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ENERGY SAVING USING HEAT EXCHANGERS
COVERED WITH POROUS COATINGS
A b s t r a c t
([SORLWDWLRQRIWHFKQLFDOGHYLFHVLVDOZD\VUHODWHGWRWKHHQHUJ\FRQVXPSWLRQ7KXVLIPRUHHI¿FLHQWKHDWH[FKDQJHUVDUH used as part of mechanical systems, it is possible to save energy. The paper presents possible ways of producing more HI¿FLHQWKHDWWUDQVIHUVXUIDFHVZRUNLQJXQGHUWKHQXFOHDWHERLOLQJPRGH:KHQSRURXVFRYHULQJVDUHXVHGVLJQL¿FDQW UHGXFWLRQRIWHPSHUDWXUHGLIIHUHQFHVLVQRWLFHGDWWKHVDPHKHDWÀX[,WOHDGVWRKLJKHUHQHUJ\HI¿FLHQF\
Keywords: boiling, porous coatings
1. Introduction
In thermodynamic cycle the temperature differences between the evaporator section and the heat source, and between the condenser and the heat sink, are VRXUFHVRILUUHYHUVLELOLW\7RREWDLQKLJKFRHI¿FLHQWVRI performance, the temperature differences need to be as VPDOODVSRVVLEOH)RUH[DPSOHLQDUHIULJHUDWLRQV\VWHP WKHUHGXFWLRQLQWHPSHUDWXUHGLIIHUHQFHIURPoC to
oC results in the reduction of required work by about
>@7KDWOHDGVWRHQHUJ\VDYLQJ6XFKDUHGXFWLRQ LQWHPSHUDWXUHGLIIHUHQFHVLQKHDWH[FKDQJHUVFDQEH achieved due to introduction of porous coverings on the surfaces. In boiling, they might dissipate the same heat ÀX[DVVPRRWKVXUIDFHVEXWDWVLJQL¿FDQWO\ORZHUHG temperature differences. Such microstructures might be used in many industrial applications – in refrigeration, chemical engineering. Orman discussed their possible DSSOLFDWLRQ LQ DXWRPRWLYH KHDW H[FKDQJHUV >@ RU LQ heating and ventilation systems [8].
2. Boiling heat transfer augmentation
7KHKHDWHUVXUIDFHFDQEHPRGL¿HGZLWKURXJKQHVV or the application of microstructures of different JHRPHWU\0HFKDQLFDOPL[LQJRIWKHÀXLGRULQGXFLQJ vibrations is also possible [1, 2]. Microstructures can be produced on the heater surface by deposition or by mechanical means. There are many kinds of such VWUXFWXUHV>@7KHLUDSSOLFDWLRQPLJKWOHDGWRD VLJQL¿FDQWHQKDQFHPHQWRIKHDWWUDQVIHU
=KDQJDQG=KDR>@GLVFRYHUHGWKDWERLOLQJKHDW WUDQVIHU FRHI¿FLHQWV IRU WKH VXUIDFHV ZLWK SRURXV coatings produced with the thermal spraying
WHFKQLTXH ZHUH ± WLPHV KLJKHU WKDQ IRU WKH VPRRWKVXUIDFH±WKHFRYHULQJVRIPPPP DQGPPKHLJKWZHUHXVHG=KDQJDQG&KHQ>@ investigated water and ethanol boiling on a horizontal surface covered with porous layer of sintered bronze SRZGHU 0LFURVWUXFWXUH KHLJKW ZDV ± PP ZKLOHWKHJUDLQGLDPHWHUUDQJHGIURP±PP +HDWWUDQVIHUFRHI¿FLHQWRIVXFKDVXUIDFHZDVWR 10 times higher than of the smooth surface. For the VDPH KHDW ÀX[ WKH WHPSHUDWXUH GLIIHUHQFH ZLWK WKH XVHRISRURXVOD\HUVZDVPXFKORZHU)RUH[DPSOH ZDWHUWHVWUHVXOWVLQGLFDWHGWKDWIRUKHDWÀX[RI W/cm2 the required temperature difference for the
VPRRWKVXUIDFHZDVDERXW.ZKLOHIRUWKHSRURXV FRYHULQJRIPPKHLJKW±DERXW.)RUHWKDQRO DQGWKHVDPHKHDWÀX[WKHWHPSHUDWXUHGLIIHUHQFHIRU the smooth surface amounted to about 16 K while for WKHPLFURVWUXFWXUH±RQO\VRPH.&LHĞOLĔVNL>@ analysed water boiling on horizontal surfaces coated HOHFWURFKHPLFDOO\ZLWKD±PPSRURXVOD\HU of copper, aluminum and silver. The heat transfer FRHI¿FLHQW IRU WKH SRURXV FRDWLQJ WXUQHG RXW WR EH HYHQ WLPHV KLJKHU WKDQ IRU WKH VPRRWK VXUIDFH 5DLQH\DQG<RX>@H[SHULPHQWDOO\DQDO\VHG)& ÀXRULQHUW±DGLHOHFWULFÀXLGERLOLQJRQWKHFRSSHU [PPVXUIDFHFRYHUHGZLWKPPZLGHVTXDUH SLQ±¿QV7KHUHZHUH[SLQVRQWKHVXUIDFHORFDWHG 1 mm apart from each other. The height of the pins ZDVDQGPP)RUWKHVDPHKHDW ÀX[RI:FP2 the temperature difference required
IRUWKHVPRRWKVXUIDFHZDVDERXW.ZKLOHIRUWKH PLFUR±¿QQHGVXUIDFHDERXW.
Another type of microstructural coatings are PHWDO ¿EURXV SRURXV VWUXFWXUHV 7KH FRQVLGHUDEOH LQFUHDVHLQKHDWWUDQVIHUFRHI¿FLHQWGXHWRDWWDFKPHQW WR WKH VXUIDFH RI WKH KHDW H[FKDQJHU PHWDO ¿EURXV porous structures was reported by Wójcik in [19]. +H SUHVHQWHG WKDW WKH KHDW WUDQVIHU FRHI¿FLHQW DPRXQWHGWRā:P2.IRUWKHKHDWÀX[RI
W/m2 ZDWHU SRURVLW\ WKLFNQHVV PP ,Q
the boiling process there is a strong dependence of ERLOLQJ KHDW WUDQVIHU FRHI¿FLHQW IURP WKH VWUXFWXUDO SDUDPHWHUVSRURVLW\WKLFNQHVV7KHPD[LPXPYDOXH RIWKHKHDWWUDQVIHUFRHI¿FLHQWZDVUHFRUGHGZKHQWKH covering was 0.6 – 0.8 mm thick. The heat transfer DXJPHQWDWLRQ IRU VXFK VWUXFWXUHV ZDV FRQ¿UPHG E\ Orzechowski and Orman [10]. Moreover, for the VDPHKHDWÀX[RIDERXWN:P2 the temperature
difference for the smooth surface was 12 K, while for the porous layers 9 K (for water). In the case of the VDPHKHDWÀX[IRUHWKDQROERLOLQJWKHVPRRWKVXUIDFH WHPSHUDWXUHGLIIHUHQFHDPRXQWHGWRDERXW.DQG DERXW.IRUWKHSRURXVVWUXFWXUHV
Quite common are also wire mesh microstructures >@ 7KH GDWD SUHVHQWHG LQ >@ SURYHV WKDW KHDW transfer augmentation is possible with the application of such structures. A coating consisting of three copper mesh layers of wire diameter 0.18 mm and PHVKDSHUWXUHPPZDVXVHG+HDWÀX[IRUWKH mesh structure was even a few times higher than for WKHVPRRWKVXUIDFH)RUWKHKHDWÀX[RIN:P2
the required temperature difference for water boiling KHDWWUDQVIHURQWKHVPRRWKVXUIDFHZDVDERXW. ZKLOHIRUWKHPHVKFRYHULQJ.ZKLOHIRUHWKDQRO DERXW.DQG.IRUVPRRWKDQGSRURXVVXUIDFHV respectively. Orzechowski and Orman [12] also H[SHULPHQWDOO\ DQDO\VHG ERLOLQJ KHDW WUDQVIHU IURP mesh structures consisting of two mesh layers – each from a different material: copper and stainless steel – sintered together on a copper heater surface.
Many techniques can be used to enhance heat transfer. Xiuling et al. [21] studied boiling of nitrogen RQDFRSSHU¿QQHGWXEH7KH¿QV¶KHLJKWZDVPP and an additional porous coating was sintered onto WKH¿QQHGWXEH7KLVFRYHULQJZDVPPKLJKDQG KDGSRURVLW\RI)RUWKHVDPHKHDWÀX[WKHKHDW WUDQVIHU FRHI¿FLHQW RI WKH ¿QQHG VXUIDFH ZLWK WKH coating was 6 – 8 times higher than of the smooth tube. It was also higher than of the tube without the ¿QVDQGRQO\ZLWKWKHSRURXVOD\HU
New methods of heat transfer augmentation are GHYHORSHG 5DGHN DQG 2UPDQ >@ H[SHULPHQWDOO\ analysed electro – spark deposition as a means of
ERLOLQJKHDWWUDQVIHUHQKDQFHPHQW6LJQL¿FDQWYDOXHV RIWKHKHDWWUDQVIHUFRHI¿FLHQWSURYLGHQHZJHQHUDWLRQ coverings investigated by Wójcik et al. [20]. These structures are sintered from copper powder with the DGGLWLRQRIFRSSHUR[LGHSRZGHU
3. Modelling boiling heat transfer for porous coatings Modelling of boiling heat transfer is of practical YDOXH±IRUH[DPSOHLQWKHGHVLJQRIKHDWH[FKDQJHUV One of the models has been proposed by Nishikawa HWDO>@+HDWLVDVVXPHGWREHWUDQVIHUUHGWKURXJK conduction from the heater surface to liquid according WRWKHHTXDWLRQIRUWKHKHDWÀX[
(1) where: G is the height of the porous layer, 'T is the difference between the temperature of the heater surface and the saturation temperature of the liquid (often referred to as wall superheat), Om describes effective thermal conductivity.
Om is calculated as:
(2) where: H is porosity of the microstructure, Ol and Os conductivity values of liquid (l) and structure material (s), respectively.
The value of Om is crucial for the model calculations. ,WXVXDOO\OHDGVWRHOHYDWHGKHDWÀX[HVXVLQJHTXDWLRQ LQFRPSDULVRQWRWKHH[SHULPHQWDOGDWD$FFRUGLQJWR [17] formula (2) describes the effective conductivity of the liquid – solid system if the solid elements are parallel to the heater. In the case of the perpendicular direction the following equation has been proposed in [17]:
0RVW FRYHULQJV ± IRU H[DPSOH PHWDO ¿EHU VWUXFWXUHV KDYH D FRPSOH[ JHRPHWU\ DQG GR QRW VDWLVI\DVVXPSWLRQRIWKHSDUDOOHOVROLGKHDWÀRZ,Q the case of these microstructures another method of thermal conductivity calculation needs to be adopted according to the equation given in [17] as:
7KLV FRQFHSW KDV EHHQ XVHG E\ 2UPDQ >@ WR GHWHUPLQHZLWKWKH¿WWLQJSURFHGXUHWKHFRHI¿FLHQW) IRUFRSSHUPHWDO¿EURXVVWUXFWXUHVZKLFKIRUZDWHU HTXDOOHG )LJXUH SUHVHQWV FRPSDULVRQ RI
WKHH[SHULPHQWDOUHVXOWVRIZDWHUERLOLQJRQDFRSSHU ¿EHU SRURXV VWUXFWXUH RI DQG PP WKLFNQHVV according to data by Wójcik [18] with the calculations performed using the Nishikawa model – original DQG ZLWK D PRGL¿HG FRQGXFWLYLW\ YDOXH DFFRUGLQJ WR HTXDWLRQ DQG ) 7KH UHVXOWV DUH graphically presented as so called “boiling curves” – GHSHQGHQFHVRIKHDWÀX[YVZDOOVXSHUKHDW )LJ%RLOLQJFXUYHVIRUZDWHUIRUWKHFRSSHU¿EURXV VWUXFWXUH±H[SHULPHQWDOGDWD>@±FDOFXODWLRQVZLWK WKHRULJLQDO1LVKLNDZDPRGHO±FDOFXODWLRQVZLWKWKH PRGL¿HG1LVKLNDZDPRGHOZLWK) ±FDOFXODWLRQVZLWKWKHQHZ)YDOXHRI 7KHFDOFXODWHGKHDWÀX[YDOXHVEDVHGRQWKHRULJLQDO 1LVKLNDZDPRGHODQGWKHPRGHOPRGL¿HGE\2UPDQ >@ ZLWK D GLIIHUHQW HIIHFWLYH WKHUPDO FRQGXFWLYLW\ YDOXH FXUYHV DQG UHVSHFWLYHO\ RYHUSUHGLFW WKH H[SHULPHQWDO GDWD ,Q >@ WKH FRHI¿FLHQW YDOXH RI ZDV GHWHUPLQHG IRU D SRURXV VWUXFWXUH RI SRURVLW\ DQG WKLFNQHVV PP ,Q >@ WKH geometrical parameters of the coating are different. Consequently, a different value of F should be H[SHFWHG+DYLQJFRQVLGHUHGWKLVFDOFXODWLRQVKDYH been preformed to determine a new value of F for the analysed microstructure. It has been calculated as 7KHUHVXOWVDUHSUHVHQWHGDVWKHFXUYH1R DQGDUHDOPRVWLGHQWLFDOZLWKWKHH[SHULPHQWDOGDWD 4. Discussion
$OWKRXJK SRURXV FRDWLQJV RIIHU VLJQL¿FDQW possibilities in heat transfer enhancement and reduce WKHWHPSHUDWXUHGLIIHUHQFHIRUWKHVDPHKHDWÀX[WKH knowledge of the physical processes inside porous VWUXFWXUHVLVVWLOOLQVXI¿FLHQW&RQVHTXHQWO\WKHUHDUH FRQVLGHUDEOHGLI¿FXOWLHVLQFUHDWLQJDPRGHOWRSUHGLFW
KHDWÀX[RUKHDWWUDQVIHUFRHI¿FLHQWEDVHGRQSK\VLFDO and chemical properties of the microstructure. In the case of smooth surfaces more is known. In [6] the discussion of this issue is presented.
)RU SRURXV OD\HUV GXH WR WKH FRPSOH[LW\ RI WKH structures and different production methods, it is YHU\GLI¿FXOWWRSURSRVHDVDWLVIDFWRU\FRUUHODWLRQRU a model. However, the concept presented here (based RQPRGL¿HG1LVKLNDZDPRGHOPLJKWEHLQWHUHVWLQJ to consider. A method of calculating the F value, which seems to be related to the structural properties of the porous covering, could be a new approach. 7KDWPLJKWEHIXUWKHUGHYHORSHGERWKH[SHULPHQWDOO\ and theoretically.
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4. Dyskusja
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