## Pi Sentence Examples

- In 2009,
**pi**was calculated to more than two trillion digits—in less than thirty hours. - We consider a system of points
**Pi**, P1.. - Oldenberg, The Vinaya
**Pi**(akam (5 vols., London, 1879-1883); V. - ': opal e ° °o T A R ple ' ag a ',ap iJ,wl Karkinit A C K r B L Scale, English Miles D S E A 32 Stavropol P O L A
**PI**A N L A s E Derbent ° I? - 1 It has also been pointed out that the employment of the sign
**PI**for wa and the use of z for s, cited in support of the earlier date, survived in the Kassite period. - (From Gegenbaur,
**pi**, Pallial nerve. - Mines are also worked at Kwanyin-shan, opposite the Russian frontier town of Radevska, and at Chia-
**pi-kou**, on an affluent of the upper Sungari. - I eac
**Pi**c sto ?ers De o teon ? - A partition, (pipipip2p2p3) = can be separated in the manner (p 1 p 2) (PIP2) (p1P3) = (1)12,2) 2 (plp3), and we may take the general form of a partition to be (
**pi**i p2 2 p3 3 ...) and that of a separa tion (J 1) 1 1(J 2) 5 2(J 3) 1 3... - .-1 (
**PI**+V2+V3+...- 1)! **Pi**, Pulmonary lamellae.- The oldest and for the most part Jewish portion of this literature is preserved to us in Greek, Armenian, Latin and Slavonic. (i.) The Greek Ooryr7vcs r€
**pi**'ASaµ rcai Eras (published under the misleading title 'AlroicaXvi/ics Mwvo ws in Tischendorf's Apocalypses Apocryphae, 1866) deals with the Fall and the death of Adam and Eve. - Of the amphibious rodents, the
**pi-ea**(Cavia aperea), mod, (C. rupestris), paca (Coelogenys paca), cutia (Dasyprocta aguti) and capybara (Hydrochoerus capybara) are noteworthy for their size and extensive range. - Whose coefficients are connected by a relation of the form pocr+plcr_1+...-i-pkcr-k= o, where po,
**pi**, ï¿½ ..pk are independent of x and of r. - 14, &c.), a derivative of the verb hitter (
**Pi**.) or hiktir (Hiph.), which verb is used, not only in Ex. - A considerable school of carvers soon began to work in the Matsumoto style, and hundreds of their
**pi-oductions**have gone to Europe and America, finding no market in Japan. - Qr,, be the generalized coordinates of any dynamical system, and let
**pi**, P2, - If the system is supposed to obey the conservation of energy and to move solely under its own internal forces, the changes in the co-ordinates and momenta can be found from the Hamiltonian equations aE aE qr = 49 - 1 57., gr where q r denotes dg r ldt, &c., and E is the total energy expressed as a function of
**pi**, qi,. - Let us suppose that an infinite number of exactly similar systems start simultaneously from all possible values of
**pi**, q1, - Let us confine our attention to those systems for which the initial values of
**pi**, qi, ... - Pn, qn lie within a range such that p t is between p i and
**pi**+dpi qi „ „ qi „ qi +dq i, and so on. - Thus after a time dt the values of the coordinates and momenta of the small group of systems under consideration will lie within a range such that
**pi**is between**pi**+**pidt**and**pi**+dp,+(**pi**+ap?dpi) dt „ qi +gidt „ qi+dqi+ (qi +agLdgi) dt, Thus the extension of the range after the interval dt is dp i (i +aidt) dq i (I +?gidt). - From equations (i), we find that aq _ o a
**pi**qi -, so that the extension of the new range is seen to be dp i dq i ... - This is equivalent to a steady pressure p i per unit area where +0
**pi**- zfff v J 1 (h3m3/ir3)e hm(u2+v2+w2)mu2dudvdw. - TO Ti ?
**pi**€ivat), i.e. - Then, if the true moments are denoted by
**Pi**, v 2, ..., their values are given by vi ?Pl P2 - 11. - Of travelling loads at fixed distances, let
**PI**, P2, P3,. - Then the economic span is 1= loo-1
**PI**/ G. **Pi**Margall, and A.- AiyEl 'IT] O'oUS iav µi 7 v77(rTEb(r77TE Ten, KOopOV p1 7 EUpr7TE Ti) v (3a0'i%ELav Beou' Kai iav
**pi**7 (ra013aTi(rr 7 TE TO aciMarov obi(64Ã†cree 7raripa. - Xiyel '177(eou)s' [ra y Tb
**pi**) 1p7rpo(rBEV T9] S t4'dWS (rOV Kai [TO KEKpvppivov Q7rO vol3 h7roKaXv4(0)i crer[ai O"ot. - Let (x1, yi, Zi) be the co-ordinates of a point
**Pi**on the line of action of one of the forces, whose components are (say) X1, Yi, Zi. - The force X1 at
**Pi**with K - - If through
**Pi**, Pf,. - In,., acting at
**Pi**, P2. - If
**Pi**, P2,. - Denoting these limits by
**Pi**, Pa we have P1/W=L1H/HK=sin (aX)/cos (0+X), **Pi**/W=L1H/HK=sin (a+X)/cos (0X).- It appears, moreover, that if 0 be varied P will be least when L1H is at right angles to KLi, in which case
**Pi**=W sin (aX), corresponding to 0 = X. - A number of particles attached at various points of a string are acted on by given extraneous forces
**Pi**, P, P3. - The given forces
**Pi**,**Pi**, P2.. - As a special, but very important case, the forces
**Pi**, F2, P~...