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به نام خدا
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Patch Clamp
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Opposing views on the time course of the single-channel current
1. A microscopic version of the end-plate current recorded with voltage clamp 2. All-or-none manner
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Problem in the measurement of single-channel currents
ik=Υk ( Vm – Ek ) Vm – Ek=50 mV ,Υk =20 pS → ik=1 pA Johnson noise current σn=√(4kTΔf/R) Δf=1 kHz , R=1/20 pS , T=293 K k= Boltzmann’s constant → σn=0.018 pA → S/N=56
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R1= 10 MΩ Rchannel= 5*10^10 Ω RT= 10 MΩ → σn=1.3 pA
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The micropipette tip is around 1 µm diameter so measurement is unaffected by spatial variations and is hence “space clamped”, the “clamp” in the name “patch clamp” arises from this feature.
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Considerations to ensure adequate signal to noise ratio
A high resistance seal The pipette should be carefully fire-polished and clean Cells should be clean and free of connective tissue Application of gentle suction
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Configurations of patch clamp
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Single channel conductance
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The choice of tip diameter of around 1 µm is about ten times larger than available intracellular micropipettes. This results in a lower tip resistance, a desirable factor to achieve a lower noise, as noted above. On the other hand, it may mean that more than one channel may find itself under the patch electrode; an examination of the recorded signal will reveal whether, in fact, only a single channel is accessed.
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