## Dynamical Sentence Examples

- Devoting himself next to optics, he produced memoirs which entitle him to a high place among the early, searchers after a true
**dynamical**theory of light. - In 1832, by the aid of a particular hypothesis as to the constitution of the ether, he reached by a rigorous
**dynamical**calculation results agreeing with those obtained by A. - Though we may allow that the results obtained by Rumford and Davy demonstrate satisfactorily that heat is in some way due to motion, yet they do not tell us to what particular
**dynamical**quantity heat corresponds. - The
**dynamical**equilibrium between rhombic, liquid and monosymmetric sulphur has been worked out by H. - Therefore, according to Kekule, the double linkages are in a state of continual oscillation, and if his
**dynamical**notion of valency, or a similar hypothesis, be correct, then the difference between the 1.2 and 1.6 di-derivatives rests on the insufficiency of his formula, which represents the configuration during one set of oscillations only. - A
**dynamical**theory due to E. - The heading "Measurement of
**Dynamical**Quantities" includes the topics units, measurements, and the constant of gravitation. - Mechanics (including
**dynamical**astronomy) is that subject among those traditionally classed as "applied" which has been most completely transfused by mathematics - that is to say, which is studied with the deductive spirit of the pure mathematician, and not with the covert inductive intention overlaid with the superficial forms of deduction, characteristic of the applied mathematician. - The
**dynamical**equivalent of the calorie is 4.18 X Io 7 ergs or C.G.S. - Thomson (Applications of Dynamics to Physics and Chemistry, 47) that on
**dynamical**principles there must be a reciprocal relation between the changes of dimensions produced by magnetization and the changes of magnetization attending mechanical strain. - Besides this most important contribution to the general fabric of
**dynamical**science, we owe to Lagrange several minor theorems of great elegance, - among which may be mentioned his theorem that the kinetic energy imparted by given impulses to a material system under given constraints is a maximum. - Although the matter can be fully treated only upon the basis of a
**dynamical**theory, it is proper to point out at once that there is an element of assumption in the application of Huygens's principle to the calculation of the effects produced by opaque screens of limited extent. **Dynamical**Theory of Diffraction.- This question was treated by Stokes in his "
**Dynamical**Theory of Diffraction " (Camb. - Cohnheim (1839-1884) and of Iliya Metchnikoff on the
**dynamical**side of his- Fevers tology. - Calling the sum of the pressure and potential head the statical head, surfaces of constant statical and
**dynamical**head intersect in lines on H, and the three surfaces touch where the velocity is stationary. - In the general motion again of the liquid filling a case, when a = b, 52 3 may be replaced by zero, and the equations, hydrodynamical and
**dynamical**, reduce to d =- 2+ 2 J, = 2 x22111, d = 2 2`2 (+/'15-Om) (1 yy y n`t dt a +c dt a +c dt a +c) dc2, a2-1-c2 d122 a2 c2 dt ="2) +a2= G2y 71' dt = 121 1 - a 2 -c 2SJ, (19) of which three integrals are e +777 r z y 2= L -?2J2, (20) (a2 + c2) 2 2 121+14 =M+ 2c2(a2-c2)1 ' (21) 121+522hN = + x24 2,2 and then (dt / 2 = (a2 + c 2) 2(° v 2 - 12171) 2 4C4 2 2 - (+ c2)2?(E+77) (? - Thus if T is expressed as a quadratic function of U, V, W, P, Q, R, the components of momentum corresponding are dT dT dT (I) = dU + x2=dV, x3 =dW, dT dT dT Yi dp' dQ' y3=dR; but when it is expressed as a quadratic function of xi, 'x2, x3, yi, Y2, Y3, U = d, V= dx, ' w= ax dT Q_ dT dT dy 1 dy2 dy The second system of expression was chosen by Clebsch and adopted by Halphen in his Fonctions elliptiques; and thence the
**dynamical**equations follow X = dt x2 dy +x3 d Y = ..., Z ..., (3) = dt1 -y2?y - '2dx3+x3 ' M =.. - When no external force acts, the case which we shall consider, there are three integrals of the equations of motion (i.) T =constant, x 2 +x 2 +x 2 =F 2, a constant, (iii.) x1y1 +x2y2+x3y3 =n = GF, a constant; and the
**dynamical**equations in (3) express the fact that x, x, xs. - The precedin investigation, the liquid stops dead when the body is brought to rest and when the body is in motion the surrounding liquid moves in uniform manner with respect to axes fixed in the body, and the force experienced by the body from the pressure of the liquid on it surface is the opposite of that required to change the motion of the liquid; this has been expressed by the
**dynamical**equations give above. - 00 ab2dX °0 ab2dX (22) L (I JS)' (18) (t9) This impulse will remain of constant magnitude, and fixed relatively to the body, which thus experiences an additional reaction from the circulation which is the opposite of the force required to change the position in space of the circulation impulse; and these extra forces must be taken into account in the
**dynamical**equations. - Social physics will consist of the conditions and relations of the facts of society, and will have two departments, - one, statical, containing the laws of order; the other
**dynamical**, containing the laws of progress. - In later memoirs Reynolds followed up this subject by proceeding to establish definitions of the velocity and the momentum and the energy at an element of volume of the molecular medium, with the precision necessary in order that the
**dynamical**equations of the medium in bulk, based in the usual manner on these quantities alone, without directly considering thermal stresses, shall be strictly valid - a discussion in which the relation of ordinary molar mechanics to the more complete molecular theory is involved. - A number of molecules moving in obedience to
**dynamical**laws will pass through a series of configurations which can be theoretically determined as soon as the structure of each molecule and the initial position and velocity of every part of it are known. - We begin with a general
**dynamical**theorem, whose special application, when the**dynamical**system is identified with a gas, will appear later. - Qr,, be the generalized coordinates of any
**dynamical**system, and let pi, P2, - Are very large, then, for all states except an infinitesimal fraction of the whole number, the values of u, v, w lie within ranges such that (i) the values of u (and similarly of v, w) are distributed among the s molecules of the first kind according to the law of trial and error; and similarly of course for the molecules of other kinds: (ii) E2mu2 E2mv 2 E2mw2 ?2aie12 s S s s s s - s E s' S' s' - - s' ' See Jeans,
**Dynamical**Theory of Gases (1904), ch. - The planetary theory and other particular
**dynamical**problems likewise occupied his attention from time to time. - Lamb, The
**Dynamical**Theory of Sound (1910), is intended as a stepping-stone to the study of-the writings of Helmholtz and Rayleigh. - These antinomies are four - two mathematical, two
**dynamical**- connected with (I) the limitation of the universe in respect of space and time, (2) the theory that the whole consists of indivisible atoms (whereas, in fact, none such exist), (3) the problem of freedom in relation to universal causality, (4) the existence of a universal being - about each of which pure reason contradicts the empirical, as thesis and antithesis. - (2) An allowance is sometimes made for impact, that is the
**dynamical**action of the live load due to want of vertical balance in the moving parts of locomotives, to irregularities of the permanent way, or to yielding of the structure. - It has been repeatedly claimed for Mayer that he calculated the value of the
**dynamical**equivalent of heat, indirectly, no doubt, but in a manner altogether free from error, and with a result according almost exactly with that obtained by J. - The wider view, according to which the hypothesis of direct transmission of physical influences expresses only part of the facts, is that all space is filled with physical activity, and that while an influence is passing across from a body, A, to another body, B, there is some
**dynamical**process in action in the intervening region, though it appears to the senses to be mere empty space. - MacCullagh's hands the correct equations were derived from a single energy formula by the principle of least action; and while the validity of this
**dynamical**method was maintained, it was frankly admitted that no mechanical analogy was forthcoming. - In this place it must suffice to indicate the gist of the more recent developments of the electro-optical theory, which involve the
**dynamical**verification of Fresnel's hypothesis regarding optical convection and the other relations above described. - The latter force is, by Maxwell's hypothesis or by the
**dynamical**theory of an aether pervaded by electrons, the same as that which strair s the aether, and may be called the aethereal force; it thereby produces an aethereal electric displacement, say (f,g,h), according to the relation (f,g,h) = (41 r c 2) - 1(P',Q', RI), in which c is a constant belonging to the aether, which turns out to be the velocity of light. - Acting on the electrons situated on it which move with the velocity of the matter) is equal to minus the time-rate of change of the magnetic induction through that circuit as it moves with the matter, this being a
**dynamical**consequence of the aethereal constitution assigned in (i). - The
**dynamical**series of stages in nature, the forms in which the ideal structure of nature is realized, are matter, as the equilibrium of the fundamental expansive and contractive forces; light, with its subordinate processes - magnetism, electricity, and chemical action; organism, with its component phases of reproduction, irritability and sensibility.' - Just as nature exhibits to us the series of
**dynamical**stages of processes by which spirit struggles towards consciousness of itself, so the world of intelligence and practice, the world of mind, exhibits the series of stages through which self-consciousness with its inevitable oppositions and reconciliations develops in its ideal form. - Lord Rayleigh,' who has also investigated vibrating systems giving series of lines approaching a definite limit of " root," remarks that by
**dynamical**reasoning we are always led to equations giving the square of the period and not the period, while in the equation representing spectral series the simplest results are obtained for the first power of the period. - The discovery of the magnetic rotation of the plane of polarized light, though it did not lead to such important practical applications as some of Faraday's earlier discoveries, has been of the highest value to science, as furnishing complete
**dynamical**evidence that wherever magnetic force exists there is matter, small portions of which are rotating about axes parallel to the direction of that force. - A definition of the measurement dependent on
**dynamical**theory has Time. - Nevertheless, the theoretical possibility, and its realization in many cases, has brought considerations to the front which have recently become of predominant interest; consequently the possible transformations of isomers and polymers will be considered later under the denomination of reversible or
**dynamical**isomerisms. - Th~ axial moments have alone a
**dynamical**significance, but the others are useful as subsidiary conceptions. - But from the
**dynamical**standpoint it is obvious that equations which represent the facts correctly on one system of time-measurement might become seriously defective on another. - (See also UNITS, DIMENSIONS or.) In any absolute system of
**dynamical**measurement the fundamental units are those of mass, length and time we may denote them by the symbols M, L, T, respectively They may be chosen quite arbitrarily, e.g. - In any general
**dynamical**equation the dimensions of each term in the fundamental units must be the same, for a change of units would otherwise alter the various terms in different ratios. - For the determination of the motion it has only, been necessary to use one of the
**dynamical**equations. - QX +Pu = N.j These equations are applicable to any
**dynamical**system whatever. - When the origin of the moving axes is also in motion with a velocity whose components are u, v, w, the
**dynamical**equations are ~rn+qi=X, ~pl+rE=Y, ~f_qE+Pi,=Z, (II)