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Gilles Louis René Deleuze (/ d ə ˈ l uː z / də-LOOZ; French: [ʒil dəløz]; 18 January 1925 – 4 November 1995) was a French philosopher who, from the early 1950s until his death in 1995, wrote on philosophy, literature, film, and fine art.
Deleuze proposes (citing Leibniz) that difference is better understood through the use of dx, the differential. A derivative, dy/dx, determines the structure of a curve while nonetheless existing just outside the curve itself; that is, by describing a virtual tangent (46). Deleuze argues that difference should fundamentally be the object of ...
Deleuze attempts to understand the wider literary and semiotic context of Bacon's art through employing the rhizomatic, or nonlinear mode of analysis, which he and psychoanalyst Félix Guattari had popularized in their work A Thousand Plateaus published one year before. This form of analysis seeks to disentangle the socio-cultural roots of a ...
Cinema 1: The Movement Image (French: Cinéma 1. L'image-mouvement) (1983) is the first of two books on cinema by the philosopher Gilles Deleuze, the second being Cinema 2: The Time Image (French: Cinéma 2. L'image-temps) (1985). Together Cinema 1 and Cinema 2 have become known as the Cinema books, the two volumes both complementary and ...
Martin Heidegger (/ ˈ h aɪ d ɛ ɡ ər, ˈ h aɪ d ɪ ɡ ər /; [3] German: [ˈmaʁtiːn ˈhaɪdɛɡɐ]; [3] 26 September 1889 – 26 May 1976) was a German philosopher best known for contributions to phenomenology, hermeneutics, and existentialism.
Trajectory of a particle with initial position vector r 0 and velocity v 0, subject to constant acceleration a, all three quantities in any direction, and the position r(t) and velocity v(t) after time t. The initial position, initial velocity, and acceleration vectors need not be collinear, and the equations of motion take an almost identical ...
All frames of reference with zero acceleration are in a state of constant rectilinear motion (straight-line motion) with respect to one another. In such a frame, an object with zero net force acting on it, is perceived to move with a constant velocity, or, equivalently, Newton's first law of motion holds. Such frames are known as inertial.
Mathematically, if the velocity of the first object in the previous discussion is denoted by the vector u = ud and the velocity of the second object by the vector v = ve, where u is the speed of the first object, v is the speed of the second object, and d and e are unit vectors in the directions of motion of each object respectively, then the ...