Consider an RLC circuit with resistance 2 ohms, inductance 0.05 henrys, capacitance 0.006 farads, and an impressed voltage, provided by an alternating current generator, of E(t) = 5 sin(25t). At t = 0 the charge is 1 coulomb and the current is 1 amps. a. Complete the ODE below in terms of the charge in the circuit Q(t) Q" ] Q² + [ Q' Q = b. Solve the ODE and complete the equation for the charge Q(t) =
Consider an RLC circuit with resistance 2 ohms, inductance 0.05 henrys, capacitance 0.006 farads, and an impressed voltage, provided by an alternating current generator, of E(t) = 5 sin(25t). At t = 0 the charge is 1 coulomb and the current is 1 amps. a. Complete the ODE below in terms of the charge in the circuit Q(t) Q" ] Q² + [ Q' Q = b. Solve the ODE and complete the equation for the charge Q(t) =
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![### Solving an RLC Circuit with Given Parameters
Consider an RLC circuit with:
- Resistance: \( 2 \) ohms
- Inductance: \( 0.05 \) henrys
- Capacitance: \( 0.006 \) farads
This circuit is driven by an alternating current generator with an impressed voltage defined by \( E(t) = 5 \sin(25t) \). At \( t = 0 \), the initial conditions are:
- Charge: \( 1 \) coulomb
- Current: \( 1 \) amp
#### a. Completing the ODE
Given the information:
\[ \boxed{0.05}Q'' + \boxed{2}Q' + \boxed{\frac{1}{0.006}}Q = 5 \sin(25t) \]
Substituting the provided values:
\[ 0.05Q'' + 2Q' + \frac{1}{0.006}Q = 5 \sin(25t) \]
Simplifying the coefficient for \(Q\):
\[ \frac{1}{0.006} = 166.\overline{6} \]
Thus, the completed ordinary differential equation (ODE) in terms of the charge \( Q(t) \) is:
\[ 0.05Q'' + 2Q' + 166.67Q = 5 \sin(25t) \]
#### b. Solving the ODE
To solve for the charge \( Q(t) \), one must follow the procedures for solving second-order linear differential equations, potentially involving methods such as undetermined coefficients or variation of parameters. You'd generally:
1. Solve the corresponding homogeneous equation:
\[ 0.05Q'' + 2Q' + 166.67Q = 0 \]
2. Find particular solutions to the non-homogeneous equation:
\[ 0.05Q'' + 2Q' + 166.67Q = 5 \sin(25t) \]
Combining the solutions will yield the general form of \( Q(t) \).
For detailed, step-by-step solutions, please refer to resources on solving second-order linear differential equations with non-homogeneous terms.
#### Solution:
Given \( Q(t) \):
\[ \boxed{Q(t) = \text{(The detailed solved equation in terms of } t)} \]](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F3d3733a5-5e9e-433b-b6d1-2cfec636672d%2F496fd2f3-226d-4150-ad50-3c6b25162ca2%2F7qjh0yc_processed.png&w=3840&q=75)
Transcribed Image Text:### Solving an RLC Circuit with Given Parameters
Consider an RLC circuit with:
- Resistance: \( 2 \) ohms
- Inductance: \( 0.05 \) henrys
- Capacitance: \( 0.006 \) farads
This circuit is driven by an alternating current generator with an impressed voltage defined by \( E(t) = 5 \sin(25t) \). At \( t = 0 \), the initial conditions are:
- Charge: \( 1 \) coulomb
- Current: \( 1 \) amp
#### a. Completing the ODE
Given the information:
\[ \boxed{0.05}Q'' + \boxed{2}Q' + \boxed{\frac{1}{0.006}}Q = 5 \sin(25t) \]
Substituting the provided values:
\[ 0.05Q'' + 2Q' + \frac{1}{0.006}Q = 5 \sin(25t) \]
Simplifying the coefficient for \(Q\):
\[ \frac{1}{0.006} = 166.\overline{6} \]
Thus, the completed ordinary differential equation (ODE) in terms of the charge \( Q(t) \) is:
\[ 0.05Q'' + 2Q' + 166.67Q = 5 \sin(25t) \]
#### b. Solving the ODE
To solve for the charge \( Q(t) \), one must follow the procedures for solving second-order linear differential equations, potentially involving methods such as undetermined coefficients or variation of parameters. You'd generally:
1. Solve the corresponding homogeneous equation:
\[ 0.05Q'' + 2Q' + 166.67Q = 0 \]
2. Find particular solutions to the non-homogeneous equation:
\[ 0.05Q'' + 2Q' + 166.67Q = 5 \sin(25t) \]
Combining the solutions will yield the general form of \( Q(t) \).
For detailed, step-by-step solutions, please refer to resources on solving second-order linear differential equations with non-homogeneous terms.
#### Solution:
Given \( Q(t) \):
\[ \boxed{Q(t) = \text{(The detailed solved equation in terms of } t)} \]
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