How can Kirchoff's first law be applied to electrical circuits?

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SUMMARY

The discussion focuses on applying Kirchoff's first law for electrical circuits, represented by the equation V=RI+L(dI/dt), where V is the electromotive force, R is resistance, L is inductance, and I is current. The participants derive the expression I=I(0)e^(-Rt/L) under the condition that the electromotive force is terminated at time t=0. Key points include the importance of variable consistency and the necessity of checking solutions by substituting back into the original differential equation.

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  • Understanding of Kirchoff's laws in electrical circuits
  • Familiarity with differential equations
  • Knowledge of electromotive force, resistance, and inductance
  • Basic calculus for solving equations involving derivatives
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nameVoid
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According to Kirchoff's first law for electrical circuits V=RI+L(dI/dt) where constants V, R and L denote the electromotive force, the resistance, and the inductance, respectively, and I denotes the current at time t. If the electromotive force is terminated at time t=0 and if the current is I(0) at the instant of removal, prove that I=I(0)e^(-Rt/L)

Homework Equations





The Attempt at a Solution


<br /> v=RI+L(\frac{dI}{dT})<br />
<br /> dt=\frac{LdI}{v-RI}<br />
<br /> t+b=Lln|v-RI|(-R) <br />
<br /> e^{\frac{t+b}{-LR}}=v-RI<br />
<br /> t-&gt; v-&gt; 0 , I=I(0)<br />
<br /> e^{\frac{b}{-LR}}=-RI(0)<br />
<br /> -e^{\frac{t}{-LR}}(RI(0))=v-RI<br />
<br /> I=\frac{e^{\frac{t}{-LR}}RI(0)+v}{R}<br />
im afraid to do anymore work on this but looks good to me so far
 
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nameVoid said:
According to Kirchoff's first law for electrical circuits V=RI+L(dI/dt) where constants V, R and L denote the electromotive force, the resistance, and the inductance, respectively, and I denotes the current at time t. If the electromotive force is terminated at time t=0 and if the current is I(0) at the instant of removal, prove that I=I(0)e^(-Rt/L)

Homework Equations





The Attempt at a Solution


<br /> v=RI+L(\frac{dI}{dT})<br />
<br /> dt=\frac{LdI}{v-RI}<br />
OK up to here, but I think instead of (-R) you want (-1/R) in the next line. This comes from the substitution you did but don't show. In any case, you can check your answer by differentiating it and substituting back into the original differential equation.

Also, pay closer attention to your variables. You started with T and changed to t. Since this is time, t is a better choice. If you run into differential equations that involve time and temperature (usually represented by t and T, respectively), you'll run into trouble.
nameVoid said:
<br /> t+b=Lln|v-RI|(-R) <br />
<br /> e^{\frac{t+b}{-LR}}=v-RI<br />
<br /> t-&gt; v-&gt; 0 , I=I(0)<br />
<br /> e^{\frac{b}{-LR}}=-RI(0)<br />
<br /> -e^{\frac{t}{-LR}}(RI(0))=v-RI<br />
<br /> I=\frac{e^{\frac{t}{-LR}}RI(0)+v}{R}<br />
im afraid to do anymore work on this but looks good to me so far
 

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