, elicited by a nerve action potential, triggers the release of $Ca^{2+}$ from the sarcoplasmic reticulum(SR). The resulting rise in intracellular $Ca^{2+}$ concentration$([Ca^{2+}]_i)$ activates the troponin complex, thereby initiating the contraction of the muscle. The question remains as to what factors are involved in the inhibition of SR $Ca^{2+}$ release in fatigued muscle. The purpose of this study was determine whether ATP-sensitive $K^+(K_{ATP})$ channels are activated and contribute to decrease in $[Ca^{2+}]_i$ during fatigue development in the mouse skeletal muscle. To elucidate a role of $K_{ATP})$ in relation to ECC, I measured the modulation effects of $K_{ATP})$ channel blocker(glibenclamide) and opener(pinacidil) on $[Ca^{2+}]_i$ after fatiguing electrical field stimulation(FEFS). Intracellular $Ca^{2+}$ signals were recorded by conforcal laser microscopy(LSM 410) and monitored using the fluorescent $Ca^{2+}$-Sensitive indicator Fluo-3 AM. The results of this study were as followed: 1. The relative [Ca2'li after FEFS in the pre-glibenclamide-treated group was higher than the control. And relative $[Ca^{2+}]_i$ after FEFS in the pre-glibenclamide-treated group was lower than the control. 2. The relative $[Ca^{2+}]_i$ after FEFS for 3 min in the control, pre-glibenclamide-treated group and pre-pinacidil-treated group showed a similar pattern; the gradually significant decrease in $[Ca^{2+}]_i$. But, these decreasing pattern was most significant in the control. These findings suggest a tight relationship between $K_{ATP})$ and $Ca^{2+}$ in ECC during fatigue. Therefore, 1 thought that activation of $K_{ATP})$ channels may be one of mechanisms of the fatigue in skeletal muscle.

• Bulletin of the Korean Chemical Society
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• v.10 no.6
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• pp.504-509
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• 1989

The effect of oxygen-deficiency on the charge distributions and orbital energies for small copper oxide clusters representing the superconducting materials $YBa_2Cu_3O_x (6{\leq}x{\leq}7)$ were investigated by the extended Huckel molecular orbital (EHMO) method with the tight-binding model. Our calculations show +3 oxidation state of Cu(1) in the $CuO_3$ chain and +2 or +1 of Cu(2) in the $CuO_2$ layers for $YBa_2Cu_3O_7$ with the nominal charge of $Cu_3$ = +7 (or +5), while for $YBa_2Cu_3O_6$ +1 oxidation state of Cu(1) and +3 (or +2) of Cu(2) in the $CuO_2$ layers with the nominal charge of $Cu_3$ = +7 (or +5). For $Cu_3O_{12}$ cluster representing $YBa_2Cu_3O_7$ with the nominal charge of $Cu_3$ = +7 the Cu(2) $d_{{x^2}-{y^2}}$ orbitals in the $CuO_2$ layers is a typical Jahn-Teller $d^9$ system with the partial hole and the Cu(1) $d_{{_z2}-{_y2}}$ orbital in the $CuO_3$ chain contains hole occupancy. For $Cu_3O_{10}$ cluster representing $YBa_2Cu_3O_6$ with the nominal charge of Cu = +5 the orbital character of the highest partially occupied MO (HPOMO) and the lowest completely unoccupied MO (LCUMO) of $Cu_3O_{12}$ representing $YBa_2Cu_3O_7$ with the nominal charge of $Cu_3$ = +7 is reversed, and the character of Cu(1) $d{{x^2}-{y^2}}$ orbital of LCUMO of the $Cu_3O_{12} $cluster is vanished. It is suggested that the local crystal field environment of Cu(1) by the oxygens in the Cu(1) chain may play a vital role in conductivity and superconductivity, either alone or through cooperative electronic coupling with the Cu(2) layers in $YBa_2Cu_3O_7.$.