Search results

The gray wall emissivity, the absorption coefficient of the medium is set to 1 m-1, both boundary and medium temperatures are set to 1000K.
Inverse results at different positions using SPSO have been shown in table 1.
Fig.1.
Heat Transfer, 7, 479–486, 1993
Radiative Transfer, 87, 1–14, 2004

Fig. 1 Magnetic domain structure schematic of short glass-coated amorphous alloy microwire.
The simulated result for the 1 mm microwires shows a very low permeability and resonance values.
References [1] R.
Phys. 42 (2009) 095004(1-3)
Phys. 74 (1993) 475-479.

A Sensor Network Flooding Routing Algorithm Based on Sector Area Nodes Selection Kaiguo Qian 1,a, Ming Ni 1,b，Zucheng Dai 1,c 1 Department of Physics Science and Technology,Kunming university, 650031 China aqiankaiguo@qq.com, bLiming@qq.com, c dzcheng88@126.com Keywords: Sensor Network; Routing Algorithm; Sector Area: energy consumption Abstract.
Radio Energy Model.We take the same Radio Energy Model that stated in paper [4], the energy dissipation as shown equation 1
(1) Equation 1 Energy Dissipation Equation for k-bit message and receive k -bit message the energy dissipation as shown equation 2.
References [1] L.F.Akyildiz, W.L.Su, Y.Sankarasubramaniam, E.
IEEE/ACM Transactions on Networking (TON) archive Volume 14 Issue 3, June 2006 ,Pages 479 - 491 [5] J.Kulik,W.Rabiner,H.Balakrishnan.

The value of the coefficient C can change in the range from 1 to 0.
For T pattern dimensions 30x30 points the computation speed achieved was ten times faster (Fig.1 - “GPU”).
Fig.1.
References [1] D.
Chu, Measurement of whole-field surface displacements and strain using a genetic algorithm based intelligent image correlation method, Journal of Dynamic Systems, Measurement, and Control, v. 126, 3 (2004) 479-488

[1-3].
All the tests were carried out at an initial strain rate of 1.0 × 10 −3 S−1.
Figure 1.
References [1] H.
Forum Vol. 475-479 (2005), p. 537

The control flow and the overall assembly structure are in Fig.1 and Fig.2 Fig.1.
The overall assembly structure (1: Base , 2: Motor 1 , 3: Transducer , 4: Guide pin , 5: Linking piece , 6: Motor 2 , 7: Thread rod, 8: Support board , 9: Motor 3) Piezoelectric transducers set piezoelectric effect and converse piezoelectric effect at a suit, the assembly process of piezoelectric transducers is the realization process of piezoelectric effect and piezoelectric transducers used process is to realize the process of converse piezoelectric effect.
Motor 1 adopts open-loop control.
Receive and send program SCM is as follows: void rs_dmx() interrupt 4 using 2// Interrupt service routines of Serial { if( RI == 1) { Flag_Com = 1 ;//Setting marks b=SBUF ;//receive datas RX_buf[ RX_count ] = b; SBUF= RX_buf[ RX_count ];// returning the datas to the PC RX_count++; RI=0; } } When starting SCM, the system will enter the main program.
Engineering practice of SCM application [5] Lan Jing, HaiJun Zhu, ShuoCheng Zhang, etc.The design of control for stepper motor and its application [6].journal of nuclear technology, 2005,28 (6) : 479-482.

The schematic polishing process is shown in Fig.1.
The process under various temperatures in Table 1 as: 1.
Table 1.
References [1] J.
Zhang: Journal of Alloys and Compounds Vol. 479 (2009), p.

In 1981, Raibert and Craig[1] brought forward the hybrid movement–force control policy and provided the best way for a robot in free-form surfaces polishing.
Table 1 Structure and performances of the stepper motor Step angle Step Minimal thrust Wring Operation voltage Current /phrase Resistance /phrase Inductance /phrase 1.8o 0.0508mm 8kg at 1000pps Double polarity 5V 1.3A 3.85Ω 16.4mH Power consumption Temperature rise Insulation resistance Rotor inertia Weight Operating temperature Storage condition Other 13W 75oC 20MΩ 166gcm2 511g -40 oC~+55 oC -40 oC ~+100 oC The performance of a PID controller lies on the initialized values of , and .
(1)A passive wrist system is developed to make the grinding ring adapt the curved surface.
References [1] T.
De Gersem: Advanced Robotics, Vol.19 (20055)No.5, pp. 479-499 [2] R.S.

Caries Inhibitory Activity of the Nano-HA in Vitro Xiangcai MENG 1, a , Kuilong LV 1, 2, b , Jiuxing ZHANG 2 , Dali QU 1 1.The Key Laboratory of Advanced Functional Materials, Ministry of Education, Beijing University of Technology, Beijing 100022, China. 2.
The SEM photographs of the biofilms under the different conditions in 72 hours are shown in the Fig.1.
It shows that the biofilms are very thick and there are a mass of extra-cellular polysaccharide with the pulsing of sucrose solution, as shown in Fig.1 (b); with former contrast, the biofilms are thin and there are less of extra-cellular polysaccharide with the pulsing of mixed HA, spherical HA and fluorine sodium solution, as shown in Fig.1 (e), (f) and (g); the biofilms are between them with the pulsing of sol HA and prism HA solution, as shown in Fig.1(c) and (d).
Bacterial colonization can be simplified to two basic mechanisms: (1) direct: bacterial-oral surface interaction; (2) indirect: bacterial-bacterial interaction [9].
Lu: Materials Science Forum Vol.475-479 (2005), p. 2423 [5] T.

Photoluminescence of 10H-SiC Anne Henry1,a, Hiroshi Yano2,3,b and Tomoaki Hatayama2,c 1 Department of Physics, Chemistry and Biology, Linköping University, Sweden 2 Graduate School of Materials Science, Nara Institute of Science and Technology, 8916-5 Takayama, Ikoma, Nara 630-0192, Japan 3 present address: Graduate School of Pure and Applied Sciences, University of Tsukuba,11-1 Tennodai, Tsukuba, Ibaraki 305-8573, Japan a anhen@ifm.liu.se, b yano.hiroshi.fn@u.tsukuba.ac.jp and c phi3ic3@bma.biglobe.ne.jp Keywords: 10H-SiC, photoluminescence, excitonic band gap, ionization.
Fig.1: a) Selected area diffraction pattern observed from the substrate and b) atomic structure of 10H-SiC b) Characterization procedure.
At room temperature in the backscattering geometry using the 514.5nm line of an Ar+ laser focused in a 10 μm diameter spot as an excitation source and with a resolution of 1 cm-1 the Raman spectroscopy (not shown here) revealed four peaks in the range from 760 to 800cm-1 in agreement with the literature and associated to the transverse optical (TO) mode (for detail and comparison with other polytypes please see for detail ref [3]).
Phonon replicas of the N-BE lines are observed at lower energies with energy separation between them and the Px0 and Qx0 lines, very close to the phonon energies observed in other polytypes [1,2].
Forum 778-780 (2014) 479