Give step-by-step solution with explanation and final answer:Exercise 1.6.3: Consider x" = x2. a) Draw the phase diagram, find the critical points, and mark them stable or unstable. b) Sketch typical solutions of the equation. ¢) Find Jim x(t) for the solution with the initial condition x(0) = —1.
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Give step-by-step solution with explanation and final answer:
Exercise 1.6.3: Consider x" = x2.
a) Draw the phase diagram, find the critical points, and mark them stable or unstable.
b) Sketch typical solutions of the equation.
¢) Find Jim x(t) for the solution with the initial condition x(0) = —1.
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Asked by: gvr
Created at: 2025-06-18 10:47:22
Asked by: gvr
Created at: 2025-06-18 10:47:22
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Let's solve each part step by step.
---
### **Given:**
\[
x' = x^2
\]
---
## **a) Phase diagram, critical points, stability**
### **Step 1: Find the critical points**
Critical points occur where \( x' = 0 \):
\[
x^2 = 0 \implies x = 0
\]
So, the only critical point is at \( x = 0 \).
---
### **Step 2: Analyze stability**
- For \( x > 0 \): \( x^2 > 0 \implies x' > 0 \), so \( x \) increases.
- For \( x < 0 \): \( x^2 > 0 \implies x' > 0 \), so \( x \) increases (toward 0).
#### **Phase Line:**
- Draw a line with \( x \) values.
- At \( x = 0 \), mark a point (critical point).
- For \( x > 0 \), draw arrows pointing **away from 0** (to the right).
- For \( x < 0 \), draw arrows pointing **toward 0** (to the right).
#### **Stability:**
- At \( x = 0 \), both sides point **away from 0** (for \( x>0 \)) and **toward 0** (for \( x<0 \)), but notice for negative values, \( x \) increases toward 0, but as soon as it crosses to positive, it moves away rapidly (since \( x^2 \) grows fast).
- **\( x = 0 \) is an unstable critical point** (since any positive perturbation causes \( x \) to blow up).
---
## **b) Sketch typical solutions**
### **Step 1: Solve the equation analytically**
\[
\frac{dx}{dt} = x^2
\]
Separate variables:
\[
\frac{dx}{x^2} = dt
\]
Integrate both sides:
\[
\int x^{-2} dx = \int dt
\]
\[
- x^{-1} = t + C
\]
\[
\frac{1}{x} = - (t + C)
\]
\[
x(t) = \frac{1}{- (t + C)}
\]
### **Step 2: Typical solutions**
- For \( x(0) = x_0 \):
\[
x(0) = \frac{1}{-C} \implies C = -\frac{1}{x_0}
\]
\[
x(t) = \frac{1}{- (t - \frac{1}{x_0})} = \frac{x_0}{1 - x_0 t}
\]
- **If \( x_0 > 0 \):** denominator hits zero at \( t = \frac{1}{x_0} \) (blows up in finite time).
- **If \( x_0 < 0 \):** denominator never hits zero for positive \( t \), approaches zero from below as \( t \to \infty \).
**Sketch:**
- All solutions with \( x_0 > 0 \): blow up in finite time.
- Solutions with \( x_0 < 0 \): approach 0 from below as \( t \to \infty \).
- \( x_0 = 0 \): stays at 0 (critical point).
---
## **c) Limit for \( x(0) = -1 \) as \( t \to \infty \)**
From above:
\[
x(t) = \frac{-1}{1 + t}
\]
As \( t \to \infty \), \( x(t) \to 0^- \).
### **Final Answer:**
\[
\boxed{0}
\]
---
### **Summary Table**
| Part | Result |
|------|--------|
| (a) | Critical point at \( x=0 \), unstable. |
| (b) | Solutions: \( x(t) = \frac{x_0}{1 - x_0 t} \). Positive initial values blow up; negative initial values approach 0 from below. |
| (c) | \( \lim_{t\to\infty} x(t) = 0 \) for \( x(0) = -1 \). |
If you need the phase diagram or a sketch, let me know!
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