A series "RLC" circuit with R=6 ohm, C=0.02 Farad and L=0.1 has no applied voltage. Find the subsequent current in the circuit if the initial charge, on the capacitor is "q_0" and the initial current is zero.
Kirchhoff's voltage law:
"u_R+u_L+u_C=0"
where "u_R,u_L,u_C" are the voltages across R,L and C respectively.
Substituting in the constitutive equations:
"Ri(t)+L\\frac{di(t)}{dt}+\\frac{1}{C}\\int \\limits_{-\\infty}^{t}i(\\tau)d\\tau=0"
Differentiating and dividing by L :
"\\frac{d^2i(t)}{dt^2}+\\frac{R}{L}\\frac{di(t)}{dt}+\\frac{1}{LC}i(t)=0"
This can usefully be expressed in a more generally applicable form:
"\\frac{d^2i(t)}{dt^2}+2\\alpha\\frac{di(t)}{dt}+\\omega_0^2i(t)=0\\\\\n\\alpha=\\frac{R}{2L}, \\omega_0=\\frac{1}{\\sqrt{LC}}"
The differential equation has the characteristic equation:
"s^2+2\\alpha s+\\omega_0^2=0"
The roots of the equation in s are:
"i(t)=A(e^{s_1t}-e^{s_2t})=\\\\\n=Ae^{-\\alpha t}(e^{\\sqrt{\\alpha^2-\\omega_0^2}t}-e^{-\\sqrt{\\alpha^2-\\omega_0^2}t})\\\\\n\\alpha=\\frac{6}{0.2}=30, \\omega_0=\\frac{1}{\\sqrt{0.002}}\\\\\n\\sqrt{\\alpha^2-\\omega_0^2}=\\sqrt{900-\\frac{1}{0.002}}=\\sqrt{400}=20"
therefore
"i(t)=Ae^{-30 t}(e^{20t}-e^{-20t})=A(e^{-10t}-e^{-50t})"
The initial charge on the capacitor is "q_0" and initial current is zero:
"L\\frac{di(t)}{dt}|_{t=0}+\\frac{q_0}{C}=0\\\\\n\\frac{di(t)}{dt}|_{t=0}=A(-10e^{-10t}+50e^{-50t})\\\\\n\\frac{di(t)}{dt}|_{t=0}=40A\\\\\n\\frac{q_0}{LC}=-40A\\\\\nA=-\\frac{q_0}{40LC}=-12.5q_0"
Therefore:
"i(t)=-12.5q_0(e^{-10t}-e^{-50t})"
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