CURRENT DECREASING TO ZERO: Previously we found the current immediately after a circuit is changed and the current a long time after. Now we want to know how the current I(t) depends on time, not just at t = 0 and at t=0, 1. Assume the switch is in position (b). Applying the loop rule around the right loop counterclockwise gives dl (t) EAVAV₁-1(t)R= -L- -1(t) R = 0 dt where I (t) is the current at time t. We can rewrite the differential equation as: dl R == I dt L 1 t R t (bet) = - = - 10 e ½ + = - = - 100 71 E d dt 00000 www The only function whose derivative is proportional to the function itself is the exponential. Substitute /(t) = A e-t/t into both the left and right hand side of the differential equation above and take the derivative (remember the chain rule). Solve for the time constant T₁. R The constant A is just the initial current at t = 0. Therefore the current as a function of time is I (t) = 1, e-t/¹¹ for the case of the current decaying from I, at t = 0 to zero at t = co.
CURRENT DECREASING TO ZERO: Previously we found the current immediately after a circuit is changed and the current a long time after. Now we want to know how the current I(t) depends on time, not just at t = 0 and at t=0, 1. Assume the switch is in position (b). Applying the loop rule around the right loop counterclockwise gives dl (t) EAVAV₁-1(t)R= -L- -1(t) R = 0 dt where I (t) is the current at time t. We can rewrite the differential equation as: dl R == I dt L 1 t R t (bet) = - = - 10 e ½ + = - = - 100 71 E d dt 00000 www The only function whose derivative is proportional to the function itself is the exponential. Substitute /(t) = A e-t/t into both the left and right hand side of the differential equation above and take the derivative (remember the chain rule). Solve for the time constant T₁. R The constant A is just the initial current at t = 0. Therefore the current as a function of time is I (t) = 1, e-t/¹¹ for the case of the current decaying from I, at t = 0 to zero at t = co.
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