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on_electronics_._note [2016/07/23 14:29]
nikolaj
on_electronics_._note [2016/07/23 14:29]
nikolaj
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 == Models for devices == == Models for devices ==
->$G=c_R+a_C\dfrac{\partial}{\partial t}+c_L\int{\mathrm d}t$+>$G = a_R + a_C \dfrac{\partial}{\partial t} + a_L \int{\mathrm d}t$
  
 An capacitor are two ends of a conducting line that hold charges with a some voltage between them. Ideally, i.e. in the simplest case, we double the voltage if we double the charges - thus the number $C:​=\frac{q_x}{U}$ is a constant. The factor $\frac{1}{C}$ says how strongly $U$ rises in reaction to a rise of $q_x$. Expressing that rise in terms of the time dependent incoming charge current, $q_x\propto \int^t I(t)$, we find $G{\sim}C\dfrac{\partial}{\partial t}$. An capacitor are two ends of a conducting line that hold charges with a some voltage between them. Ideally, i.e. in the simplest case, we double the voltage if we double the charges - thus the number $C:​=\frac{q_x}{U}$ is a constant. The factor $\frac{1}{C}$ says how strongly $U$ rises in reaction to a rise of $q_x$. Expressing that rise in terms of the time dependent incoming charge current, $q_x\propto \int^t I(t)$, we find $G{\sim}C\dfrac{\partial}{\partial t}$.
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