Search

15 Dec 2017: Minmod(a, b) =. 0 if ab < 0. a if ab > 0 and |a| < |b|b if ab > 0 and |b| < |a|. ... a if ab > 0 and(|a| < 12|b| or |b| < |a| < 2|b|. ),.

10 Jan 2017: 22 ln A A. ), 212 =. (121 ln B B. ),. ... 21 ln B B. )dX 1. (122 ln A A. )dX 2.

4 Apr 2017: holds. B B 'But from this and the last equation obtained itfollows that.

2 Oct 2017: A b b i l d u n g e n begleitete D a r s t e l l u n g dcr E i n z e l e ... B. Diatomeen), olivengrUne oder spangrtine Farbe (viele Flaggellaten, Oseillarien) besitzen. Rothgef'9 (Haematococcus z.

3 Dec 2017: for the first clear one located close to reservoir B—ultimately break up into lines of periodic spots [Fig.1(b)]. ... Reactants are fed through the well-mixed reservoirs A and B (b) Contrast-enhan.

3 Dec 2017: B. 51 75 72 80 85 85. 1OSBD. 36 37 33 34 32 33. ... U n d e r the circumstances it seems to me best to express the connexion between D and B b y an empirical equation, n a m e l y : - -.

7 Nov 2017: b β(b b‖) (42). and. U(C)1 =. 1. 2. (b. 2. ... and. |γ̇ dr | b‖ 2. 2. 2π. (1 b‖/b)b‖/b. O( 4), (50).

9 Jul 2017: a þ b†b is the total number of particles inthe coupled system. ... Similarly, thecurrent operator between the two condensates is given byJ iða†b b†aÞ 2Sy.

19 Dec 2017: T h e exact result is unity. where b = 2 in this calculation. ... f ( K ) = a l n 2 d 6 - d K b b - d f ( K ‘ ). (38) Here, a = b - d [ b d - 1 - d ( b - l)] is the fraction of decoupled

11 Dec 2017: A B B, ,-------_. D a C, Consider the prism AC in motion relatively to the ether in direction AB with velocity 0. ... the velocity in the free ether; or if f1= then t=fla b.

2 Oct 2017: b b- -. ( ). ( ). ( ) ( ). F y f f. Ay. w. y. wA. y. w. y. ... a, b) Dilute and dense suspensions of motile ellipseswithout hydrodynamical interactions (s = 0).

7 Nov 2017: on the ribbon surface in orders of b b/ 1 and a a/ 1 [35]. ... This derivation generates an integral equation,valid to O(b), with the form.

15 Feb 2017: A , [B, [A , C ]]] = 0, [B, [A , [B, G ]]] = 0, [C , [A , [C , E ]]] = 0, (3.24)[A , [B, [A , E ]]] = 0, [B, [B, [B, C ]]] = 0, [C , [A , [C , G ]]] = ... 0, (3.25)[A , [B, [A , G ]]] = 0, [B, [B, [B, E ]]] = 0, [C , [A , [E , E ]]] = 0, (3.26).

7 Nov 2017: This is shown infigure 2 in the b f– plane for squirmers with random initial orientations. ... 32. 93.56. 11c cb b b< = - » - ( ). This number is off by about a factor of two from the results of our numerical simulations ( 1.8c,numb » - ). Sincethe

11 Dec 2017: F Y Y G1 m b J b —B = a Positive quantity. ... A S x KS l > J p - B’<P$d eb a y - k.

16 Oct 2017: A A’ A’’. B B’ B’’. C C’ C’’. D D’ D’’. ... Orb Merge DAPInlsGFP. C C’ C”. B B’ B”. A A’ A”.

11 Jan 2017: Following [36], we let k = {B gl(N 1) :255ι(B) = B} and p = {B gl(N 1) : ι(B) = B} be the fixed points and anti-fix256points of the automorphism ... abρ′B. Multiplication by b and integration implies the integral bρA(t)aσ(t) =498.

9 Oct 2017: Moreover, we can manipulate the curl terms with. ( B) B = B B (B2)/2 , (4.9). ... E E E E 12E2. ). 1. µ0. (B B B B 1.

2 Oct 2017: Von 0,50 (B]au) an begann dann eine starke Ver- dunkelung des violetteu Endes. ... S c h r e e k b e w e g u n g.

11 Dec 2017: values ofTh and ho:> given in Table 1 ofHodgkin & Huxley (1952c) (method B). ... Thetime scale changes between d, D and e, E. The current scale changes after b, B; c, C; d, Dandf, F.

29 Jul 2017: AB =.  0 11 0.  and A′B′ = 0 11 0. ... kernels of the span of the frame eA′B′C′D′. 30 CHAPTER 2.

7 Apr 2017: M i t 25 T e x t a b b i l d u n g e n. ... die GELEIschen A b b i l d u n g e n fiber Paramevium-Ln'gssehnitte m i t d e m y o n WETZET, a n Flaehschnitten.

3 Dec 2017: Bu-Bi. B/,u. £ Bi2. Bg —. JÏ//Î2. £. ,. BI/M. Bam,. ... B«. B/»i. 0. B. B/a. s. 0. lîs/,,. • • • B,,,,,,—e.

1 Dec 2017: We will use ”abstract indices” a,b,c etc to denote tensors, e.g. ... Aµνfν, e′µ = B. νµeν (2.25). for some matrices Aµν and Bνµ.