## Coefficient Sentence Examples

- Suppose the
**coefficient**of association be n, i.e. - Solving the equation by the Ordinary Theory Of Linear Partial Differential Equations, We Obtain P Q 1 Independent Solutions, Of Which P Appertain To S2Au = 0, Q To 12 B U =0; The Remaining One Is Ab =Aobl A 1 Bo, The Leading
**Coefficient**Of The Jacobian Of The Two Forms. This Constitutes An Algebraically Complete System, And, In Terms Of Its Members, All Seminvariants Can Be Rationally Expressed. - We may, by a well-known theorem, write the result as a
**coefficient**of z w in the expansion of 1 - z n+1. - Ramsay and Shields found from investigations of the temperature
**coefficient**of the surface energy that Tin the equation y(Mv) 3 = KT must be counted downwards from the critical temperature T less about 6°. - But the temperature
**coefficient**of conductivity is now generally less than before; thus the effect of temperature on ionization must be of opposite sign to its effect on fluidity. - The earliest formulation of the subject, due to Lord Kelvin, assumed that this relation was true in all cases, and, calculated in this way, the electromotive force of Daniell's cell, which happens to possess a very small temperature
**coefficient**, was found to agree with observation. - At barometric pressures such as exist between 18 and 36 kilometres above the ground the mobility of the ions varies inversely as the pressure, whilst the
**coefficient**of recombination a varies approximately as the pressure. - For the pressure
**coefficient**per degree, between o° and Ice C., they give the value 0036-6255, when the initial pressure is 700 mm. - In the case of the inductive mode of exciting the oscillations an important quantity is the
**coefficient**of coupling of the two oscillation circuits. - If L and N are the inductances of any two circuits which have a
**coefficient**of mutual inductance M, then M/-/ (LN) is called the**coefficient**of coupling of the circuits and is generally expressed as a percentage. - Two circuits are said to be closely coupled when this
**coefficient**is near unity and to be loosely coupled if it is very small. - Viscosity increases with density, but oils of the same density often vary greatly; the
**coefficient**of expansion, on the other hand, varies inversely with the density, but bears no simple relation to the change of fluidity of the oil under the influence of heat, this being most marked in oils of paraffin base. - This ratio, termed by Guye the critical
**coefficient**, has the following approximate values: C. H. - 6 1.86 3.01 o 88 1.03 Since at the boiling-point under atmospheric pressure liquids are in corresponding states, the additive nature of the critical
**coefficient**should also be presented by boiling-points. - By division we obtain n 3 = 2.121/K i, or n=(2.121/K i) i, the
**coefficient**of association being thus determined. - It is then possible to assign to each body a specific
**coefficient**of affinity. - Arrhenius has pointed out that the
**coefficient**of affinity of an acid is proportional to its electrolytic ionization. - The temperature
**coefficient**of conductivity has approximately the same value for most aqueous salt solutions. - Nevertheless, in certain cases, the temperature
**coefficient**of conductivity becomes negative at high temperatures, a solution of phosphoric acid, for example, reaching a maximum conductivity at 75° C. - We can calculate the heat of formation from its ions for any substance dissolved in a given liquid, from a knowledge of the temperature
**coefficient**of ionization, by means of an application of the well-known thermodynamical process, which also gives the latent heat of evaporation of a liquid when the temperature**coefficient**of its vapour pressure is known. - If we regard the thermal effect at each junction as a measure of the potential-difference there, as the total thermal effect in the cell undoubtedly is of the sum of its potentialdifferences, in cases where the temperature
**coefficient**is negligible, the heat evolved on solution of a metal should give the electrical potential-difference at its surface. - ï¿½ Oxl d 2x 77n If we have new variables z such that zs=4s(yl, Y2,...yn), we have also z s =1 Y 8(x1, x2,ï¿½ï¿½ï¿½xn), and we may consider the three determinants which i s 7xk, the partial differential
**coefficient**of z i, with regard to k . - Now by the theory of symmetric functions, any symmetric functions of the mn values which satisfy the two equations, can be expressed in terms of the
**coefficient**of those equations. - Hence, finally, the resultant is expressed in terms of the
of the three equations, and since it is at once seen to be of degree mn in the**coefficients****coefficient**of the third equation, by symmetry it must be of degrees np and pm in theof the first and second equations respectively.**coefficients** - On the right-hand side is such that the
**coefficient**of x n ix n Zx n 3... - = ...+O(s i s 2 s 3 ...)xl1x12x13...+..., where 0 is a numerical
**coefficient**, then also O ?2 0.3 P1 P2 P3 Al A2 A3 +. - 1 2 3 We have found above that the
**coefficient**of (x 1 1 x 12 x 13...) i n the product XmiXm2X m3 ... - And take therein the
**coefficient**of the function (mi t tm7t t m 31 t ...), we obtain the same result as if we formed the separation function in regard to the specification (mï¿½ It t'tm2 32tm"`l3t...), multiplied by Alt!! - It is definied as having four elements, and is written the
**coefficient**of a0 o a1 a2 2 ... - The number of partitions of a biweight pq into exactly i biparts is given (after Euler) by the
**coefficient**of a, z xPy Q in the expansion of the generating function 1 - ax. - And the weight' of the
**coefficient**of the leading term xi +Q+T+.ï¿½ï¿½ is equal to i+j+k+.... - The internal force F is opposite to the direction of the magnetization, and equal to NI, where N is a
**coefficient**depending only on the ratio of the axes. - The
**coefficient**K/(i +171-K) is positive for ferromagnetic and paramagnetic substances, which will therefore tend to move from weaker to stronger parts of the field; for all known diamagnetic substances it is negative, and these will tend to move from stronger to weaker parts. - For small bodies other than spheres the
**coefficient**will be different, but its sign will always be negative for diamagnetic substances and positive for others; hence the forces acting on any small body will be in the same directions as in the case of a sphere' Directing Couple acting on an Elongated Body. - 1 -az 74 - 2.1 -azn-4....1 - azn+4.1 - az n+2.1 - az-n in which we have to take the
**coefficient**of aezne-2', the expansion. - In general the
**coefficient**, of any product A n A m A 7, 3 ..., will have, as**coefficient**, a seminvariant which, when expressed by partitions, will have as leading partition (preceding in dictionary order all others) the partition (Tr1lr2lr3ï¿½..). - The existence of such a relation, as 0-1+0-2+.,.+cr2=0, necessitates the vanishing of a certain function of the
A2, A 3, ...A 9, and as a consequence one product of these**coefficients**can be eliminated from the expanding form and no seminvariant, which appears as a**coefficients****coefficient**to such a product (which may be the whole or only a part of the complete product, with which the seminvariant is associated), will be capable of reduction. - The generating function is I - z2' 52 For 0 =3, (alai +a2a2+a3a3) 10; the condition is clearly a1a2a3 = A3 = 0, and since every seminvariant, of proper degree 3, is associated, as
**coefficient**, with a product containing A3, all such are perpetuants. - The Number Of Linearly Independent Seminvariants Of The Given Type Will Then Be Denoted By (W; 0, P; 0', Q) (W; 0, P; 0', Q); And Will Be Given By The
**Coefficient**Of A E B E 'Z W In L Z 1 A. - Two of these show that the leading
**coefficient**of any covariant is an isobaric and homogeneous function of theof the form; the remaining two may be regarded as operators which cause the vanishing of the covariant.**coefficients** - Let a covariant of degree e in the variables, and of degree 8 in the
(the weight of the leading**coefficients****coefficient**being w and n8-2w = ï¿½), be Coxl -}- ec l l 1 x 2 -{-... - It is for this reason called a seminvariant, and every seminvariant is the leading
**coefficient**of a covariant.