 | 1857 - 1142 pages
...imparted by them will be (2) 17. In order to determine the intensity of a shock, the whole velocity must be resolved into two components, one parallel and the other perpendicular to the side. Of these components, the first will not be affected by the shock, and will not enter into consideration... | |
 | Julius Ludwig Weisbach - 1883 - 622 pages
...Let P be the oblique force exerted by FIG. 340. FIG. 341. the connecting rod on the pin A ; let it be resolved into two components, one parallel and the other perpendicular to the direction of the piston rod, and represented by K and N respectively. The component TV will exert a... | |
 | George Minchin Minchin - 1886 - 560 pages
...axis exists for all displacements round which the equilibrium is astatic, prove that if each force is resolved into two components, one parallel and the other perpendicular to the axis, each of these component sets is astatic for displacements round the axis. 13. In a non-equilibrating... | |
 | George Minchin Minchin - 1889 - 556 pages
...axis exists for all displacements round which the equilibrium is astatic, prove that if each force is resolved into two components, one parallel and the other perpendicular to the axis, each of these component sets is astatic for displacements round the axis. 13. In a non-equilibrating... | |
 | Joseph Frederic Klein - 1892 - 240 pages
...L of the known accelerations BCand AL. If the total accelerations of each of the points of the rod be resolved into two components, one parallel and the other perpendicular to the rod, and these components be laid off as ordinates, (taking the rod as an axis of abscissas), one set... | |
 | 1896 - 458 pages
...instrument. If the displacement of the point D is not perpendicular to the plane of the paper, it may be resolved into two components, one parallel and the other perpendicular to that plane. The former component merely alters very slightly the horizontal distance between the points... | |
 | 1905 - 546 pages
...force E which produces a harmonic alternating current I in a circuit. This electromotive force may be resolved into two components, one parallel and the other perpendicular to I, as shown, for example, in Fig. 41. The component of E parallel to I is equal to El. The resistance... | |
 | Louis Adolphe Martin - 1907 - 260 pages
...rigidly connected so that the line PiP2 cannot change its length. The velocities vi and v2 can each be resolved into two components, one parallel and the other perpendicular to the line PiP2, as shown. As, by hypothesis, the distance PiP2 cannot change, the components of the velocities... | |
 | 1908 - 512 pages
...force E which produces a harmonic alternating current I in a circuit. This electromotive force may be resolved into two components, one parallel and the other perpendicular to I, as shown, for example, in Fig. 41. The component of E parallel to I is equal to RI. The resistance... | |
 | American School (Lansing, Ill.), William Esty - 1912 - 504 pages
...force E which produces a harmonic alternating current 7 in a circuit. This electromotive force may be resolved into two components, one parallel and the other perpendicular to 7, as shown, for example, in Fig. 43. The component of E parallel to 7 is equal to RI. The resistance... | |
| |
This electromotive force may be resolved into two components, one parallel and the other perpendicular to I, as shown, for example, in Fig. 
