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Deleuze, citing film writer Jean Mitry, sees Chaplin as giving "mime a new model, a function of space and time, a continuity constructed at each instant […] instead of being related to prior forms which it was to embody" as well as happening "in the street, surrounded by cars, along a pavement".
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.
An ant starts to crawl along a taut rubber rope 1 km long at a speed of 1 cm per second (relative to the rubber it is crawling on). At the same time, the rope starts to stretch uniformly at a constant rate of 1 km per second, so that after 1 second it is 2 km long, after 2 seconds it is 3 km long, etc.
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.
Deleuze's concept of art goes beyond the representation of an image. According to Ronald Bogue in "Gilles Deleuze: The Aesthetics of Force", Deleuze emphasizes a common problem across various art forms. He focuses not on reproducing or inventing different forms of representation in art, but on "harnessing forces." [5]
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 ...
Because speed is constant, the velocity vectors on the right sweep out a circle as time advances. For a swept angle dθ = ω dt the change in v is a vector at right angles to v and of magnitude v dθ , which in turn means that the magnitude of the acceleration is given by a c = v d θ d t = v ω = v 2 r {\displaystyle a_{c}=v{\frac {d\theta ...