## Resultant Sentence Examples

- Through the
**resultant**scarcity of labor, much land fell out of cultivation. - The main branches of the
**resultant**" tree " may be rendered as follows: [[Coraciomorphae Odontolcae..Colymbo-+Pelargoalectoromorphae..Ratitae Morphae Morphae ' 'Neornithes]] The Odontolcae seem to be an early specialized offshoot of the Colymbo-Pelargomorphous brigade, while the Ratitae represent a number of side branches of early Alectoromorphae. - The general character of the country,
**resultant**on these conditions, varies according to elevation and latitude. - Temperance and the
**resultant**health and vigour). - There is no difficulty in expressing the
**resultant**by the method of symmetric functions. - The historian evidently decomposes Alexander's power into the components: Talleyrand, Chateaubriand, and the rest--but the sum of the components, that is, the interactions of Chateaubriand, Talleyrand, Madame de Stael, and the others, evidently does not equal the
**resultant**, namely the phenomenon of millions of Frenchmen submitting to the Bourbons. - The radiations interfere in an optical sense of the word, and in some directions reinforce each other and in other directions neutralize each other, so making the
**resultant**radiation greater in some directions than others. - It is also the custom to balance a proportion of the reciprocating masses by balance weights placed between the spokes of the wheels, and the actual balance weight seen in a driving-wheel is the
**resultant**of the separate weights required for the balancing of the revolving parts and the reciprocating parts. - Another of Roberval's discoveries was a very general method of drawing tangents, by considering a curve as described by a moving point whose motion is the
**resultant**of several simpler motions. - He treated the
**resultant**electric force at any point as analogous to the flux of heat from sources distributed in the same manner as the supposed electric particles. - When the solutions of two substances are mixed, similar considerations to those given above enable us to calculate the
**resultant**changes in dissociation. - Thus, the thermal equivalent of the unit of
**resultant**electrochemical change in Daniell's cell is 5.66 - 3.00 =2.66 calories. - R is a function of the coefficients which is called the "
**resultant**" or " eliminant " of the k equations, and the process by which it is obtained is termed " elimination." - If al, a2, ...a, n be the roots of f=o, (1, R2, -Ai the roots of 0=o, the condition that some root of 0 =o may qq cause f to vanish is clearly R s, 5 =f (01)f (N2) ï¿½ ï¿½;f (Nn) = 0; so that Rf,q5 is the
**resultant**of f and and expressed as a function of the roots, it is of degree m in each root 13, and of degree n in each root a, and also a symmetric function alike of the roots a and of the roots 1 3; hence, expressed in terms of the coefficients, it is homogeneous and of degree n in the coefficients of f, and homogeneous and of degree m in the coefficients of 4.. - This expression of R shows that, as will afterwards appear, the
**resultant**is a simultaneous invariant of the two forms. - +al pxp = 0, a21x1 +a22x2 + ï¿½ ï¿½ ï¿½ +a2pxp = 0, aplxl+ap2x2+...+appxp = 0, be the system the condition is, in determinant form, (alla22...app) = 0; in fact the determinant is the
**resultant**of the equations. - Forming the
**resultant**of these equations we evidently obtain the**resultant**of f and 4,. - Thus to obtain the
**resultant**of aox 3 +a i x 2 +a 2 x+a 3, 4, =box2+bix+b2 we assume the identity (Box+Bi)(aox 3 +aix 2 +a2x+a3) = (Aox 2 +Aix+ A 2) (box2+bix+b2), and derive the linear equations Boa ° - Ac b o = 0, Boa t +B i ao - A 0 b 1 - A 1 bo =0, Boa t +B 1 a 1 - A0b2 - A1b1-A2b° = 0, Boa3+Bla2 - A l b 2 -A 2 b 1 =0, B 1 a 3 - A 2 b 2 =0, = = (y l, y2,...ynl `x1, x2,...xnl for brevity. - And by elimination we obtain the
**resultant**ao 0 bo 0 0 al ao b1 bo 0 a 2 a i b 2 b 1 bo a numerical factor being disregarded. - Taking the same example as before the process leads to the system of equations acx 4 +alx 3 +a2x 2 +a3x =0, aox 3 +a1x 2 +a2x+a 3 = 0, box +bix -1-b2x =0, box' +b i x 2 -{-h 2 x = 0, box + b i x + b:: = 0, whence by elimination the
**resultant**a 0 a 1 a 2 a 3 0 0 a 0 a 1 a 2 a3 bo b 1 b 2 0 0 0 bo b 1 b 2000 bo b 1 b2 which reads by columns as the former determinant reads by rows, and is therefore identical with the former. - Bezout's method gives the
**resultant**in the form of a determinant of order m or n, according as m is n. - He first divides by the factor x -x', reducing it to the degree m - I in both x and x' where m>n; he then forms m equations by equating to zero the coefficients of the various powers of x'; these equations involve the m powers xo, x, - of x, and regarding these as the unknowns of a system of linear equations the
**resultant**is reached in the form of a determinant of order m. - Put (aox 3 -}-a l x 2 +a 2 x +a 3) (box' +b1x'+b2) - (aox'3+aix'2+a2x'+a3) (box' + bix + b2) = 0; after division by x-x the three equations are formed aobcx 2 = aobix+aob2 =0, aobix 2 + (aob2+a1b1-a2bo) x +alb2 -a3bo = 0, aob2x 2 +(a02-a3bo)x+a2b2-a3b1 =0 and thence the
**resultant**aobo ao aob2 aob 1 aob2+a1b1-a2bo alb2-a3b0 aob 2 a1b2 - a 3 bo a2b2 - a3b1 which is a symmetrical determinant. - = 0, we find that, eliminating x, the
**resultant**is a homogeneous function of y and z of degree mn; equating this to zero and solving for the ratio of y to z we obtain mn solutions; if values of y and z, given by any solution, be substituted in each of the two equations, they will possess a common factor which gives a value of x which, corn bined with the chosen values of y and z, yields a system of values which satisfies both equations. - Hence this product is the required
**resultant**of the three equations. - Hence, finally, the
**resultant**is expressed in terms of the coefficients of the three equations, and since it is at once seen to be of degree mn in the coefficient of the third equation, by symmetry it must be of degrees np and pm in the coefficients of the first and second equations respectively. - The general theory of the
**resultant**of k homogeneous equations in k variables presents no further difficulties when viewed in this manner. - It is the
**resultant**of k polynomials each of degree m-I, and thus contains the coefficients of each form to the degree (m-I)'-1; hence the total degrees in the coefficients of the k forms is, by addition, k (m - 1) k - 1; it may further be shown that the weight of each term of the**resultant**is constant and equal to m(m-I) - (Salmon, l.c. p. loo). - This can be seen at once because the factor in question being once repeated in both differentials, the
**resultant**of the latter must vanish. - Af Expression in Terms of Roots.-Since x+y y =mf, if we take cx any root x 3, y1, ofand substitute in mf we must obtain, y 1 C) zaZ1 ï¿½; hence the
**resultant**of and f is, disregarding numerical factors, y,y2...y,,. - (x y m - x m y), ar _ y1(x y 2 - and substituting in the latter any root of f and forming the product, we find the
**resultant**of f and d, viz. - The process of magnetization consists in turning round the molecules by the application of magnetic force, so that their north poles may all point more or less approximately in the direction of the force; thus the body as a whole becomes a magnet which is merely the
**resultant**of an immense number of molecular magnets. - Terminate outside the magnet or inside, have a
**resultant**, equal to the sum of the forces and parallel to their direction, acting at a certain point N. - Similarly, the forces acting in the opposite direction on the negative poles of the filaments have a
**resultant**at another point S, which is called the south or negative pole. - The line through the given point along which the potential decreases most rapidly is the direction of the
**resultant**magnetic force, and the rate of decrease of the potential in any direction is equal to the component of the force in that direction. - If V denote the potential, F the
**resultant**force, X, Y, Z, its components parallel to the co-ordinate axes and n the line along which the force is directed, then - sn = F, b?= X, - Sy = Y, -s Surfaces for which the potential is constant are called equipotential surfaces. - The
**resultant**magnetic force at every point of such a surface is in the direction of the normal (n) to the surface; every line of force therefore cuts the equipotential surfaces at right angles. - For the
**resultant**force at P, F=-VF r 2. - Since 7ra'I is the moment of the sphere (=volume X magnetization), it appears from (10) that the magnetized sphere produces the same external effect as a very small magnet of equal moment placed at its centre and magnetized in the same direction; the
**resultant**force therefore is the same as in (14). - The
**resultant**magnetic field, therefore, is compounded of two fields, the one being due to the poles, and the other to the external causes which would be operative in the absence of the magnetized metal. - Magnetization is usually regarded as the direct effect of the
**resultant**magnetic force, which is therefore often termed the magnetizing force. - Demagnetizing Force.-It has already been mentioned that when a ferromagnetic body is placed in a magnetic field, the
**resultant**magnetic force H, at a point within the body, is compounded of the force H o, due to the external field, and of another force, Hi, arising from the induced magnetization of the body.