Nonlinear Dynamics and Chaos2nd EditionSteven H. Strogatz Publisher: PERSEUS DISBN: 9780813349107
Nonlinear Dynamics and Chaos
Solutions for Nonlinear Dynamics and Chaos
Browse All Chapters of This Textbook
Chapter 2.1 - A Geometric Way Of ThinkingChapter 2.2 - Fixed Points And StabilityChapter 2.3 - Population GrowthChapter 2.4 - Linear Stability AnalysisChapter 2.5 - Existence And UniquenessChapter 2.6 - Impossibility Of OscillationsChapter 2.7 - PotentialsChapter 2.8 - Solving Equations On The ComputerChapter 3.1 - Saddle-node BifurcationChapter 3.2 - Transcritical Bifurcation
Chapter 3.3 - Laser ThresholdChapter 3.4 - Pitchfork BifurcationChapter 3.5 - Overdamped Bead On A Rotating HoopChapter 3.6 - Imperfect Bifurcations And CatastrophesChapter 3.7 - Insect OutbreakChapter 4.1 - Examples And DefinitionsChapter 4.2 - Uniform OscillatorChapter 4.3 - Nonuniform OscillatorChapter 4.4 - Overdamped PendulumChapter 4.5 - FirefliesChapter 4.6 - Superconducting Josephson JunctionsChapter 5.1 - Definitions And ExamplesChapter 5.2 - Classification Of Linear SystemsChapter 5.3 - Love AffairsChapter 6.1 - Phase PortraitsChapter 6.2 - Existence, Uniqueness, And Topological ConsequencesChapter 6.3 - Fixed Points And LinearizationChapter 6.4 - Rabbits Versus SheepChapter 6.5 - Conservative SystemsChapter 6.6 - Reversible SystemsChapter 6.7 - PendulumChapter 6.8 - Index TheoryChapter 7.1 - ExamplesChapter 7.2 - Ruling Out Closed OrbitsChapter 7.3 - Poincaré−bendixson TheoremChapter 7.4 - Liénard SystemsChapter 7.5 - Relaxation OscillationsChapter 7.6 - Weakly Nonlinear OscillatorsChapter 8.1 - Saddle-node, Transcritical, And Pitchfork BifurcationsChapter 8.2 - Hopf BifurcationsChapter 8.3 - Oscillating Chemical ReactionsChapter 8.4 - Global Bifurcations Of CyclesChapter 8.5 - Hysteresis In The Driven Pendulum And Josephson JunctionChapter 8.6 - Coupled Oscillators And QuasiperiodicityChapter 8.7 - Poincaré MapsChapter 9.1 - A Chaotic WaterwheelChapter 9.2 - Simple Properties Of The Lorenz EquationsChapter 9.3 - Chaos On A Strange AttractorChapter 9.4 - Lorenz MapChapter 9.5 - Exploring Parameter SpaceChapter 9.6 - Using Chaos To Send Secret MessagesChapter 10.1 - Fixed Points And CobwebsChapter 10.2 - Logistic Map: NumericsChapter 10.3 - Logistic Map: AnalysisChapter 10.4 - Periodic WindowsChapter 10.5 - Liapunov ExponentChapter 10.6 - Universality And ExperimentsChapter 10.7 - RenormalizationChapter 11.1 - Countable And Uncountable SetsChapter 11.2 - Cantor SetChapter 11.3 - Dimension Of Self-similar FractalsChapter 11.4 - Box DimensionChapter 11.5 - Pointwise And Correlation DimensionsChapter 12.1 - The Simplest ExamplesChapter 12.2 - Hénon MapChapter 12.3 - Rössler SystemChapter 12.4 - Chemical Chaos And Attractor ReconstructionChapter 12.5 - Forced Double-well Oscillator
Book Details
This textbook is aimed at newcomers to nonlinear dynamics and chaos, especially students taking a first course in the subject. The presentation stresses analytical methods, concrete examples, and geometric intuition.
Sample Solutions for this Textbook
We offer sample solutions for Nonlinear Dynamics and Chaos homework problems. See examples below:
a) The differential equation which shows the velocity v(t) of a skydiver falling to the ground is...From the given differential equation x˙=x(1-x), the variable x˙ explicitly depends on x and...(a) We have, x˙ = r - x2 To find the potential V(x) -dVdx= r - x2 dV= (- r + x2)dx By integrating...Given information: dxdτ = rx (1- xk) - x21 + x2 The given expression is dimensionless for budworm...The period of oscillation for the non-uniform oscillator is T = ∫-ππdθω-asinθ Here, ω is the angular...Josephson junctions are superconducting devices that are capable of generating voltage oscillations...a) The vector field of the given system x˙ = -y, y˙ = -x is shown below b) Consider the given...The linear system equations are x˙ = 4x - y And, y˙ = 2x + y. The above linear equations can be...The forecast for lovers is governed by the general linear system R˙= aR+bJ And J˙= cR+dJ Here, R˙ is...
a) The system is given as: x˙ = x + e- y, y˙ = -y The given equations can be rewritten as: dxdt = x...Using the first equation r˙ = - rdrdt = -rdrr = -dt∫r0rdrr= - ∫0tdtlnr - lnr0= -tlnrr0=-tr(t) =...a) The given system equations are n˙1= G1(N0- α1n1- α2n2)n1-K1n1 n˙2= G2(N0- α1n1- α2n2)n2-K2n2...For a given solution x (t), the total energy E can be expressed as, E = 12mx˙2 + V(x) Here, V(x) is...Given information: The system is with bead and hoop in motion. The total energy is expressed as E =...a) The system is given as x˙ = y - y3, y˙ = - x - y2 Nullclines are the curves in the phase portrait...Following fixed points have an index equal to +1. Sketch for the stable spiral, The above sketch...Index theory provides global information about the phase portrait. The index of the closed curve C...In the linear system the determination of the matrix A is defined by Δ. If det (A) is positive so...(a) System is given as, P˙ = P[(aR−S)−(a−1)(PR+RS+PS)]……………………………………… (1) R˙ =...The power series expansion of the function f(x)= an(x- c)n is given as, ∑0∞an(x - c)n=a0+ a1(x- c)+...Conservation of energy: This theorem states that the energy of an isolated system is constant over...The expression for the averaging equation for magnitude is: x(t,ε) = x0+O(ε) Here, x is the position...Consider the Interacting bar magnets system with system equation θ˙1 = K sin (θ1 - θ2) - sin θ1 and...a) The system equations are: x˙1 = - x1 + F(I - bx2 - gy1)y˙1 = (- y1 + x1) / Tx˙2 = - x2 + F(I -...The general equation of the weekly nonlinear oscillator is x¨ + x + εh(x, x˙) = 0 The average or...Let r0 be an initial condition on the surface curve S. Since θ˙ = 1 the first return to S occurs...a) The given system equations are x˙ + x = F(t) Multiply the complete equation by et. etx˙ + etx =...a) The quasi periodic system is given as θ˙1 = ω1, θ˙2 = ω2 This system is periodic, but it is not...a) V˙=−e22−4be32 e2 and e3 are error dynamic terms. The given condition is V˙≤−kV Putting...In the given Newton’s method, consider the map xn+1 = f(xn), where f(xn) = xn- g(xn)g'(xn) Here xn+1...a) The cubic map equation is xn+1 = rxn - xn3, The difference equation xn+1 = f (xn). Let xn = x*...Consider the logistic map xn+1 = f(x) and function f(x) = rxn(1- xn) for the period cycle 3 that...The function equation arose in renormalization equation is, g(x) = αg2(xa) The power series...First we introduce some notation. Let f(x, r) denote a unimodal map that undergoes a period-doubling...The von Koch snowflake curve can be constructed by the computer: The arc length of S0= 3; each...Consider a fractal that divides the closed unit interval [0,1] into four quarters. Consider the set...Using Matlab, we can write a program to compute the correlation dimension of the Lorenz attractor....From the Henon map equations, xn+2= bxn+1−a(yn+1−axn2)2 yn+2=b(yn+1−axn2)x = bx+1−a(y+1−ax2)2 y =...
More Editions of This Book
Corresponding editions of this textbook are also available below:
Nonlinear Dynamics And Chaos: With Applications To Physics, Biology, Chemistry, And Engineering (studies In Nonlinearity)
1st Edition
ISBN: 9780738204536
EBK NONLINEAR DYNAMICS AND CHAOS WITH S
2nd Edition
ISBN: 9780429680151
Nonlinear Dynamics and Chaos
2nd Edition
ISBN: 9780429972195
NONLINEAR DYNAMICS & CHAOS
2nd Edition
ISBN: 9780813350844
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