Book contents
- Frontmatter
- Contents
- Preface
- Acknowledgments
- Introduction: new perspectives on the causes and management of systems crisis
- Part 1 Dynamics of state power and role: systems structure
- Part 2 Dynamics of major war and systems transformation
- Part 3 Dynamics of general equilibrium and world order
- Part 4 Systems transformation and world order at century's end
- Appendix: Mathematical relations in the power cycle
- References
- Index
Appendix: Mathematical relations in the power cycle
Published online by Cambridge University Press: 08 September 2009
- Frontmatter
- Contents
- Preface
- Acknowledgments
- Introduction: new perspectives on the causes and management of systems crisis
- Part 1 Dynamics of state power and role: systems structure
- Part 2 Dynamics of major war and systems transformation
- Part 3 Dynamics of general equilibrium and world order
- Part 4 Systems transformation and world order at century's end
- Appendix: Mathematical relations in the power cycle
- References
- Index
Summary
For a function of one variable, a critical point is a point at which the derivative is zero (at which the tangent is horizontal).
The concept of critical points in the dynamic, as used in power cycle theory, refers to (1) critical points on the relative power curve itself, and (2) critical points on the curve of the dynamic of change in relative power, that is, on the curve of the rate of change in relative power. Hence, the critical points in the dynamic are (1) the maximum and minimum of the relative power curve itself, and (2) the points of inflection on the relative power curve, since these are the maximum and minimum of the curve of the first derivative.
Likewise, inflection point is as defined in both calculus and differential geometry. The calculus definition stems from calculus of variations and differential manifolds theory: the second derivative is zero (note that the first derivative is not required to be zero, which is a special case of inflection point of importance in catastrophe theory) (Bronshtein and Semendyayev 1985, pp. 242–8). The differential geometry definition (pp. 554–55) is based on curvature conditions, namely, that the curvature changes sign at the point of inflection. A few algebraic steps show that the curvature condition required at the inflection point occurs for the general asymmetric logistic precisely when the second derivative is zero.
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- Systems in CrisisNew Imperatives of High Politics at Century's End, pp. 260 - 267Publisher: Cambridge University PressPrint publication year: 1991