Chapter 8: Problem 8
Solve the \(L-R-C\) equation for \(I(t)\) if \(L=\) \(1 \mathrm{H}, R=6 \Omega, C=1 / 9 \mathrm{~F}, E(t)=100 \sin t \mathrm{~V}\), and \(I(0)=0\).
Short Answer
Expert verified
\[ I(t) = \left( \frac{200}{63} + Bt \right) e^{-3t} + \frac{500}{63} \sin t - \frac{200}{63} \cos t \]
Step by step solution
01
Identify the given values
Given: Inductance (L) = 1 H Resistance (R) = 6 Ω Capacitance (C) = 1/9 F Voltage (E(t)) = 100 sin(t) V Initial current (I(0)) = 0 A
02
Write the differential equation
The general form of the L-R-C equation for a series circuit is \[ L \frac{d^2I}{dt^2} + R \frac{dI}{dt} + \frac{1}{C} I = E(t) \] Substituting the given values: \[ 1 \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 100 \, \sin t \]
03
Simplify the differential equation
The simplified differential equation is: \[ \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 100 \, \sin t \]
04
Find the homogeneous solution
Solve the homogeneous equation: \[ \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 0 \] Assume a solution of the form \( I_h = e^{rt} \). Substituting in gives: \[ r^2 + 6r + 9 = 0 \] Factoring, we get: \[ (r+3)^2 = 0 \] So, \( r = -3 \). The homogeneous solution is then: \[ I_h = (A + Bt)e^{-3t} \]
05
Find the particular solution
Guess a particular solution of the form \( I_p = A \sin t + B \cos t \). Substitute into the non-homogeneous equation: \[ ( - A \sin t - B \cos t ) + 6 ( A \cos t - B \sin t ) + 9( A \sin t + B \cos t ) = 100 \sin t \] Group the \( \sin t \) and \( \cos t \) terms: \[ (-A + 6B + 9A) \sin t + (-B + 6A + 9B) \cos t = 100 \sin t \] Simplify: \[ 8A + 6B \sin t + 6A + 8B \cos t = 100 \sin t \] Equate coefficients: \[ 15A + 6B = 100 \] \[ 6A + 15B = 0 \]
06
Solve for coefficients A and B
From \[ 6A + 15B = 0 \] we get \( A = -\frac{5B}{2} \). Substitute into \[ 15A + 6B = 100 \]: \[ 15(-\frac{5B}{2}) + 6B = 100 \] \[ -\frac{75B}{2} + 6B = 100 \] \[ -75B + 12B = 200 \] \[ -63B = 200 \] \[ B = -\frac{200}{63} \] \[ A = \frac{500}{63} \]
07
Write the particular solution
The particular solution is: \[ I_p = \frac{500}{63} \sin t - \frac{200}{63} \cos t \]
08
Write the general solution
The general solution is: \[ I(t) = I_h + I_p = (A + Bt)e^{-3t} + \frac{500}{63} \sin t - \frac{200}{63} \cos t \]
09
Apply initial condition
Apply \( I(0) = 0 \): \[ 0 = (A + B \cdot 0)e^{-3 \cdot 0} + \frac{500}{63} \sin 0 - \frac{200}{63} \cos 0 \] \[ 0 = A - \frac{200}{63} \] \[ A = \frac{200}{63} \]
10
Write the specific solution
Therefore, the complete solution is: \[ I(t) = \left( \frac{200}{63} + Bt \right) e^{-3t} + \frac{500}{63} \sin t - \frac{200}{63} \cos t \]
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Homogeneous Solution
In mathematics, solving a differential equation often starts with finding the homogeneous solution. This involves setting the right-hand side of the differential equation to zero, which simplifies our task. Here, we deal with the equation:
\[ L \frac{d^2I}{dt^2} + R \frac{dI}{dt} + \frac{1}{C} I = 0 \]
For our specific problem, after substituting the values for L, R, and C, we get:
\[ \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 0 \]
The homogeneous solution is found by solving this simplified equation. Assume the solution of the form \[ I_h = e^{rt} \] and substitute into the equation to find the characteristic equation
\[ r^2 + 6r + 9 = 0 \].
Factoring gives \[ (r+3)^2 = 0 \], so the roots are \[ r = -3 \]. Hence, the homogeneous solution becomes:
\[ I(h) = (A + Bt)e^{-3t} \].
\[ L \frac{d^2I}{dt^2} + R \frac{dI}{dt} + \frac{1}{C} I = 0 \]
For our specific problem, after substituting the values for L, R, and C, we get:
\[ \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 0 \]
The homogeneous solution is found by solving this simplified equation. Assume the solution of the form \[ I_h = e^{rt} \] and substitute into the equation to find the characteristic equation
\[ r^2 + 6r + 9 = 0 \].
Factoring gives \[ (r+3)^2 = 0 \], so the roots are \[ r = -3 \]. Hence, the homogeneous solution becomes:
\[ I(h) = (A + Bt)e^{-3t} \].
Particular Solution
To solve the differential equation completely, we need the particular solution, which addresses the non-zero right-hand side of our equation:
\[ \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 100 \sin t \].
We guess a solution of the form:
\[ I_p = A \sin t + B \cos t \].
Substituting this guess into the differential equation and comparing coefficients helps us find the values of A and B. After working through the algebra:
\[ (-A \sin t - B \cos t) + 6 (A \cos t - B \sin t) + 9(A \sin t + B \cos t) = 100 \sin t \],
we simplify and solve the system of equations to get:
\[ 15A + 6B = 100 \]
\[ 6A + 15B = 0 \].
Solving these gives:
\[ A = \frac{500} {63}, \ B = -\frac{200}{63} \].
The particular solution then is:
\[ I_p = \frac{500}{63} \sin t - \frac{200}{63} \cos t \].
\[ \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 100 \sin t \].
We guess a solution of the form:
\[ I_p = A \sin t + B \cos t \].
Substituting this guess into the differential equation and comparing coefficients helps us find the values of A and B. After working through the algebra:
\[ (-A \sin t - B \cos t) + 6 (A \cos t - B \sin t) + 9(A \sin t + B \cos t) = 100 \sin t \],
we simplify and solve the system of equations to get:
\[ 15A + 6B = 100 \]
\[ 6A + 15B = 0 \].
Solving these gives:
\[ A = \frac{500} {63}, \ B = -\frac{200}{63} \].
The particular solution then is:
\[ I_p = \frac{500}{63} \sin t - \frac{200}{63} \cos t \].
Initial Conditions
Initial conditions are vital to determine the constants in our general solution. Here, it is specified that \[ I(0) = 0 \].
Applying this condition to our general solution which combines both the homogeneous and particular solutions:
\[ I(t) = (A + Bt)e^{-3t} + \frac{500}{63} \sin t - \frac{200}{63} \cos t \],
we substitute t = 0:
\[ 0 = (A + B \cdot 0)e^{-3 \cdot 0} + \frac{500}{63} \sin 0 - \frac{200}{63} \cos 0 \],
which simplifies to:
\[ 0 = A - \frac{200}{63} \],
therefore, \[ A = \frac{200}{63} \].
This final value of A is used to write our specific solution.
Applying this condition to our general solution which combines both the homogeneous and particular solutions:
\[ I(t) = (A + Bt)e^{-3t} + \frac{500}{63} \sin t - \frac{200}{63} \cos t \],
we substitute t = 0:
\[ 0 = (A + B \cdot 0)e^{-3 \cdot 0} + \frac{500}{63} \sin 0 - \frac{200}{63} \cos 0 \],
which simplifies to:
\[ 0 = A - \frac{200}{63} \],
therefore, \[ A = \frac{200}{63} \].
This final value of A is used to write our specific solution.
Non-Homogeneous Differential Equation
A non-homogeneous differential equation is one that includes a term independent of the function we aim to solve. Here our equation is:
\[ \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 100 \sin t \],
where the term \[ 100 \sin t \] makes it non-homogeneous.
Solving such equations typically involves two steps:
Combining these two solutions gives us the general solution. For our equation, this results in:
\[ I(t) = (\frac{200}{63} + Bt)e^{-3t} + \frac{500}{63} \sin t - \frac{200}{63} \cos t \].
\[ \frac{d^2I}{dt^2} + 6 \frac{dI}{dt} + 9 I = 100 \sin t \],
where the term \[ 100 \sin t \] makes it non-homogeneous.
Solving such equations typically involves two steps:
- Finding the homogeneous solution, \[ I_h \], by solving the equation where this independent term is set to zero.
- Finding the particular solution, \[ I_p \], that directly responds to the non-homogeneous part.
Combining these two solutions gives us the general solution. For our equation, this results in:
\[ I(t) = (\frac{200}{63} + Bt)e^{-3t} + \frac{500}{63} \sin t - \frac{200}{63} \cos t \].