Carbon Nanotubes Episode 3 pptx
Báo cáo hóa học: " Carbon Nanotubes for Supercapacitor" pptx
... on carbox- ylated carbon nanotubes by preventing agglomeration among RuO 2 nanoparticles through bond formation between the RuO 2 and the surface carboxyl groups of the carbon nanotubes [92] or ... graphitized carbon layers, where the mesopore volume for the diffusion of ions and the active surface for the formation of the electrical double layer are very limited in this materia...
Ngày tải lên: 22/06/2014, 00:20
Chemistry of Carbon Nanotubes phần 3 potx
... AgCl x Br y , 38 9a CdI 2 and ThCl 4 , 39 6 CdCl 2 , 39 6 ,39 7a TbCl 3 , 39 7a TiCl and PbI 2 , 39 7b CoI 2 , 39 8 LaCl 3 and LaI 3 , 39 9 KI, 38 9d ,39 7a,400 ZrCl 4 , 401 AgCl x I 1-x , 402 BaI 2 , 4 03 and MoCl 5 and ... et al. 38 4a Other ex- amples of metallofullerenes inside nanotubes include Gd@C 82 , 37 7b,c Sm@C 82 , 38 4b Dy@C 82 , 38 4c Ti 2 @C 80 , 38 4d G...
Ngày tải lên: 06/08/2014, 13:22
Orr, F. M. - Theory of Gas Injection Processes Episode 3 pptx
... 1/component 3 side of the diagram (CO 2 /C 10 ), x 12 = 1 − K 3 K 1 −K 3 ,x 11 = K 1 1 − K 3 K 1 − K 3 . (3. 5.5) For four–component systems, Eqs. 3. 5 .3 and 3. 5.4 indicate that the surfaces of vapor ... [18]. Otherwise Table 3. 2 reports values of δ ij recommended by Peng and Robinson [99]. Eqs. 3. 3.7 3. 3.16 provide the description of volumetric behavior needed...
Ngày tải lên: 12/08/2014, 16:21
Proakis J. (2002) Communication Systems Engineering - Solutions Manual (299s) Episode 3 pptx
... f 0 =3. -1 -0 .8 -0 .6 -0 .4 -0 .2 0 0.2 0.4 0.6 0.8 1 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 -1 -0 .8 -0 .6 -0 .4 -0 .2 0 0.2 0.4 0.6 0.8 1 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 -1 -0 .8 -0 .6 -0 .4 -0 .2 0 0.2 0.4 0.6 0.8 0 0.2 ... f c − 30 00) + δ(f − f c + 30 00) +δ(f + f c − 30 00) + δ(f + f c + 30 00)] The next figure depicts the spectrum...
Ngày tải lên: 12/08/2014, 16:21
RADIATION PROTECTION MANUAL Episode 3 pptx
... 2.12E+02 Kidneys 5.77E+01 Thyroid 5.99E+01 Liver 1.23E+02 Uterus 1.70E+01 H = 1 .33 E+02 H = 2.19E+02 rem,50 E,50 ICRP 30 ALI = 30 àCi EM 38 5-1-80 30 May 97 3- 13 of the rem is essentially equal to that ... = 10 àCi x 4.99E+01 mrem/àCi x 0. 03 = 14.97 mrem Marrow = 10 àCi x 6 .36 E+01 mrem/àCi x 0.12 = 76 .32 mrem Remainder = 10 àCi x 1 .33 E+02 mrem/àCi x 0 .30 = 39 9.00...
Ngày tải lên: 12/08/2014, 16:21
Mechanical Movement Episode 3 pptx
... class="bi x0 y0 w1 h9" alt=""
Ngày tải lên: 13/08/2014, 05:22
Advanced mechanics of materials (1993-John Willey) Episode 3 pptx
Ngày tải lên: 13/08/2014, 08:21
Branched Polymers I Episode 3 pptx
... disproportionation or for the chain transfer to small mol- ecules. In this respect, any living polymerization with rapid initiation will afford polymers with a narrow DP distribution of the Poisson ... end-capping of a living polymer (termination method), (b) initiation of living polymeriza- tion (initiation method), (c) transformation of any functional end-group, and (d) polyaddition. Meth...
Ngày tải lên: 13/08/2014, 08:21
Branched Polymers II Episode 3 pptx
... . . . . 132 3. 2.5 The Second Virial Coefficient A 2 . . . . . . . . . . . . . . . . . . . . . 134 3. 3 Synopsis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 136 4 Molar ... y lin T g T g R R or R R * . .== = =0 26 0 752 0 34 57 0 701 3 3 3 Solution Properties of Branched Macromolecules 151 spectively. However, when applying Eq. (38 b) to the exponents, fo...
Ngày tải lên: 13/08/2014, 08:21
Engineering Mathematics 4 Episode 3 pptx
... x 2 C 4x C 1 D 0[ 3. 732 , 0.268] 2. 2x 2 C 5x 4 D 0[ 3. 137 , 0. 637 ] 3. 3x 2 x 5 D 0 [1 .46 8, 1. 135 ] 4. 5x 2 8x C 2 D 0 [1.290, 0 .31 0] 5. 4x 2 11x C 3 D 0 [2 .44 3, 0 .30 7] 11 .4 Solution of ... 5.2 932 (b) ln 82 .47 3 4. 829 (c) 5.62 ln 32 1.62 e 1.2 942 [(a) 0.277 74 (b) 0.9 13 74 (c) 8.8 941 ] 5. (a) 2. 946 ln e 1.76 lg 10 1 .41 (b) 5e 0.1629 2ln0.001...
Ngày tải lên: 13/08/2014, 08:21
Kinematic Geometry of Surface Machinin Episode 3 pptx
... 0 V ω 1 ω 2 ω 1 ω 2 ω 2 ω 1 ω 4 −ω 4 +ω 4 +ω ω 1 2 ω 4 −ω 1 ω 2 ω 1 ω 2 ω 2 ω 1 ω 1 ω 2 ω 3 ω 2 ω 1 ω 3 ω 2 ω 1 ω 2 ω 1 ω 2 ω 1 ω 3 ω ω V 3 31 =3 13 3 32 =3 23 3 41 =3 14 3 42 =3 24 3 43 =3 34 3 34 : ω 4 = 0 3 35 : V 1–2 = 0 V 1–2 V 1–2 3 45 : V 1–2 = 0 ω 1 ... 0 3 21 =3 12 3 41 =3 14 3 42 =3 24 3 43 =3 34 3 43 =3 34 3 23 : ω 3 =...
Ngày tải lên: 13/08/2014, 09:20
Carbon Nanotubes Episode 3 pptx
... tm21 0.5 630 0.071 0.068 5 5 1- - t12SI 0.6050 0.067 0.064 a 11~41 0. 537 0 0.076 0.0 73 'CI 0.4170 0. 133 0. 130 VSl [921 0.4060 0.140 I 431 0.2460 0 .36 6 0 .35 4 0. 137 ' ... (London) 36 3, 605 (19 93) . 5. S. Iijima and T. Ichihashi, Nature (London) 36 3, 6 03 (19 93) . 6. M. S. Dresselhaus, G. Dresselhaus, and R. Saito, Phys. Rev. B...
Ngày tải lên: 13/08/2014, 15:21
Carbon Nanotubes Episode 10 pptx
... 111 cage forms 77 cahon fibers 87 carbon nanotubes see nanotubes; pyrolitic carbon carbon- carbon intralayer distance 59 catalysis vapo-grown 1 nanotubes growth mechanism 87 nanotubule ... particles 163 open tips 11 PCNTs see pyrolyk carbon nanotubes pitch angle 59 pyrolitic carbon nanotubes (PCNTs) hemi-toroidal networks 105 vapor grown 1 Raman sca...
Ngày tải lên: 13/08/2014, 15:21
Science Technology Carbon Nanotubes Episode 3 ppsx
... distance between atoms. @-Excitation 260 280 30 0 32 0 34 0 36 0 Energy Loss (ev) b)Diamond 1 @-Excitation 260 280 30 0 32 0 34 0 36 0 Energy Loss (ev) Fig. 4. EEL spectra ... Ichihashi, T., Nature, 19 93, 36 3, 6 03. Dravid, V. P., Lin, X., Wang, Y., Wang, X. K., Yee, A., Ketterson, J. B. and Chang, R. P. H., Science, 19 93, 259, 1601. Wan...
Ngày tải lên: 13/08/2014, 17:20