Elements of Dynamic: An Introduction to the Study of Motion and Rest in Solid and Fluid Bodies, Volumer 1-3MacMillan and Company, 1878 |
Inni boken
Resultat 1-5 av 27
Side vii
... Flux · Circulation . 191 194 Strain - Flux not Homogeneous 197 Lines of Flow and Vortex - Lines 199 Circulation in Non - Homogeneous Strain - Flux 200 PAGE Expansion Irrotational Motion Equipotential Surfaces Motion partly Irrotational ...
... Flux · Circulation . 191 194 Strain - Flux not Homogeneous 197 Lines of Flow and Vortex - Lines 199 Circulation in Non - Homogeneous Strain - Flux 200 PAGE Expansion Irrotational Motion Equipotential Surfaces Motion partly Irrotational ...
Side 63
... flux . It appears from the above considerations that a flux is always to be conceived as a velocity ; because a quantity must be continuous to be fluent , must therefore be specified either by a line or an angle ( which may be placed at ...
... flux . It appears from the above considerations that a flux is always to be conceived as a velocity ; because a quantity must be continuous to be fluent , must therefore be specified either by a line or an angle ( which may be placed at ...
Side 64
... flux of a sum or difference of two or more quanti- ties is the sum or difference of the fluxes of the quantities . This is merely the rule for composition of velocities . Flux of a product of two quantities . Let p , q be the quantities ...
... flux of a sum or difference of two or more quanti- ties is the sum or difference of the fluxes of the quantities . This is merely the rule for composition of velocities . Flux of a product of two quantities . Let p , q be the quantities ...
Side 65
... FLUX OF PRODUCT AND QUOTIENT . 65 This is equally true when both the factors are scalar quantities , and when one is a scalar and the other a vector . We cannot at present suppose both factors to be vector quantities , because we have ...
... FLUX OF PRODUCT AND QUOTIENT . 65 This is equally true when both the factors are scalar quantities , and when one is a scalar and the other a vector . We cannot at present suppose both factors to be vector quantities , because we have ...
Side 66
... flux of u with regard to x , or the x - flux of u ; and it is denoted by u . Similarly if we make p move vertically with the unit velocity , a will be constant , and y will represent the time , so that u will be 3x + 10y ; this is ...
... flux of u with regard to x , or the x - flux of u ; and it is denoted by u . Similarly if we make p move vertically with the unit velocity , a will be constant , and y will represent the time , so that u will be 3x + 10y ; this is ...
Andre utgaver - Vis alle
Elements of Dynamic: An Introduction to the Study of Motion and ..., Volum 1 William Kingdon Clifford Uten tilgangsbegrensning - 1878 |
Elements of Dynamic: An Introduction to the Study of Motion and ..., Volum 1 William Kingdon Clifford Uten tilgangsbegrensning - 1878 |
Elements of Dynamic: An Introduction to the Study of Motion and ..., Volumer 1-3 William Kingdon Clifford Uten tilgangsbegrensning - 1878 |
Vanlige uttrykk og setninger
abcd acceleration angular velocity approximately axes axis axode bisects ca² called centimeter centrode circle circulation round complex number component compound conjugate diameters constant cross-ratio curvature curve of positions cycloidal cylinder cylindroid described direction displacement draw eccentric anomalies ellipse ellipsoid equal equation equipotential surface expansion finite fixed point flux function given Hence hodograph homogeneous strain hyperbola hyperboloid instant interval inverse length lines of flow magnitude mean velocity moving plane moving point multiplied orbit parabola parallelogram path perpendicular projection quantity radius rate of change ratio represented resultant right angles rigid body rolling rotation scalar screw shew simple harmonic motion solid angle sphere spin step straight line strained position suppose surfaces of revolution theorem translation triangles twist uniform circular motion vector velocity-potential velocity-system vortex-filament zero
Populære avsnitt
Side 102 - A conic is the locus of a point whose distance from a fixed point called the focus is in a constant ratio to its distance from a fixed line, called the directrix.
Side 99 - E, &c., causing the body to describe in the successive intervals of time the straight lines CD, DE, EF, &c., these will all lie in the same plane ; and the triangle SCD will be equal to the triangle SBC, and SDE to SCD, and SEF to SDE. Therefore equal areas are described in the same...
Side iii - CLIFFORD- THE ELEMENTS OF DYNAMIC. An Introduction to the Study of Motion and Rest in Solid and Fluid Bodies.
Side 98 - ... fixed center of force, are in one fixed plane, and are proportional to the times of describing them. Let the time be divided into equal parts, and in the first interval let the body describe the straight line AB with uniform velocity, being acted on by no force. In the second interval it would, if no force acted, proceed to c in AB produced, describing Be equal to AB : so that the equal areas ASB, BSc described by radii AS, BS, cS drawn to the center S, would be completed in equal intervals.
Side 31 - A, it may be resolved into two components, one in the plane PCA and the other perpendicular to it, and both tangential to the spherical surface.
Side 103 - SP-HP=2a; that is, the difference of the focal distances of any point on the hyperbola is equal to the transverse axis. 219. The equation y* = -i (x2 — a2), may be written y=~. (xHence (see Fig. to Art. 213), _ AM.A'M~ AC*' Tangent and Normal to an Hyperbola.
Side 33 - ... the resultant of any number of simple harmonic motions of the same period and in the same line.