Degree | Type | Year |
---|---|---|
Mathematics | OT | 4 |
You can view this information at the end of this document.
Ordinary differential equations: existence and uniqueness of solutions of the Cauchy problem.
Linear differential systems with constant coefficients.
Linear algebra: spaces and vector subspecies, diagonalization.
This course is an introduction to the modern theory of dynamical systems. The first objective is for students to become familiar with the abstract notion of a dynamical system and the basic concepts of this theory: stability, attractor, invariant sets, omega limits, etc. The second objective is to understand the local behavior of both discrete and continuous dynamical systems in the vicinity of an equilibrium point or a periodic orbit. This local behavior is based on the topological classification of linear systems in ℝⁿ, both those derived from the flow of ordinary differential equations (continuous dynamical systems) and those arising from function iteration (discrete dynamical systems). Linear systems are very important because, on the one hand, they appear in the study of many relevant physical phenomena, and on the other hand, they represent the first approximation to more complex systems.
The qualitative theory of differential equations began with the work of Poincaré around 1880, in the context of his studies in celestial mechanics. It aims to understand properties of solutions without the need to solve the equations, among other reasons because exact solutions are only possible in exceptional cases. This qualitative approach, when combined with appropriate numerical methods, can in some cases be equivalent to having the solutions of the equation. The course will deepen the knowledge and study—introduced in previous subjects—of the qualitative theory of differential equations in higher-dimensional spaces, with an emphasis on the local structure of equilibrium points (both degenerate and non-degenerate) and the stability of periodic orbits.
The final objective of the course is to introduce techniques for understanding global discrete dynamics. The guiding thread will be a parametric family of discrete dynamical systems: unimodal maps, which (for certain parameter values) exhibit dynamics that naturally lead to the notion of chaos. For these systems, numerical approximation is not feasible, and new tools are required to understand their dynamics. Chaotic systems often appear in applications (e.g., weather prediction problems, electrical circuits, etc.).
1. Dynamical systems on topological spaces.
2. Study of local dynamics, discrete and continuous in Rn.
3. Global dynamics in continuous systems.
4. Global dynamics in discrete systems.
Title | Hours | ECTS | Learning Outcomes |
---|---|---|---|
Type: Directed | |||
Problem solving classes | 14 | 0.56 | |
Seminars | 6 | 0.24 | |
Theoretical lessons | 29 | 1.16 | |
Type: Autonomous | |||
Exam Preparation | 15 | 0.6 | |
Problem solving | 42 | 1.68 | |
Study of the theoretical part | 32 | 1.28 |
The course includes two hours of theoretical classes and one hour of problem-solving classes per week. During the semester, there will also be three seminar sessions, each lasting two hours.
Schedules and classroom assignments must be consulted through the UAB's online platforms. A dedicated space for this course will be available on the Virtual Campus (VC) to provide materials and share information related to the classes.
Theoretical classes: The teaching staff will develop the topics of the syllabus in the indicated order. A bibliography and part of the supporting materials, if necessary, for both theory and problem-solving, will also be available to students on the VC.
Problem-solving classes: Problem sets will be available on the VC. Some of these problems will be worked on in class.
During the seminars, certain concepts will be explored in greater depth and developed by the students.
Annotation: Within the schedule set by the centre or degree programme, 15 minutes of one class will be reserved for students to evaluate their lecturers and their courses or modules through questionnaires.
Title | Weighting | Hours | ECTS | Learning Outcomes |
---|---|---|---|---|
First midterm | 40% | 3 | 0.12 | 2, 5, 1, 9, 8, 7, 6, 3, 4 |
Second midterm | 40% | 3 | 0.12 | 5, 9, 3, 4 |
Seminars (3 activities) | 20% | 6 | 0.24 | 2, 1, 9, 8, 7, 3 |
Continuous assessment
The course is organized into the following components, each of which carries a specific weight in the final grade:
Seminars (SEM): Reports and the work assigned during the three seminar sessions will be evaluated.
First midterm (P1): Written exam scheduled for the middle of the semester.
Second midterm (P2): Written exam at the end of the semester.
If N1 = 0.2SEM + 0.4*(P1 + P2) is greater than or equal to 5, then N1 will be the final grade for the course. If N1 is below 5, the student may take a resit exam (R), and the final grade will be N2 = 0.2*SEM + 0.8*R. To be eligible, the student must have participated in at least 66% of the assessed activities.
Single assessment
On the same day as the second midterm exam of the continuous assessment, students who have previously opted for the single assessment will submit the work assigned during the seminar sessions (SEM) and take a final exam (F) covering the entire syllabus. The final grade will be N3 = 0.2*SEM + 0.8*F. If N3 < 5, the same resit system as in the continuous assessment will apply.
L.H. ALVES, Sistemas Dinâmicos, Mack Pesquisa, 2006.
D.K. ARROWSMITH, C.M. PLACE, An Introduction to dynamical Systems, Cambridge University Press, 1990.
D.K. ARROWSMITH, C.M. PLACE, Dynamical Systems, differential equations, maps and chaotic behaviour, Chapman & Hall Mathematics, 1992.
R.L. DEVANEY, An introduction to chaotic dynamical systems, The Benjamin/Cummings Publishing Company, Inc., 1986.
R.L. DEVANEY, Chaos, fractals and Dynamics, Computer experiments in mathematics, Addison-Wesley, 1990.
R.L. DEVANEY, A first course in chaotic dynamical systems, Theory and Experiment, Studies in Nonlinearity, 1992.
F. DUMORTIER, J.LLIBRE and J.C. ARTES, Qualitative Theory of Planar Differential Systems, Universitext, Springer-Verlag Berlin, 2006.
C. FERNANDEZ, F. j. VAZQUEZ, J. M. VEGAS, Ecuaciones diferenciales y en diferencias. Sistemas Dinámicso, Thomson 2003.
J. GUCKENHEIMER, P. HOLMES, Nonlinear oscillations, Dynamical Systems and Bifurcations of Vector Fields, Springer-Verlag, 1993.
M. HIRSCH, S. SMALE and R. DEVANEY, Differential Equations, Dynamical Systems and an Introduction to Chaos, Elsevier Academic Press, 2004.
M.C. IRWIN, Smooth Dynamical Systems, Advanced series in Nonlinear Dynamics, vol.17, World Scientific, 2001.
S. LYNCH, Dynamical Systems with Applications using MAPLE, Birkhäuser, 2000.
L. PERKO, Differential Equations and Dynamical Systems, Springer-Verlag, 1996.
C. ROBINSON, Dynamical Systems: Stability, Symbolic Dynamics and Chaos CRC Press, 1999.
J. L. ROMERO, C. GARCIA, Modelos y Sistemas Dinámicos, Univesidad de Cádiz, 1998.
J. SOTOMAYOR, Liçoes de equacoes diferenciais ordinárias, Projecto Euclides, Gráfica Editora Hamburg Ltda., 1979.
Please note that this information is provisional until 30 November 2025. You can check it through this link. To consult the language you will need to enter the CODE of the subject.
Name | Group | Language | Semester | Turn |
---|---|---|---|---|
(PAUL) Classroom practices | 1 | Catalan | first semester | morning-mixed |
(SEM) Seminars | 1 | Catalan | first semester | afternoon |
(TE) Theory | 1 | Catalan | first semester | morning-mixed |