$B9V1i(B $B;~9o(B | $B9V1i(B $BHV9f(B | $B9V1iBjL\!?H/I=$B%-!<%o!<%I(B | $BJ,N`(B $BHV9f(B | $B$BHV9f(B | |
$B%7%s%]%8%&%`(B $B!cG.9)3X%7%s%]%8%&%`!d(B |
(9:00$B!A(B10:40)$B!!(B($B:BD9(B $B;3K\(B $B9d(B) |
9:00$B!A(B 9:20 | F101 | $BH?1~G.NL7W$rMQ$$$?(BLiBr$B?eMO1U$NHfG.(B ($BH,8M9)Bg(B) $B!{(B($B3X(B)$BLnKY(B $B@2$B!&(B($B@5(B)$B9b66(B $B?8(B$B!&(B$BGr@P(B $BBY(B$B!&(B($B@5(B)$BLnED(B $B1QI'(B | absorption refrigeration working liquid specific heat
| S-14 | 800 |
9:20$B!A(B 9:40 | F102 | $B>uBVJ}Dx<0$K$h$k%U%l%*%s:.9gNdG^$N@_7W(B ($BK!@/Bg1!(B) $B!{(B($B3X(B)$B9uLZ(B $BM}Bg(B$B!&(B($BK!@/Bg(B) ($B@5(B)$B@>3$(B $B1QM:(B | EoS C.O.P refrigerant
| S-14 | 808 |
9:40$B!A(B 10:00 | F103 | 2$B?'(BLIF$B$N51EYI>2A$K$h$k1UAjFb29EY>l7WB,(B ($BIY;3Bg9)(B) ($B@5(B)$B;3:,(B $B3Y;V(B$B!&(B$B!{NkLZ(B $BD>$B!&(B$BIYED(B $BM4B$(B$B!&(B($B@5(B)$B5HED(B $B@5F;(B | Temperature measurement Laser Induced Fluorescence Visualization
| S-14 | 436 |
10:00$B!A(B 10:20 | F104 | $B?M9)GYMQG.8r494o$K$*$1$kFsAjN.$H?6F0$N8z2L(B ($B@EBg(B) $B!{(B($B3X(B)$B5WJ];3(B $B>4Li(B$B!&(B($B@5(B)$BLZB<(B $B85I'(B$B!&(B($B@5(B)$BBg66(B $BOB5A(B | heat exchanger vibration two phase flow
| S-14 | 914 |
10:20$B!A(B 10:40 | F105 | $B%^%$%/%mGH>Hl$K$*$1$k%J%NIC;~4VJ,2r7V8w0[J}@-$NB,Dj(B ($BL>Bg1!9)(B) $B?$B!&(B($B6bBtBg<+A38&(B) $B1JC+(B $B=(B@O:(B$B!&(B$B>.@>(B $B0&(B$B!&(B$B!{Hf9>Eh(B $BM42p(B$B!&(B($B@5(B)$B9b66(B $B7{;J(B | microwave anisotropy
| S-14 | 870 |
(10:40$B!A(B12:00)$B!!(B($B:BD9(B $B0$AIC+Mx8w(B) |
10:40$B!A(B 11:00 | F106 | W/O$BF}2=G3NAE)$N%_%/%mGzH/5sF0$K5Z$\$92CG.>r7o$N1F6A(B ($B9bCN9)Bg(B) $B!{(B($B3X(B)$B>>2,(B $B98(B$B!&(B($B3X(B)$BKLB<(B $BM4$B!&(B$Bc7F#(B $BM5?M(B$B!&(B$B@P86(B $B?5(B$B!&(B($B@5(B)$BN>3Q(B $B?NIW(B$B!&(B($B%(%L%(%U%8!<(B) $BK\4V(B $B5AO/(B | W/O emulsified fuel micro explosion heating condition
| S-14 | 699 |
11:00$B!A(B 11:20 | F107 | $BG3NA2aG;>r7o$K$*$1$k(BDME$BItJ,M=:.9gG3>F$K4X$9$k8&5f(B ($BL>Bg9)(B) $B!{(B($B3X(B)$B2Li(B$B!&(B($B3X(B)$BKYED(B $B9@?-(B$B!&(B($BL>Bg%(%3%H%T%"(B) ($B@5(B)$BKQ(B $B3$MN(B$B!&(B($B6&(B)$B5WJ](B $B5.(B$B!&(B($B@5(B)$B>.Eg(B $B5A90(B$B!&(B($B6&(B)$BD9C+@n(B $BK-(B$B!&(B($B@5(B)$BKL@n(B $BK.9T(B | DME Fuel-rich combustion Gas turbine
| S-14 | 900 |
11:20$B!A(B 11:40 | F108 | $B%a%?%s;@AGIY2=3H;6G3>F$K$*$1$k(BNO$B!"(BNO2$B$N@8@.NL$H;@AGG;EY$H$NAj4X(B ($B0&9)Bg9)(B) $B!{(B($B3X(B)$Bc7F#(B $B>4(B$B!&(B($BL>Bg(B) ($B@5(B)$B>.NS(B $B7I9,(B$B!&(B($B0&9)Bg9)(B) ($B@5(B)$B2MC+(B $B>;?.(B | Oxygen Combustion NOx
| S-14 | 185 |
11:40$B!A(B 12:00 | F109 | $B%@%V%k%W%m!<%VK!$K$h$kBg5$05;@AGG3>F%W%i%:%^$NEE;RJ*@-I>2A(B ($BL>Bg1!9)(B) $B!{(B($B3X(B)$BBg:d(B $BPR8c(B$B!&(B($BL>Bg%(%3%H%T%"(B) ($B@5(B)$B>.NS(B $B7I9,(B$B!&(B$BBgLn(B $BE/Lw(B$B!&(B($B0&9)Bg9)(B) $B9bB<(B $B=(0l(B$B!&(B($B6bBtBg<+A3(B) $BEDCf(B $B9/5,(B$B!&(B$B>e?y(B $B4nI'(B | oxy-combustion atmospheric pressure plasma RF inductive heat
| S-14 | 138 |
(13:00$B!A(B14:20)$B!!(B($B:BD9(B $B2,LnBYB'(B) |
13:00$B!A(B 13:20 | F113 | $B%,%92=H?1~?J9TCf$K$*$1$kHy;k9=B$$r9MN8$7$?%3!<%/%9?tCM:`NA;n83(B ($BElKLBg1!9)(B) $B!{(B($B3X(B)$B>e2,(B $B7rB@(B$B!&(B($B3X(B)$BNS:j(B $B=(9,(B$B!&(B($B@5(B)$B>>2<(B $BMN2p(B$B!&(B($B@5(B)$B@DLZ(B $B=(G7(B$B!&(B($B@5(B)$B;01:(B $BN4Mx(B$B!&(B($B?7F|oD(B) ($B@5(B)$BJ!ED(B $B9L0l(B$B!&(B($B4X@>G.2=3X(B) ($B@5(B)$B>>J?(B $B42;J(B | Multiscale simulation Gasification reaction Coke strength
| S-14 | 583 |
13:20$B!A(B 13:40 | F114 | $B%3!<%/%9O'AuC:2aDx$K$*$1$kH/@8%,%9NL$K4X$9$k?tCM2r@O(B ($BElKLBg1!9)(B) $B!{(B($B3X(B)$B8FOB(B $BEsNO(B$B!&(B($B@5(B)$B>>2<(B $BMN2p(B$B!&(B($B@5(B)$B@DLZ(B $B=(G7(B$B!&(B($B@5(B)$B;01:(B $BN4Mx(B | coal charge gas yield numerical analysis
| S-14 | 608 |
13:40$B!A(B 14:00 | F115 | $BD6NW3&Fs;@2=C:AG$rMQ$$$?G.%5%$%U%)%sFb$NEAG.FC@-(B ($B;37ABg1!M}9)(B) $B!{(B($B3X(B)$BBgM'(B $BM%(B$B!&(B($B;37ABg9)(B) ($B@5(B)$BLg3p(B $B=($B!&(B($B@5(B)$B86ED(B $B1QFs(B$B!&(B($B@5(B)$B7*;3(B $B2mJ8(B | Supercritical Carbon Dioxide
| S-14 | 100 |
14:00$B!A(B 14:20 | F116 | $B%U%m!<7?%^%$%/%mGH2=3XH?1~AuCV$N3+H/(B ($B%^%$%/%m2=3X%W%m%;%9(B) $B!{(B($B@5(B)$B>>_7(B $B8w9((B$B!&(B($BF|N)5!3#8&(B) ($B@5(B)$BIY3_(B $B@9E5(B$B!&(B($B5~Bg9)(B) ($B@5(B)$BD9C+It(B $B?-<#(B | Microwave Flow processing Chemical reactor
| S-14 | 675 |
(14:20$B!A(B15:40)$B!!(B($B:BD9(B $B>>2 |
14:20$B!A(B 14:40 | F117 | $BD6C;%Q%k%9%l!<%6!<$N%9%]%C%H>H ($B5~Bg9)(B) $B!{(B($B3X(B)$B9b;3(B $B1Q=S(B$B!&(B($B@5(B)$B4];3(B $BIRO/(B | heat conduction ultrashort laser laser processing
| S-14 | 644 |
14:40$B!A(B 15:00 | F118 | $B%/%i%C%AMQ<><0%Z!<%Q! ($B%(%U!&%7!-IR(B$B!&(B$B86(B $B9@$B!&(B$B:4!9LZ(B $BG&(B$B!&(B$B1|0f(B $B0lG7(B$B!&(B($B@EBg(B) ($B3X(B)$B@DLZ(B $BM&M4(B$B!&(B($B@EBgAO2J1!(B) ($B@5(B)$B2,Ln(B $BBYB'(B | Simulation heat transfer wet clutch
| S-14 | 577 |
15:00$B!A(B 15:20 | F119 | $BH>5eMF4oFb<+A3BPN.$N<'>l0u2C8z2L(B ($B6eBg9)(B) $B!{(B($B@5(B)$B6bED(B $B>;G7(B$B!&(B($B$B!&(B($B;37ABg9)(B) ($B@5(B)$B@V>>(B $B@5?M(B$B!&(B($B6eBg9)(B) ($B@5(B)$B?<0f(B $B=a(B | Magnetizing force natural convection hemisphere
| S-14 | 860 |
15:20$B!A(B 15:40 | F120 | FZ$BFb29EY:9!&G;EY:9%^%i%s%4%KBPN.$K4X$9$k(B3$B ($B@EBg1!(B) $B!{(B($B3X(B)$BJ?ED(B $BK.9I(B$B!&(B($B@EBg9)(B) $B@PED(B $BFX;R(B$B!&(B($B@EBgAO2J1!(B) ($B@5(B)$B2,Ln(B $BBYB'(B | Numerical simulation Marangoni convection Floating-zone method
| S-14 | 556 |
(16:00$B!A(B16:40)$B!!(B($B:BD9(B $B>.NS7I9,(B) |
16:00$B!A(B 16:20 | F122 | $BIwGH5$1U3&LL$rDL$7$F$NG.M"AwNL$NI>2A(B ($B5~Bg1!(B) $B!{(B($B3X(B)$BBgDZ(B $B<~J?(B$B!&(B$BH>ED(B $BOBBg(B$B!&(B($B5~Bg9)(B) ($B@5(B)$B>.?9(B $B8g(B | Heat Transfer Shear Flow Air-Water Interface
| S-14 | 884 |
16:20$B!A(B 16:40 | F123 | $BHyJ4C:G3>F>l$K$*$1$kmU ($B=P8w%(%s%8%K%"%j%s%0(B) $B!{(B($B@5(B)$B0$AIC+(B $BMx8w(B$B!&(B($B=P8w6=;:(B) ($B@5(B)$B;32<(B $B5|(B$B!&(B($BG3>FN.BN8&(B) ($B@5(B)$BIY1J(B $B9@>O(B$B!&(B($BL>Bg1!(B) ($B@5(B)$BHDC+(B $B5A5*(B$B!&(B($BL>BgL>M@65!(B | coal-combustion radiation simulation
| S-14 | 75 |
(16:40$B!A(B17:40)$B!!(B($B;J2q(B $BHDC+5A5*(BE$BCf@nFsI'(BE$B?<0f(B $B=a(B) |
16:40$B!A(B 17:40 | _ |