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Experimental design is shown in Table 1.
Pectinase and cellulase, a ratio of 1:2 for the best.
Table 3 Box-Behnken design and results Table 4 Coefficient significance test of regression equation Experimental point A B C Y flavonoid（％） 1 0 1 1 0.8618 2 1 1 0 0.9235 3 1 0 1 0.8183 4 0 -1 1 0.8312 5 -1 1 0 0.9273 6 -1 -1 0 0.9631 7 0 1 -1 0.8064 8 0 0 0 1.1125 9 -1 0 -1 0.7951 10 0 0 0 1.1097 11 1 -1 0 0.8579 12 1 0 -1 0.7611 13 0 -1 -1 0.7568 14 -1 0 1 0.8439 15 0 0 0 1.1186 item coefficient Coefficient standard deviation T P significant constant 1.11360 0.006999 159.108 0.000 ** A -0.02108 0.004286 -4.917 0.004 ** B 0.01375 0.004286 3.208 0.024 * C 0.02947 0.004286 6.877 0.001 ** A*A -0.10255 0.006309 -16.255 0.000 ** B*B -0.09310 0.006309 -14.757 0.000 ** C*C -0.20645 0.006309 -32.724 0.000 ** A*B 0.02535 0.006061 4.182 0.009 ** A*C 0.00210 0.006061 0.346 0.743 B*C -0.00475 0.006061 -0.784 0.469 note：** extremely significant level (P < 0. 01) ； * significant level (P < 0. 05)。
Chemistry, 2005, (68) :1-3
Journal of Jilin University (Engineering Science), 2007,37 (2) :479-483

Modeling and Simulation Calculation of a Overwater Autonomous Air Defense Weapon System Bowei Zhao 1,a， Faxing LU 1,b，Xiaowei Tang 2,c 1College of Electronic Engineering,Naval University,Wuhan 430033,China 2Navy 92730,Sanya 572016,China azhaoboweinavy@163.com Keywords: floating platform autonomous air defense weapon accuracy analysis capture probability Abstract.
How to ensure island security and reinforce island defense has become an issue that requires great attention[1]~[2].
The system’s precision chain derived from this is shown in figure 1.
Table 2 The results of the simulation parameters the first capture probability the final capture probability the time of the capture (s) the base value 0.913 1.000 6.776 =0.1° 0.923 1.000 4.182 =1.5° 0.781 1.000 9.615 =0.1° 0.926 1.000 4.638 =1.5° 0.733 1.000 12.124 =5m 0.913 1.000 6.721         =50m 0.907 1.000 7.733 =5m/s 0.912 1.000 6.770 =20m/s 0.889 1.000 9.762 =1° 0.925 1.000 4.399 =5° 0.850 1.000 7.244 =0.5m 0.915 1.000 5.395 =1.5m 0.914 1.000 5.432 =0.3° 0.961 1.000 4.342 =1.5° 0.766 1.000 9.805 =0.3° 0.928 1.000 9.643 =1.5° 0.558 1.000 19.742 ： 0.951 1.000 6.518 ： 0.361 1.000 41.877 ： 0.913 1.000 7.257 ： 0.908 1.000 7.225 ： 0.917 1.000 4.037 ： 0.916 1.000 7.291 ：cm 0.919 1.000 4.306 ：cm 0.868 1.000 4.194 ： 0.450 1.000 10.121 ： 1.000 1.000 2.421 ：s 0.894 1.000 6.979 ：s 0.890 1.000 4.127 The following conclusions can be got from the results of the simulation: 1) The accuracy of the detection of the sensor has a great influence on the accuracy of the weapon’s strike against the
[6] Hongmei Li: Error Transfer and Sensitivity Analysis of Ship-Borne Radar Detecting Journal of Data Acquisition and Processing, vol.27,no.4, 2012, pp:474-479

Table 1.
Spectra were recorded in transmittance mode (T) in the range 4000 cm-1 and 654 cm-1. 3.
Spectra were recorded in transmittance (T) mode in the range 4000 cm-1 and 654 cm-1 Fig.6.
For the bands located around 936 cm-1, 892 cm-1 and 877 cm-1 of new catalyst are coincident with the 30% doped catalyst are respectively Si-O-V, V-O-S vibration and the other to the V-O-V group antisymmetric elongation vibration [15]. 3.5.
Catal Today 1999, 51, 469–479

The left chart in Fig. 1 is the new-type continuous air-cooling transformation curves[1] of 25 MnCrNiMo type structural steel.
Fig.1.
Fig. 2, 3 and 4 are established based on air-cooling diameters (see Fig. 1).
The oil and water-cooling diameters of X-coordinate in Fig.1 can be called equivalent diameters.
Reference [1] Zou Qinghua, Sheng-zhong Zou, Key program for non-equilibrium phase diagram of Ni 1 type steel, Advanced Materials Research, 2011 International conference on industry, information system and material engineering, IISME2011, Guangzhou, China, April 16- 17, 204-210, (2011) 1357-1361 [2] QH Zou, CB Wang, G Wu, ZG Wang, SZ Zou, New type dynamic phase diagram of the N1 structural steel, The physics of metals and metallography[J].2008,105 (6):622-629.204-210, (2011) 1357-1361 [3] Z.Qing-Hua, C Hong, C Xiao-Dao, New-type dynamical phase diagrams and a nonequilibrium-lever rule for carbon steels[J].The physics of metals and metallography, 2005,100 (5):472-479.

Shim 1,a, Y.
Guo 1,b, H.
Gu 1,c, X.
(a) (b) Quasi-static, 0.001s-1 Dynamic, 200-300s-1 Dynamic, 200-300s-1 Quasi-static, 0.001s-1 Figure 7.
References [1] Y.

Schikorra 1, a, L.
Results The complete list of experimental results is shown in table 1.
The difference between these two and geometry 1 and 4 is extreme.
Geometry 4 with the symmetric pocket led to a profile with 3870 mm length (vavarage,4 = 7.68 mm/s) and geometry 1 with the asymmetric pockets led to a profile length of 2870 mm (vavarage,1 = 5.7 mm/s).
References [1] P.

Quartz glass (15 × 10 × 1 mm) and commercially pure Ti (CP-Ti) (10 × 10 × 1 mm) were used as substrate.
The Rdep increased with increasing Tsub, and showed a maximum value of 1.25 × 10-8 m s-1 for Ca-Ti-O films and 6.0 × 10-9 m s-1 for Ca-P-O films at Tsub = 1073 K.
The Ea of 70 kJ mol-1 for Ca-Ti-O film and 80 kJ mol-1 for Ca-P-O film in the present study can also suggest a chemical reaction limited process in the low Tsub region [11].
References [1] A.
Forum, 475-479 (2005)1219-1222

A ball-to-powder weight ratio of about 15:1 was chosen.
(heating rate of 40 K/min) Fig. 1 XRD patterns of La55Al25Cu10Ni5Co5 alloy after milling for different times.
Ball Milling 477±1 553±1 76±1 3.61±0.17 this work Melt-spun 471 552 81 4.01±0.02 20 Water-quenching(φ 4 mm rod) 482 565 83 3.85 21 Figure 6(a)-(d) illustrates the DSC scans of the ball-milled composites with different W contents.
Table 2 Data of Tg, Tx and ΔTx for the ball-milled W-containing composites with different W contents (with a heating rate of 40 K/min) W content (vol.%) Tg [K] Tx [K] ∆ Tx [K] 0 477±1 553±1 76±1 10 479±1 555±1 76±1 20 489±1 570±1 81±1 30 506±1 598±1 92±1 The findings that the addition of W particles yields a change in the thermal stability or crystallization behavior for the La-based glassy alloy as the composite matrix suggest that a small amount of W disolves in the glassy matrix, then changing its overall composition.
References [1] W.L.

Table 1 Desired properties of PCMs.
References [1] R.
Sust. 15(1) (2011). 24-46
Buildings. 70, (2014) 472-479
Nanosci. 13(1) (2018) 188-198

Figure 1.
As can be seen in Table 1, the theoretical values agree well with the experiments.
Table 1.
References [1] F.
Awschalom, Nature 479 (2011) 84