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Math 211 Math 211 Lecture #8 Qualtitative Analysis September 14, - PowerPoint PPT Presentation

1 Math 211 Math 211 Lecture #8 Qualtitative Analysis September 14, 2001 2 Qualitative Analysis Qualitative Analysis Ways to discover the properties of solutions without solving the equation. Works best with autonomous equations y


  1. 1 Math 211 Math 211 Lecture #8 Qualtitative Analysis September 14, 2001

  2. 2 Qualitative Analysis Qualitative Analysis • Ways to discover the properties of solutions without solving the equation. • Works best with autonomous equations y ′ = f ( y ) • Example: y ′ = sin y

  3. 3 Properties of Autonomous Equations Properties of Autonomous Equations • The direction field does not depend on t • Solution curves can be translated left and right to get other solution curves. � If y ( t ) is a solution, so is y 1 = y ( t + c ) for any constant c .

  4. 4 Equilibrium Points & Solutions Equilibrium Points & Solutions Autonomous equation: y ′ = f ( y ) . • Equilibrium point: f ( y 0 ) = 0 . • Equilibrium solution: y ( t ) = y 0 . • Example: y ′ = sin y � sin y = 0 ⇔ y = kπ, k = 0 , ± 1 , . . . � y ′ = sin y has infinitely many equilibrium solutions: ◮ y k ( t ) = kπ for k = 0 , ± 1 , ± 2 , . . . Return

  5. 5 Between the Equilibrium Points Between the Equilibrium Points 0 < y < π ⇒ sin y > 0 ⇒ y ′ ( t ) = sin y ( t ) > 0 ⇒ y ( t ) is increasing • By uniqueness, 0 < y ( t ) < π for all t . • Thus y ( t ) ր π as t → ∞ and y ( t ) ց 0 as t → −∞ Return Eq. Pt.

  6. 6 Between the Equilibrium Points Between the Equilibrium Points − π < y < 0 ⇒ sin y < 0 ⇒ y ′ ( t ) = sin y ( t ) < 0 ⇒ y ( t ) is decreasing • By uniqueness, 0 > y ( t ) > − π for all t . • Thus y ( t ) ց − π as t → ∞ and y ( t ) ր 0 as t → −∞ f ( y ) > 0 Return Eq. Pt.

  7. 7 Stable & Unstable EPs Stable & Unstable EPs An equilibrium point y 0 is • asymptotically stable if all solutions starting near y 0 converge to y 0 as t → ∞ . • unstable if there are solutions starting arbitrarily close to y 0 which move away from y 0 as t increases. • There are 4 possibilities: Return

  8. 8 The Phase Line for y ′ = f ( y ) The Phase Line for y ′ = f ( y ) • The phase line is a y -axis, showing � the equilibrium points and � the direction of the flow between the equilibrium points. • The y -axis in the plot of y → f ( y ) . • The y -axis in the ty -plane where solutions are plotted. Return

  9. 9 Terminal Velocity Terminal Velocity • Magnitude of the resistance proportional to the square of the velocity: v ′ = − g − k | v | v/m • One equilibrium point at � mg v term = − k . • v term is asymptotically stable. Type

  10. 10 Qualitative Analysis of y ′ = f ( y ) . Qualitative Analysis of y ′ = f ( y ) . 1. Graph y → f ( y ) . f(y) y Return 7 steps

  11. 11 Qualitative Analysis of y ′ = f ( y ) . Qualitative Analysis of y ′ = f ( y ) . 2. Find the equilibrium points where f ( y ) = 0 . f(y) f(y) y y y 1 y 2 y 3 y 4 y 5 Return Graph 7 steps

  12. 12 Qualitative Analysis of y ′ = f ( y ) . Qualitative Analysis of y ′ = f ( y ) . 3. Determine the behavior between eq. pts. f(y) f(y) y y y 1 y 1 y 2 y 2 y 3 y 3 y 4 y 4 y 5 y 5 Return Graph EPs 7 steps

  13. 13 Qualitative Analysis of y ′ = f ( y ) . Qualitative Analysis of y ′ = f ( y ) . 4. Analyze the equilibrium points. f(y) f(y) y y y 1 y 1 y 2 y 2 y 3 y 3 y 4 y 4 y 5 y 5 Return Graph EPs Between 7 steps

  14. 14 Qualitative Analysis of y ′ = f ( y ) . Qualitative Analysis of y ′ = f ( y ) . 5. Transfer the phase line to ty -space. y f(y) y 5 y 4 t y 3 y y 1 y 2 y 3 y 4 y 5 y 2 y 1 Return Graph EPs Between Anal 7 steps

  15. 15 Qualitative Analysis of y ′ = f ( y ) . Qualitative Analysis of y ′ = f ( y ) . 6. Plot the equilibrium solutions. y y y 5 y 5 y 4 y 4 t t y 3 y 3 y 2 y 2 y 1 y 1 Return Graph EPs Between Anal Transfer 7 steps

  16. 16 Qualitative Analysis of y ′ = f ( y ) . Qualitative Analysis of y ′ = f ( y ) . 7. Plot other solutions approximately. y y y 5 y 5 y 4 y 4 t t y 3 y 3 y 2 y 2 y 1 y 1 Return Graph EPs Between Anal Transfer ESols 7 steps

  17. 17 Seven Steps Seven Steps Graph y → f ( y ) . 1. 2. Find the equilibrium points where f ( y ) = 0 . 3. Determine the behavior between eq. pts. 4. Analyze the equilibrium points. Transfer the phase line to ty -space. 5. 6. Plot the equilibrium solutions. 7. Plot other solutions approximately.

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