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For L2C signal, as shown in Fig.1, the navigation message is a 25 bps data stream which is coded by a rate 1/2 convolutional coder.
Fig.1 Block diagram of L2C signal structure.
Fig.6 shows the 3D plot of C/A code acquisition, max at (479,19) means the code phase difference and the Doppler frequency offset are 479 chips and 3KHz (500Hz×(19-13)) at the maximum correlation peak.
Then 20 possible initial phases of CM code can be calculated as 479+i×1023, i=1:20.
The correlation peak is the 9th, so the initial phase of CM code is 9686 (479+9×1023).

Fig. 1 Grain size distribution of kaolinite clay and burning shell Sample preparation Five mixing ratios (kaolinitic clay : burning shell) by weight were prepared including 1:0.6, 1:0.8, 1:1, 1:1.3 and 1:1.6.
The result shows that the specimen temperature steady increased and reached about 440 oC to 479 oC after it was exposed to the heat temperature of 1,100 oC for about 15 minutes.
By subjecting the specimen to the heat of 1,100 oC, the specimen temperature reaches 440 oC to 479 oC within about 15 minutes and remains constant.
References [1] J.
Vol. 479-481 (2012), p. 357 [20] M.W.

%TiO2 coatings sprayed with the CPSP of 361, 427, 479, and 574 are referred to as 'A1', 'A2', 'A3', and 'A4', respectively.
%TiO2 coatings are shown in Figs. 1(a) and (b).
Table 1.
Volume Fraction (%) CPSP α-Al2O3 Partially Melted Region Pore Coating Thickness (µm) Bulk Density (g/cm3) 361 17.1 25.3 7.19 320 3.22 427 12.8 19.5 6.93 320 3.10 479 10.2 15.1 6.29 390 3.31 574 6.4 8.6 5.02 340 3.23 Fig. 1.
References [1] L.

The results of these calculations are summarized in Table 1.
Table 1.
This microstructural feature is now understood as a manifestation of the Kirkendall effect [1].
The average compositions of the reaction products were calculated as Ag0.154Zn0.846 for the ε"AgZn3" phase, Ag0.394Zn0.606 for the γ-"Ag5Zn8" and Ag0.521Zn0.479 for the β-"AgZn" phase.
References [1] A.

Diarylethene 1a changed the color from colorless to Orange-red upon irradiation with 297 nm UV light, in which absorption maxima were observed at 479 nm in hexane and at 485 nm in PMMA amorphous film, respectively.
Scheme 1.
The colorless 1a has the absorption maxima at 281 nm (ε, 1.7×104 mol-1 L cm-1).
Figure 1.
References [1] G.H.

Research on GPS height partition fitting method Chang Wang1, a 1 University of Science and Technology Liao Ning School of Civil Engineering, AnShan LiaoNing awangchang324@163.com Keywords: Partition Fitting;The Quadric Surface Fitting; Mobile Triangle Method Abstract.
（2）Use mobile triangle method to establish GPS height fitting method in 1 area, 2area , 6area, 7area and 8 area, from table2, 3 and fig.4～7 can see GPS height fitting result, Table 2 The quadric surface fitting accuracy in four regions unit :mm name 3region 5region 9region 4region internal accord precision 11.7 8.4 8.8 17.3 external accord accuracy 8.6 9.3 11.0 29.8 Table 3 Mobile triangle method fitting accuracy unit :mm 1 region check point residual value δ=46.29 2 region check point residual value δ=1.96 6 region check point residual value δ=31.73 411 46.29 402 1.96 455 31.73 7 region check point residual value δ=17.9 8 region check point residual value δ=33.82 443 476 17 18.78 479 33.82 Fig.4 The residual value comparison of the public point in 3 region in no partition and partition situation Fig.5 The residual value comparison of the public points in 5 region in no partition and partition situation Fig.6 The residual value comparison
From fig.7,we can see that the residual value of three points(402, 443, 479) is less than that in no partition situation by mobile triangle method in 2 region, 7 region and 8 region.
Summary 1.If the effect of GPS height fitting is better in whole region, use partition fitting to establish fitting model in this region can effectively improves the fitting precision. 2.
Reference [1]Gongyusheng.

The samples without visible defects showed a mean conventional tensile failure stress of 479 MPa and a residual deformation of about 0.04%, which confirms their brittleness when not heat-treated.
The latter can show magnetically induced strain (MIS) much higher than magnetostrictive alloys do due to martensitic transformation taking place in FSMA [1].
The parameters are presented in Table 1.
(1) Table 1 – SLM modes used for manufacturing Ni36Co37Al27 samples Mode P, [W] v, [mm/s] h, [mm] t, [mm] Energy density, [J/mm3] 1 225 500 0.06 0.05 150 2 200 550 0.08 0.05 91 3 200 480 0.12 0.05 69 4 300 500 0.06 0.05 200 5 200 550 0.06 0.05 121 6* 200 550 0.06 0.05 121 7* 225 500 0.06 0.05 150 8* 300 500 0.06 0.05 200 The modes marked with * means that every layer was preliminary scanned by 1000 W laser with the following parameters: P = 300 W, v = 2000 mm/s, h = 0.12 mm, t = 0.05 mm.
References [1] E.

A large scope plastic zone emerges in the northern slope of the pit between exploratory lines 479 and 491.
The designed scope of slope cutting is shown in Fig.1.
After a large deformation emerged, the northern slope of the pit between exploratory lines 479 and 491 reaches a new state of balance.
Analysis and calculation show that this is a limit equilibrium state, and the safety factor is close to 1.
Vol. 1 (2004), p.72

Some aging properties and stochastic comparisons on the residual life are obtained. 1.
For more details about order statistics, see [1], and [2] etc.
And from Theorem 1.C.37 of [4], for all , and , hence from Theorem 1.C.17 of [4] again, the result holds.
References [1] H.A.
Wang, The NBUC and NWUC classes of life distributions, Journal of Applied Probability 31 (1991) 473-479

Low Analysis of Steady Flow Field in Mechanical Seal Based on ANSYS Zhu Yuefeng 1,2,a Chen Delin 2,b 1 Hefei University of Technology,Hefei,China 2 Kaifeng University, Kaifeng, He Nan, China akufao@sohu.com Keywords: mechanical seal; flow field; cloud; ANSYS Abstract.
Finite element model of the grid shown in Fig.1: Fig.1 Finite element model picture Loading and the Solving.
References [1] Jiang Xiaowen, Gu Boqin.
Journal of Xi'an Jiaotong University, 2004,38(5):474-479( In Chinese) [4] Zhong Ru-lin, Chen Ci-chang, Guan Jian-feng.
Sichuan University of Science andTechnology, 2004,38(5):474-479( In Chinese) [5] Parviz Merati, Nori Aki Okita, Robert L Phillips.