Ibrahim Karim's Back to a Future for Mankind - BioGeometry PDF

By Ibrahim Karim

ISBN-10: 1449963951

ISBN-13: 9781449963958

This first-ever released selection of writings via Dr. Ibrahim Karim displays the holistic essence of his worldview. Dr Karim is the founding father of the technological know-how of BioGeometry within the early Seventies. BioGeometry is the technological know-how that makes use of shapes, colours, movement and sound to urge concord into the sophisticated strength traits of our environment. on the center of this concord is a sophisticated strength caliber present in the transcendental facilities of the forming technique of nature and is the most caliber in sacred energy spots of humanity that supply a non secular measurement to the undying monuments erected because the sunrise of humanity. together with his event as an architect and a scientist Dr. Karim has synergized points of Pythagorean Harmonics, refined strength sciences, Radiesthesia, Geobiology, construction Biology, Sacred structure & glossy wave theories to supply a brand new Physics of caliber from which the technology of BioGeometry emerged. *BioGeometry bridges technology and spirituality to supply a ordinary concord into the surroundings. *BioGeometry offers a practicable resolution in reworking the standard of the influence that electromagnetic radiation has on residing platforms. profitable initiatives in Switzerland in collaboration & acknowledgment of Swiss experts turn out its potency to take our glossy technological know-how into the longer term. *BioGeometry offers new options to Earth Radiation, that is a major wellbeing and fitness probability if no longer stated within the position and layout of our structures. * a brand new energy-quality-based research of the good Pyramid in Giza, finds new wisdom at the finest of the wonders of the realm and at the essence of the nice old Egyptian civilization.

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38), respectively. All these tensors, like the deformation gradient, do not depend at any fixed time on a material point’s location; they too are homogeneous. The velocity and acceleration of a material point A in O were computed in Sect. 4. 48b) + Ï, the above formulae may be expanded as vA = ( + Ï) · xA ˙ + Ï2 ) · xA . 49b) 30 2 Continuum Mechanics We may identify w(t) as Ï’s axial vector, and w(t) then is the angular velocity of any material line of the body. Because w(t) is homogeneous, every material line rotates at the same rate.

61), the stress tensor on the left side had six, while each “load” moment tensor on the right side had nine independent elements. The “left-over” three equations yielded global angular momentum balance. For higher moments, the number of stress moments exceeds the number of load moments, so that all stress moments of that order cannot be determined. In fact, from moments of order n 3, not all components of the (n − 1)th-stress moment may be found. As Truesdell and Toupin (1960, p. 58) yields non-unique stresses.

173, Eq. 19) show that unloading takes place only when the three conditions f = 0, δf < 0 and c˙ = 0 are together satisfied. The first of these conditions is necessary for the material to be in a plastic state before transition. 73) without equality. The final stipulation is equivalent to demanding that at transition the strain rate be zero. 78) that during plastic flow = 0, so that c˙ > 0. Thus, for unloading from a plastic state to possibly initiate, the strain rate | | must first fall to zero.

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Back to a Future for Mankind - BioGeometry by Ibrahim Karim


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