2. Solve the initial value problem z""+x" - 4x' - 4x = 0, x(0) = 1, x'(0) = 0, x" (0) = -1. Hint: Guess one eigenvalue.

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
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Please do number 2
### Exercises

1. **Find the general solution of the following differential equations.**

   a) \( x''' + x' = 0. \)

   b) \( x''' + x' = 1. \)

   c) \( x'''' + x'' = 0. \)

   d) \( x''' - x' - 8x = 0. \)

   e) \( x''' + x'' = 2e^t + 3t^2. \)

   f) \( x''' - 8x = 0. \)

2. **Solve the initial value problem** \( x'' + 4x' - 4x = 0, x(0) = 1, x'(0) = 0, x''(0) = -1. \) *Hint: Guess one eigenvalue.*

3. **Write a linear, fourth-order differential equation whose general solution is:**

   \[
   x(t) = c_1 + c_2 t + e^{5t} (c_4 \cos 2t + c_5 \sin 5t).
   \]

4. **What is the general solution of a fourth-order differential equation if the four eigenvalues are \( \lambda = 3 \pm i, 3 \pm i \)? What is the differential equation?**

---

### 2.6 Steady-State Heat Conduction*

Let us consider the following problem in steady-state heat conduction. A cylindrical, uniform, metallic bar of length \( L \) and cross-sectional area \( A \) is insulated on its lateral side. We assume the left face at \( x = 0 \) is maintained at \( T_0 \) degrees and that the right face at \( x = L \) is held at \( T_L \) degrees. What is the temperature distribution \( u = u(x) \) in the bar after it comes to equilibrium? Here \( u(x) \) represents the temperature of the entire cross-section of the bar at position \( x \) along the bar.

We assume that: 
- The temperature of the entire cross-section at the left face is \( T_0 \).
- The temperature at the right face is \( T_L \).
- The system has reached equilibrium, meaning the heat flow and temperature distribution do not change over time.

This setup provides a classic example of a boundary
Transcribed Image Text:### Exercises 1. **Find the general solution of the following differential equations.** a) \( x''' + x' = 0. \) b) \( x''' + x' = 1. \) c) \( x'''' + x'' = 0. \) d) \( x''' - x' - 8x = 0. \) e) \( x''' + x'' = 2e^t + 3t^2. \) f) \( x''' - 8x = 0. \) 2. **Solve the initial value problem** \( x'' + 4x' - 4x = 0, x(0) = 1, x'(0) = 0, x''(0) = -1. \) *Hint: Guess one eigenvalue.* 3. **Write a linear, fourth-order differential equation whose general solution is:** \[ x(t) = c_1 + c_2 t + e^{5t} (c_4 \cos 2t + c_5 \sin 5t). \] 4. **What is the general solution of a fourth-order differential equation if the four eigenvalues are \( \lambda = 3 \pm i, 3 \pm i \)? What is the differential equation?** --- ### 2.6 Steady-State Heat Conduction* Let us consider the following problem in steady-state heat conduction. A cylindrical, uniform, metallic bar of length \( L \) and cross-sectional area \( A \) is insulated on its lateral side. We assume the left face at \( x = 0 \) is maintained at \( T_0 \) degrees and that the right face at \( x = L \) is held at \( T_L \) degrees. What is the temperature distribution \( u = u(x) \) in the bar after it comes to equilibrium? Here \( u(x) \) represents the temperature of the entire cross-section of the bar at position \( x \) along the bar. We assume that: - The temperature of the entire cross-section at the left face is \( T_0 \). - The temperature at the right face is \( T_L \). - The system has reached equilibrium, meaning the heat flow and temperature distribution do not change over time. This setup provides a classic example of a boundary
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