Le Jeu de l'amour et du hasard by Marivaux

By Marivaux

Pour sonder l. a. sincérité de Dorante, qu’on lui destine sans qu’elle l’ait jamais rencontré, Silvia échange son behavior avec sa servante Lisette. Mais los angeles belle forget about que son prétendant a recours au même stratagème avec son valet. Ainsi travestis, les deux commencent à se parler d’amour… Et l. a. parole fait tomber les masques.

Les personnages parviendront-ils à mettre un terme au jeu de dupes dans lequel ils se sont enferrés ? Le spectateur trouvera-t-il une réponse aux interrogations que soulève l. a. pièce – puis-je être aimé pour moi-même ? L’amour peut-il triompher des préjugés sociaux ? Intemporels, ces questionnements expliquent sans doute le succès jamais démenti de l’oeuvre depuis sa création en 1730.

À travers son cahier photographs et les nombreux témoignages réunis dans son file, l’édition permet de confronter le texte de l. a. pièce à ses mises en scène. Elle suggest en outre trois groupements de textes et des sujets pour s’entraîner à l’épreuve de français au baccalauréat.

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Extra resources for Le Jeu de l'amour et du hasard

Example text

When t2 − 4d > 0, the matrix A has two real eigenvalues with the same sign, λ1 > λ2 . Therefore if t < 0, then E s = R2 and E u = E c = {0}; and if t > 0, then E u = R2 and E s = E c = {0}. 7, depending on t. The corresponding phase portrait of the system x˙ = Ax is obtained by a linear transformation. The origin is called an asymptotically stable node if t < 0, and an asymptotically unstable node if t > 0. When t2 − 4d = 0, there exists a unique eigenvalue λ, which is real, and the real Jordan normal form of A is λ 0 λ 1 J= or J = .

Therefore, Φ(s, x) = P −1 Ψ(s, P x). 8) From this we obtain the expressions of the flow of any planar linear system. 6. Consider the flow Φ(t, x) of the linear system x˙ = Ax, with A ∈ L(R2 ), d = det(A) and t = trace(A). Let J be the real Jordan normal form of A and P be the matrix such that J = P AP −1 . (a) If t2 − 4d > 0, then esλ1 0 Φ (s, x) = P −1 0 esλ2 P x. (b) If t2 − 4d = 0, then either Φ (s, x) = esλ x or Φ (s, x) = P −1 esλ 0 s esλ P x, depending on whether J is diagonal or not. (c) If t2 − 4d < 0, then Φ (s, x) = esα P −1 cos (βs) − sin (βs) sin (βs) cos (βs) P x.

We see that the origin, which is a focus type singular point, is a global attractor. Also, two separatrices born at the two saddles at infinity are observed. The remaining singular points at infinity are two nodes. 326 KΩ one has T = 0. 6(h). Now the global attractor, namely, the singular point at the origin, is replaced by a central region foliated by periodic orbits (bounded period annulus). The remainder of the phase portrait persists without changes. 326 KΩ we have that T > 0. 9(g). As it can be observed, the period annulus disappears and only one periodic solution persists.

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