Vectors and Rotors: With ApplicationsE. Arnold, 1903 - 204 sider |
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Resultat 1-5 av 28
Side xiv
... Bodies 155 • 187. Elastic Limit . 155 188. Strain 155 189 . Stress 156 190 . Measurement of Stress and Strain in rod under tension or compression 156 191. Hooke's Law 157 192. Bodies supposed rigid 157 193. Weight of bars and friction ...
... Bodies 155 • 187. Elastic Limit . 155 188. Strain 155 189 . Stress 156 190 . Measurement of Stress and Strain in rod under tension or compression 156 191. Hooke's Law 157 192. Bodies supposed rigid 157 193. Weight of bars and friction ...
Side 3
... body are good examples of this . In the case of the wind , we cannot say that it has any particular position ; it ... body . To describe the motion of such a body we must state about what axis of the body it is spinning ; it is not suffi ...
... body are good examples of this . In the case of the wind , we cannot say that it has any particular position ; it ... body . To describe the motion of such a body we must state about what axis of the body it is spinning ; it is not suffi ...
Side 4
... body in a given position is a localized scalar , a force acting on a body at a definite point is a localized vector . 8 . Definition . A localized vector is called a Rotor ( Clifford ) . 9. All quantities used by Euclid and those used ...
... body in a given position is a localized scalar , a force acting on a body at a definite point is a localized vector . 8 . Definition . A localized vector is called a Rotor ( Clifford ) . 9. All quantities used by Euclid and those used ...
Side 41
... bodies must therefore be at right angles to the common surface . The action between the body and the plane must be a compressive strain , the plane pushes against the body with a force R , say , and the body presses on the plane with a ...
... bodies must therefore be at right angles to the common surface . The action between the body and the plane must be a compressive strain , the plane pushes against the body with a force R , say , and the body presses on the plane with a ...
Side 42
... body horizontally , find the tension in the string and the position of equilibrium . In this case two forces are known completely , the third is unknown in magnitude and in direction . The process is as before ; take say 1 cm . to ...
... body horizontally , find the tension in the string and the position of equilibrium . In this case two forces are known completely , the third is unknown in magnitude and in direction . The process is as before ; take say 1 cm . to ...
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Vectors and Rotors: With Applications Olaus Henrici,George Charles Turner Uten tilgangsbegrensning - 1903 |
Vanlige uttrykk og setninger
a₁ Algebra angle applied axis B₁ B₂ bars base beam bending bending moment bisect C₁ called centre collinear Commutative Law components compression coordinates coplanar corresponding definite denote determined diagonals direction and sense distance divide draw drawn equal equation equilibrium figure find the mass-centre forces acting frame friction geometrical girder give given points given rotors Hence the mass-centre horizontal length line joining line parallel link-polygon load m₁ magnitude mass mass-points mid-point momental area move negative number of vectors orts parallel rotors parallelogram parallelopiped perpendicular plane pole polygon position vector projection quantity reaction rectangle represent rigid body scalar product shearing force shew shewn sides straight line stress diagram string Suppose system of rotors tension tetrahedron theorem tons triangle vanishes vector product vector-polygon vertex vertices weight
Populære avsnitt
Side 21 - If two triangles have one angle of the one equal to one angle of the other and the sides about these equal angles proportional, the triangles are similar.
Side 29 - ... line and the extremities of the base have the same ratio which the other sides of the triangle have to one...
Side 8 - If a straight line be divided into any two parts, the square on the whole line is equal to the squares on the two parts, together with twice the rectangle contained by the two parts.
Side 112 - ... is equal to the rectangle contained by the segments of the other.
Side 17 - ... from the beginning of the first to the end of the last...