In the circuit (see attachment),steady-state conditions have been reched at t=0.At t=0 switch is thrown to position 2.Solve for V(t) for "t" larger than "0" ?
Don't forget within a branch with an inductance, there's a continuity of current. That why i(0⁺)=i(0⁻)=i(0) !
I do have possible answers (see attachment) but I don get any of this,comparing my work with the answers.
There is a problem in your solutions, first v(t) is not sinusoidal. Have you sure it's the correct exercise ?
It is correct exercise.I did eliminate the first one.What about another four possible answers.
I made a mistake the solutions aren't correct. And the exponential is not 2 but -2. I will remake my demonstration and I post it here. The answer is whether (2) or (5).
It's the (2).
Thank you !!!!!!
I just find too bad we can edit a message on OpenStudy. I will make the remark to developpers. To be not confused I've preferred to delete my previous messages, and I give you the right one (with demonstration) here : Before t=0 \[v(t)=E_{generator}-R_1.i(t)\] Steady-state supposes v(t)=0 so : \[I=E_{generator}/R_1=20/4=5=i(t=0^+)\] At t=0⁺ \[v(t)=40.e^{-2.t}-R_2.i(t)=L.di(t)/dt\] We have a linear differential equation : \[di(t)/dt +(R_2/L).i(t)=(40/L).e^{-2.t}=20.e^{-2.t}\] Solution = Homogeneous Solution + Particular Solution \[HomogenousSolution=i(t)=A.e^{-(R_2/L).t}=A.e^{-5.t}\] We need to find a particular solution which works : \[\lambda'(t).e^{-5.t}=20.e^{-2.t}\] \[\lambda'(t)=20.e^{3.t}\] so \[ParticularSolution=\lambda(t).e^{-5.t}=(20/3).e^{-2.t}\] Then A=? At t=0⁺ I=5 A \[i(t=0^+)=5=A.+ (20/3)\] \[A=-5/3\] \[i(t)=(-5/3).e^{-5.t}+(20/3).e^{-2.t}\] \[v(t)=L.di(t)/dt=2*di(t)/dt=2*[(25/3).e^{-5.t} - (40/3).e^{-2.t}]\] The result is (2) !!! I've tried to be clearest, like that you could understand.
Thank you so much,very profesional.
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