Math Problem Statement

I'm solving problems dealing with bifurcations in 1D systems. The initial function given is x_dot = r + (1/2)x - (x/(1+x)). In detailed steps: determine the bifurcation point(s), sketch the bifurcation diagram of the fixed point(s) versus parameter r, and sketch all the qualitatively different phase portraits as r is varied. Double check the math before answering.

Solution

Let's carefully solve the problem step by step. The given 1D dynamical system is:

x˙=r+12xx1+x\dot{x} = r + \frac{1}{2}x - \frac{x}{1+x}

We are tasked with finding the bifurcation points, sketching the bifurcation diagram, and drawing the phase portraits as the parameter rr is varied.

Step 1: Find the fixed points

Fixed points occur when x˙=0\dot{x} = 0. Therefore, set the right-hand side equal to zero and solve for xx:

r+12xx1+x=0r + \frac{1}{2}x - \frac{x}{1+x} = 0

To make this easier to solve, first find a common denominator for the x1+x\frac{x}{1+x} term. Multiply both sides of the equation by 1+x1 + x to eliminate the denominator:

(1+x)(r+12xx1+x)=0(1 + x)\left( r + \frac{1}{2}x - \frac{x}{1 + x} \right) = 0

r(1+x)+12x(1+x)x=0r(1 + x) + \frac{1}{2}x(1 + x) - x = 0

Now expand each term:

r+rx+12x+12x2x=0r + rx + \frac{1}{2}x + \frac{1}{2}x^2 - x = 0

Simplify the terms involving xx:

r+rx+(121)x+12x2=0r + rx + \left( \frac{1}{2} - 1 \right)x + \frac{1}{2}x^2 = 0

This simplifies further to:

r+rx12x+12x2=0r + rx - \frac{1}{2}x + \frac{1}{2}x^2 = 0

Rearranging:

r+x(r12)+12x2=0r + x\left( r - \frac{1}{2} \right) + \frac{1}{2}x^2 = 0

Step 2: Analyze the nature of fixed points and bifurcations

This is a quadratic equation in xx. We can solve for xx using the quadratic formula:

x=(r12)±(r12)22r1x = \frac{-\left( r - \frac{1}{2} \right) \pm \sqrt{\left( r - \frac{1}{2} \right)^2 - 2r}}{1}

Simplifying the discriminant:

x=(r12)±(r12)22rx = -\left( r - \frac{1}{2} \right) \pm \sqrt{\left( r - \frac{1}{2} \right)^2 - 2r}

We now analyze the discriminant Δ=(r12)22r\Delta = \left( r - \frac{1}{2} \right)^2 - 2r.

Step 3: Determine bifurcation points

A bifurcation occurs when the discriminant Δ\Delta changes sign, i.e., when it becomes zero. Let's solve for when Δ=0\Delta = 0:

(r12)22r=0\left( r - \frac{1}{2} \right)^2 - 2r = 0

Expanding the first term:

r2r+142r=0r^2 - r + \frac{1}{4} - 2r = 0

Simplifying:

r23r+14=0r^2 - 3r + \frac{1}{4} = 0

Now apply the quadratic formula to solve for rr:

r=(3)±(3)24(1)(14)2(1)r = \frac{-(-3) \pm \sqrt{(-3)^2 - 4(1)(\frac{1}{4})}}{2(1)}

r=3±912=3±82=3±222r = \frac{3 \pm \sqrt{9 - 1}}{2} = \frac{3 \pm \sqrt{8}}{2} = \frac{3 \pm 2\sqrt{2}}{2}

Thus, the bifurcation points occur at:

r=3+222,r=3222r = \frac{3 + 2\sqrt{2}}{2}, \quad r = \frac{3 - 2\sqrt{2}}{2}

Step 4: Sketch the bifurcation diagram

The bifurcation diagram will plot the fixed points xx^* versus the parameter rr. At the bifurcation points, we expect changes in the number or stability of fixed points.

Since the discriminant goes from positive to negative, a saddle-node bifurcation is expected at the critical values of rr, where two fixed points merge and annihilate.

Step 5: Sketch the phase portraits

For different values of rr:

  • For rr less than the first bifurcation point: Two fixed points exist, one stable and one unstable.
  • At the bifurcation points: The two fixed points merge (saddle-node bifurcation).
  • For rr greater than the second bifurcation point: No fixed points exist, leading to divergent behavior of the system.

Final Steps

Now that we have the bifurcation points and the general structure of the bifurcation diagram, the next step is to sketch the phase portraits and bifurcation diagram based on this information.

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Math Problem Analysis

Mathematical Concepts

Bifurcation Theory
Dynamical Systems
Fixed Points
Saddle-Node Bifurcation

Formulas

ẋ = r + (1/2)x - (x / (1 + x))
Quadratic formula: x = [-b ± √(b² - 4ac)] / 2a
Discriminant Δ = (r - 1/2)² - 2r

Theorems

Saddle-Node Bifurcation

Suitable Grade Level

Undergraduate (Math, Physics, or Engineering)