Search

4 Nov 2005: Cop. yrig. ht. 200. 5 U. nive. rsity. of C. ambr. ... r. ]. 1. Cop. yrig. ht. 200. 5 U. nive. rsity.

4 Nov 2005: Cop. yrig. ht. 200. 5 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 5 U. nive. rsity. of C.

15 Mar 2005: imposed vertical magnetic field Bz = (200)1/2. Units are such that Lx = Ly/4 = Lz = = ρ = µ0 = 1.

16 Jan 2005: Firstly, to elucidate the stages of the secondary folding we consider a sequence of fiveamino acid regions each of length i = = 200 in our nondimensional units. ... 0 50 100 150 200. 5. 10. 15. 20. the nonlinear Schrödinger equation.

27 Sep 2005: 1-3. 0 100 200 300 400. 50. 100. 150. 200. 250.

19 Sep 2005: DT. Dt=κT. p. Dp. Dt+ Hdiab (2.5). Cop. yrig. ht. 200. ... The relevantsolution of (3.16) is. η(x) = h sgn(x) {1 exp(|x|/LR)} ,. Cop. yrig. ht. 200. 4 U. nive. rsity. of C. ambr.

14 Sep 2005: As seen in Table 1, the actual error for ω = 200 isabout 0.042. ... Table 1: The absolute value of the errors for ω = 200 of the following methods of orderO. (

3 Oct 2005: We. 4. 50 100 150 200 250 300. 0.340.360.38. 0.420.44. Figure 1: The error of QLg [f, (0, 1)], scaled by ω2, with only endpoints and ... 14. 150 200 250 300 350 400. 3.5. 4. 4.5. 5.

12 Jan 2005: 4. Transformed Eq. (2)was expressed in second-order finite difference form us-ing 250 200 grid points, and the resulting nonlinearequations were solved by the Newton-Raphson iterationprocedure using banded

21 Sep 2005: 6040. ω80. 1.4. 200. 1. 0.8. 0.6. 0100. 1.2. 0.4. 0.2. ... 6. 60. 4. 2. 400. 200. ω100. 8. 80 60. 0.5.