⟶እࡢẼࡢ⇕ఏ㐩ಀᩘhw2 ࡣࠊWilkeࡢ᪉ἲ(29)ೌࡗ࡚ồࡵࡿ㸬
ຓ㉮༊㛫࡛ࡢᖹᆒ⇕ఏ㐩ಀᩘ
3 1 3 2 2 W 2 W 3 1
1/3 1/3 2 E2
E 2
W 2 w2
W (3 4) ( )
/ g 4 1.88
092
0 / / /
Re /
/
Pr L k
Re/
C .
h 㸦3-6㸧
ὶࢀࡢⓎ㐩ࡋࡓ༊㛫࡛ࡢᖹᆒ⇕ఏ㐩ಀᩘ
Re>3200
344 0 15 2 14
E 2
W )
)( 4 ( 0066
0 k Re / Pr .
.
h 㸦3-7㸧
i 2 E
Re 4
㸦3-8㸧i 2 E
E2i i 2 E
k
Pr C 㸦3-9㸧
15 8 2 2 E
2 i 2
E )
)( 4 g (3 302
0 Re /
. (Re>1600) 㸦3-10㸧
ᚎࠎᢞධࡍࡿ Ỉࡢ⇕㔞ࡀቑࡋ࡚࠸ࡃࡇࡀࢃࡿ㸬ࡲࡓ㸪Ⓨ⏕ࡋࡓẼࡢ⇕㔞ࡀ
ࢇྠࡌ࡛࠶ࡿࡇࡽ㸪⏕ჾࡢᛶ⬟పୗࡶぢࡽࢀ࡞࠸ࡇࡀࢃࡿ㸬ᅗᅗ $+3 ࢩ ࢫࢸ࣒ࡢEERCOP࠼ࡿపᅽẼⓎ⏕ ᗘࡢᙳ㡪ࢆ♧ࡍ㸬ࡇࡇ࡛㸪ᡂ⦼ಀᩘEERࡣ ὶయ⛣㏦⏝࣏ࣥࣉࡢᾘ㈝㟁ຊᑐࡍࡿⓎ⏕ࡋࡓ⇕㔞ࡢẚ⋡㸪ᡂ⦼ಀᩘCOPࡣᢞධࡋࡓ Ỉ ࡢ⇕㔞ᑐࡍࡿⓎ⏕ࡋࡓ⇕㔞ࡢẚ⋡㸪◚⥺ࡣపᅽẼࢆⓎ⏕ࡋ࡞࠸ሙྜࡢEER㸪COPࢆ♧
ࡍ㸬పᅽẼ⏕ᡂࡢEER㸪COPࡶ㸪Ẽ⏕ᡂࡀ࡞࠸ሙྜẚ࡚㧗ࡃ㸪๓⪅ࡢEER ࡣ ࢆࡁࡃୖᅇࡿ㧗࠸ᛶ⬟ࡀᚓࡽࢀࡓ㸬ࡇࡢࡼ࠺࡞ᐇࡽ㸪⇕ᅇࡢ᭱㐺ࢆᅗࡿࡇ
ࡼࡾ㸪ࡉࡽࢩࢫࢸ࣒ᛶ⬟ࡀྥୖࡍࡿవᆅࢆ᭷ࡋ࡚࠸ࡿࡶࡢᮇᚅࡉࢀࡿ㸬
ᅗ ࡣ㸪྾ჾ࡛✵Ẽ㉁㔞ὶ㔞ࢆ0.253 kg/sࡋ࡚✵Ẽຍ⇕ࡋࡘࡘ㸪Ⓨჾ㸰࡛పᅽ
ẼࢆⓎ⏕ࡉࡏࡓࡁ㸪Ⓨჾ㸰ෆࡢఏ⇕⟶ࢆ㏻ࡋ࡚ࡢ⥲ᣓఏ⇕ಀᩘ࠼ࡿẼ ᗘࡢᙳ 㡪ࢆ♧ࡋࡓࡶࡢ࡛࠶ࡿ㸬ᅗ୰ࡣẚ㍑ࡢࡓࡵ㸪ᘧ㹼㸪ᘧ㹼࠾ࡼࡧ ᘧࡽ㸪ࡑࢀࡒࢀ᥎⟬ࡉࢀࡿఏ⇕⟶ෆቨѸ྾ᾮ㛫ᑐὶ⇕ఏ㐩⋡㸪⟶እഃ⇕ఏ㐩⋡࠾ࡼ
ࡧ⇕㏻㐣⋡ࢆᅗ♧ࡋ࡚࠸ࡿ㸬᥎⟬ࡉࢀࡓ⟶ෆഃ⇕ఏ㐩⋡ࡣ⟶እഃẚ࡚ᴟࡵ࡚పࡃ㸪⇕㏻
㐣⋡㏆࠸್࡞ࡗࡓ㸬ࡲࡓ㸪⇕㏻㐣⋡ࡢヨ㦂⤖ᯝ᥎⟬⤖ᯝࡣࡰ୍⮴ࡋⓎჾ㸰ࡢఏ
⇕ᛶ⬟ࢆᴫ⟬ࡍࡿࡇࡀ࡛ࡁ㸪タィᡭἲࡋ࡚᥇⏝ࡋ࠺ࡿ⪃࠼ࡽࢀࡿ㸬
ᮏ❶ࡢࡲࡵ
✵Ẽ⏕ࢩࢫࢸ࣒ࡢ㛤Ⓨࢆ┠ⓗࡋ࡚㸪࣋ࣥࢳࢫࢣ࣮ࣝヨ㦂⨨ࢆ〇సࡋ㸪✵Ẽຍ⇕࠾
ࡼࡧపᅽẼྠ⏕ᡂࡢ≉ᛶホ౯ヨ㦂ࢆ⾜ࡗࡓ㸬ᚓࡽࢀࡓ࡞▱ぢࡣ௨ୗࡢ࠾ࡾ࡛࠶
ࡿ㸬
྾ჾ࡛✵Ẽࢆຍ⇕ᚋ㸪྾ჾࡽ⏕ჾ⛣㏦ࡍࡿ㧗 ࡢ྾ᾮࡢ⇕ᅇࡼࡗ࡚
పᅽẼࢆⓎ⏕ࡋ࡚ࡶ✵Ẽࡢຍ ᛶ⬟ࡢపୗࡀぢࡽࢀࡎ㸪ࡇࡢࡼ࠺࡞⇕ᅇࡢࡓࡵࡢ
ࣁࣈࣜࢵࢻ᪉ᘧࢆ᥇⏝ࡍࡿࡇࡼࡾ㸪&23ࡢྥୖࡀᅗࢀࡿࡇࡀࢃࡗࡓ㸬 ⏕ჾࡢ⇕ᨭィ⟬ࡼࡗ࡚㸪㒊ศࡀ྾ᾮࡢ⮬ᕫ⇕࡛⏕ࡋ࡚࠸ࡿࡇࡀࢃࡗ
ࡓ㸬
పᅽẼⓎ⏕ࡢࡓࡵࡢⓎჾ㸰ࡢఏ⇕ィ⟬ᡭἲࢆ᫂ࡽࡋࡓ㸬
Fig.3-1 Cycle flow of experimental apparatus
Fig.3-2 Structure of upper of equipment
Table 3-1 Equations for heat transfer rate, mass balance and effective temperature difference
Heat transfer rate
Evaporator 1 QE1 CPwMWE1(TWE11 TWE12) QE1 MgE1(HgE1 HgC)
Absorber QA CPAMAA(TAA2 TAA1) QA MgE1(HgE1 HSA2)-MSA1(HSA1 HSA2) Regenerator QR CPWMWR(TWR1 TWR2) QR MgR(HgR HSR1) MSR2(HSR2 HSR1)
Condenser QC CPWMWC(TWC2 TWC12) QC MgR(HgR HgC) Evaporator 2 QE2 MgE2(HgE2 HWE2) QE2 MSE21HSE21 MSR1HSR1)
Heat pump
) (
)
(QA QE2 / QE1 QR COP
w ) (QA QE2 / ER
E
w: Input power for pump
Mass balance
Flow rate MgE1 MSA2 MSA1
M
gRM
gE1 MSR2 MSA1 MSR1 MSA2 MSE21Concentration SA2 SG1 SE21 SA1 SG2 MSG2 SG2 MSG1 SG1
Effective temperature difference Evaporator 1 TE1 (TWE11 TWE12)/ln TWE11 T gE1 / TWE12 T gE1
Absorber TA={(TSA1䠉TAA2)䠉(TSA2䠉TAA1)} /ln{(TSA1䠉TAA2))/(TSA2䠉TAA1)}
Regenerator TR={(TWR1䠉TSR2)䠉(TWR2䠉TSR1)} /ln{(TWR1䠉TSR2))/(TWR2䠉TSR1)}
Condenser TC (TWC2 TWC1)/ln T gC TWC1 / T gC TWC2 Evaporator 2 TE2 (TSE21 TSR1)/ln TSE21 TgE2 / TSR1 TgE2
Table 3-2 Dimensions and shape of tubes in equipment
Element Evaporator 1 Absorber Regenerator Condenser Evaporator 2 Material copper copper copper copper copper The number of the
tubes 74 46 42 91 4
Length [mm] 4848 4940 4352 5500 3200 Inner diameter [mm] 23 23 23 16.6 16.6
Effective heat transfer
area [m2]
25.9 16.4 13.2 26.8 0.67
Fig.3-3Experimental apparatus for low-pressure steam generation
Fig.3-4 Changes of temperature in AHP system with time
Inlet hot water temp.: 80°C Hot water mass flow rate: 9.9 kg/s Inlet cooling water temp.: 15°C Cooling water mass flow rate: 7.2 kg/s
40 50 60 70 80 90 100 110 120 130 140
0.0 1.0 2.0
Time [h]
Temperature [°C]
0 0.1 0.2 0.3 0.4 0.5
Mass flow rate of air [kg/s]
Inlet temp. of air Mass flow rate of air
Generated steam temp.
Outlet temp. of absorbent in Evaporator 2
Outlet temp. of air Inlet temp. of absorbent
in Evaporator 2
Generated steam: 0.0047 kg/s Generated steam: 0.0025 kg/s
Valve adjustment 40
50 60 70 80 90 100 110 120 130 140
0.0 1.0 2.0
Time [h]
Temperature [°C]
0 0.1 0.2 0.3 0.4 0.5
Mass flow rate of air [kg/s]
Inlet temp. of air Mass flow rate of air
Generated steam temp.
Outlet temp. of absorbent in Evaporator 2
Outlet temp. of air Inlet temp. of absorbent
in Evaporator 2
Generated steam: 0.0047 kg/s Generated steam: 0.0025 kg/s
Valve adjustment
Fig.3-5 Düehring plot for cycle solution
Fig.3-6 Effect of low-pressure steam temperature for heat balance in absorber
Mass flow rate of air: about 0.25 kg/s Temp.of air㸸80 °C -124°C
Fig.3-7Effect of low-pressure steam temperature for heat balance in regenerator
Mass flow rate of air: about 0.25 kg/s Temp.of air㸸80 °C -124°C
㻜 㻝㻜㻜㻜㻜㻜 㻞㻜㻜㻜㻜㻜 㻟㻜㻜㻜㻜㻜 㻠㻜㻜㻜㻜㻜 㻡㻜㻜㻜㻜㻜
ධཱྀ ฟཱྀ ධཱྀ ฟཱྀ ධཱྀ ฟཱྀ
⇕㔞>N-K@ ✵Ẽ䛾ຍ ⇕㔞
྾ᾮ䛾⇕㔞䠄ฟཱྀ䠅
Ẽ䛾⇕㔞
྾ᾮ䛾⇕㔞㻔ධཱྀ䠅
㼠 㼠
EΥ పᅽẼ
Ⓨ⏕
FΥ పᅽẼ
Ⓨ⏕
DపᅽẼ
Ⓨ⏕࡞ࡋ
㻜 㻝㻜㻜㻜㻜㻜 㻞㻜㻜㻜㻜㻜 㻟㻜㻜㻜㻜㻜 㻠㻜㻜㻜㻜㻜 㻡㻜㻜㻜㻜㻜
ධཱྀ ฟཱྀ ධཱྀ ฟཱྀ ධཱྀ ฟཱྀ
⇕㔞>N-K@ Ⓨ⏕䛧䛯Ẽ䛾⇕㔞
྾ᾮ䛾⇕㔞䠄ฟཱྀ䠅 ᢞධ䛧䛯 Ỉ䛾⇕㔞
྾ᾮ䛾⇕㔞䠄ධཱྀ䠅
㼠 㼠
EΥ పᅽẼ
Ⓨ⏕
FΥ పᅽẼ
Ⓨ⏕
DపᅽẼ
Ⓨ⏕࡞ࡋ
Fig. 3-8 Effect of generated steam temperature on EER and COP (air flow rate: 0.25 kg/s)
Fig. 3-9 Effect of generated steam temperature on overall heat transfer coefficient in evaporator 2
グ グྕ
ᮏ❶⏝ࡍࡿグྕࢆࡲࡵࡿࠋ
A = heat transfer surface area [m2]
COP = coefficient of performance [-]
Cp = specific heat [J/(kg·K)]
Do = outside diameter of tube [m]
EER = energy efficiency ratio [-]
Gc = mass flux of air [kg/(m2㺃s]
g = gravity [m/s2]
H = specific enthalpy [J/kg]
h = heat transfer coefficient [W/m2·K]
k = thermal conductivity [W/m·K]
= mass flow rate of falling liquid per perimeter [kg/m㺃s]
= mass flow rate [kg/s]
= heat transfer rate [W]
Re = Reynolds number [-]
T = temperature [K]
UA = overall heat transfer coefficient [W/m2·K]
w = input power for pumps [W]
T = temperature difference [K]
T = temperature difference [K]
Special characters
= correction factor for the heat transfer coefficient [-]
= concentration of LiBr in solution [wt%]
a = viscosity in bulk temperature [Pa·s]
w = viscosity in tube wall temperature [Pa·s]
M Q
Subscripts
1 = inlet of fluid 2 = outlet of fluid
A = absorber
a = air
C = condenser
E1 = evaporator 1 E2 = evaporator 2 g = gas phase (steam) p = input pump power base R = regenerator
S = absorption solution
W = water
➨
➨㸲❶ ࢫࣃࣛࣝ⟶ࢆ⏝࠸ࡿ $+3 ࡢ⇕࣭≀㉁⛣ື≉ᛶ
⇕ࡣఏ⇕⟶ቨࢆ㏻ࡋ࡚྾ᾮ⟶እ✵Ẽࡢ㛫࡛⾜ࢃࢀࡿ㸬ࡋࡋ࡞ࡀࡽ྾ᘧࣄ
࣮ࢺ࣏ࣥࣉ࠾ࡅࡿ྾ᾮ✵Ẽࡢ ᗘศᕸࡣᚑ᮶ࡢྥὶᆺ⇕ჾࡣ㐪ࡗ࡚ࡃࡿ㸬྾
ᾮࡀẼࢆ྾ࡋ᪼ ࡋ࡞ࡀࡽὶୗࡍࡿࡓࡵ྾ᾮࡢ᭱㧗 ᗘࡣఏ⇕⟶ࡢධཱྀ࡛ࡣ࡞ࡃ㸪 ධཱྀࡼࡾὶୗࡋࡓሙᡤ࡛☜ㄆࡉࢀࡿ㸬ࡇࢀࡣධཱྀฟཱྀࡢ ᗘࢆ⏝ࡋࡓᚑ᮶ࡢᑐᩘᖹᆒ ᗘᕪ࡛ࡣ ᗘᕪࢆᐃ⩏࡛ࡁ࡞࠸ࡇࢆពࡍࡿ㸬
ᚋࢫࢣ࣮ࣝࢵࣉ➼ࡢ⨨タィୖ㸪ఏ⇕⟶ࢆ㏻ࡋ࡚ࡢఏ⇕≉ᛶࡸఏ⇕⟶ෆࡢ⇕࣭≀㉁
⛣ື≉ᛶࢆ᫂ࡽࡋ࡚࠾ࡃᚲせࡀ࠶ࡿࡀ㸪྾ჾෆࡣఏ⇕⟶ࡀከ⟶࡛㓄⨨ࡉࢀ࡚࠾ࡾ༢
⟶࠾࠸࡚ࡢ≉ᛶࢆ☜ㄆࡍࡿࡇࡀ㞴ࡋ࠸㸬ࡲࡓ྾ჾෆࡢࡇࡢࡼ࠺࡞⇕࣭≀㉁⛣ືࡢ࣓
࢝ࢽࢬ࣒ࡸᾮ⭷✵Ẽࡢ㛫࠾ࡅࡿ⥲ᣓ⇕ఏ㐩ಀᩘࢆồࡵࡿࡓࡵࡢ ᗘᕪࢆ᫂☜ᐃ⩏ࡍ
ࡿࡇࡣ༑ศゎ᫂ࡉࢀ࡚࠸࡞࠸㸬ࡑࡇ࡛ᮏ❶࡛ࡣ㸪࣋ࣥࢳࢫࢣ࣮ࣝ྾ᘧࣄ࣮ࢺ࣏ࣥࣉ
ࡢᛶ⬟ᢕᥱࢆᨵၿࡍࡿࡓࡵࡢᇶ♏◊✲ࡋ࡚㸪ఏ⇕⟶࡛࠶ࡿ㖡〇ࢫࣃࣛࣝ༢⟶ࡢఏ⇕ヨ 㦂ࢆ⾜࠸ఏ⇕⟶ࡢ⇕࣭≀㉁⛣ື≉ᛶࢆᢕᥱࡍࡿ◊✲ࢆ⾜࠸ࡲࡓᖹ⟶࡛ࡢఏ⇕ᐇ㦂ࡶ⾜
࠸ࢫࣃࣛࣝ⟶ࡢẚ㍑ࢆ⾜࠺㸬
ᐇ㦂⨨࠾ࡼࡧᐇ㦂᪉ἲ
ᐇ㦂⨨ᅗ4-1(a)ᅗᅗ4-1(b) ᐇ㦂⨨య┿ᴫ␎ᅗࢆ♧ࡍ㸬ఏ⇕⟶ࡣෆᚄ23mm㸪እᚄ
25mm㸪㛗ࡉ1.6mࡢ㖡〇ࢫࣃࣛࣝ⟶ᖹ⟶࡛㸪ᆶ┤タ⨨ࡋ࡚࠶ࡿ㸬ᅗᅗ4-2ࡣఏ⇕⟶,
྾ᾮ ᗘࡢ ᐃ⨨ࢆ⾲ࡋ࡚࠾ࡾ,ᅗ୰ࡢձࠥմࡣ㡰ධཱྀ྾ᾮ ᗘฟཱྀ྾ᾮ ᗘ ఏ⇕⟶ධཱྀ⾲㠃 ᗘఏ⇕⟶ฟཱྀ⾲㠃 ᗘࡢ ᐃ⨨ࢆ♧ࡍ㸬ᅗᅗ4-3ᐇ㦂࡛⏝࠸ࡓ྾ჾ ࡢୖ㒊ᵓ㐀ࡢᴫ␎ᅗࢆ♧ࡍ㸬LiBrỈ⁐ᾮࡣୖ㒊ࣜࢨ࣮ࣂ࣮ࡽ౪⤥ࡋ࡚ఏ⇕⟶ෆ㠃ἢࡗ
࡚ᾮ⭷≧ὶୗࡉࡏࡿ㸬ఏ⇕⟶ୖ㒊ࡣᅗᅗ4-4♧ࡍⓎჾࡶ᥋⥆ࡉࢀ࡚࠾ࡾ㸪ᡤᐃ ᗘ
ຍ ࡋࡓỈẼࡣୖ㒊ࡽὶධࡋ࡚ఏ⇕⟶ෆ㠃ࡢᾮ⭷྾ࡉࢀࡿ㸬ࡑࡢᚋ྾ᾮࡣᅗᅗ 4-5♧ࡍୗ㒊ࣜࢨ࣮ࣂ࣮⁀ࡲࡾ㸪ᐇ㦂⤊ᚋࡣࢧࣥࣉཱྀࣝࡼࡾࢧࣥࣉࣝࢆ᥇ྲྀࡋ⃰ᗘ
ࢆ ᐃࡍࡿ㸬
ᐇ㦂᮲௳
ὶ㔞㸸0.1㹼0.7 kg/min
྾ᾮ⃰ᗘ㸸56㹼58%
Ẽ ᗘ㸸20 Υ㸪60 Υ
ఏ⇕⟶㸸㖡〇ࢫࣃࣛࣝ⟶㸪ᖹ⟶
ᐇ㦂᪉ἲ
┿✵࣏ࣥࣉ࡛⨨ෆࢆ㣬Ẽᅽ௨ୗࡲ࡛ῶᅽࡍࡿ
Ⓨჾୖ㒊ࣜࢨ࣮ࣂ࣮ୗ㒊ࣜࢨ࣮ࣂ࣮ࡢ㛫ࡢࣂࣝࣈࢆ㛢ࡌࡿ
Ⓨჾ࡛Ẽࢆసࡿ
Ⓨჾୖ㒊ࣜࢨ࣮ࣂ࣮ࡢ㛫ࡢࣂࣝࣈࢆ㛤ࡅ྾ჾẼࢆὶࡍ
Ẽࢆὶࡍྠ⁐ᾮࢱࣥࢡࡽ࣏ࣥࣉ࡛྾ᾮࢆ㏦ࡿ
ఏ⇕⟶ෆࢆᾮ⭷ࡀẼࢆ྾ࡋ࡞ࡀࡽὶୗࡍࡿ
ᐇ㦂⤊ᚋୗ㒊ࣜࢨ࣮ࣂ࣮⁀ࡲࡗ࡚࠸ࡿ྾ᾮࡢ⃰ᗘࢆ ᐃ
ͤ྾ᾮࡣᐇ㦂๓ࡶ ᐃ
ྛ㒊 ᗘࢹ࣮ࢱࡼࡾ⇕ఏ㐩ಀᩘࢆヨ⟬
ࡲࡓࢧࣥࣉࣜࣥࢢ᪉ἲࡣᅗ4-5ࡢ␒ྕ,グྕࢆᇶୗグ♧ࡍ㸬 ձࡢࣂࣝࣈࢆ㛤ࡅ┿✵࣏ࣥࣉ࡛ῶᅽࡍࡿ
ձࡢࣂࣝࣈࢆ㛢ࡵղࡢࣂࣝࣈࢆ㛤ࡅࡿ
㸿⁐ᾮࡀධࡿ
ղࡢࣂࣝࣈࢆ㛢ࡵࡿ
ձࡢࣂࣝࣈࢆ㛤ࡅ⁐ᾮࢆ᥇ྲྀࡍࡿ
ᗘ ᐃ⨨
᮲௳ࡼࡿ ᗘศᕸࡢ㐪࠸
ྛ✀್ࢆ⟬ฟࡍࡿ࠶ࡓࡾ୍❶♧ࡋࡓࡼ࠺ᑐᩘᖹᆒ ᗘᕪࡢၥ㢟ࡀ࠶ࡿ㸬ᅗᅗ 4-6(a)
Ẽ ᗘ60 Υ࠾ࡅࡿఏ⇕⟶ୖ㒊 ᗘศᕸࡢᴫ␎ᅗࢆ㸪ࡲࡓᅗᅗ4-6(b) Ẽ ᗘ20 Υ
࠾ࡅࡿఏ⇕⟶ୖ㒊 ᗘศᕸࡢᴫ␎ᅗࢆ♧ࡍ㸬ᅗ୰ࡢձࡣୖ㒊ࣜࢨ࣮ࣂ࣮ෆࡢ྾ᾮ ᗘ, ղࡣఏ⇕⟶ὶධ┤ᚋࡢ ᗘ,ճࡣఏ⇕⟶ୖ㒊⾲㠃 ᗘࢆ♧ࡍ㸬ᮏ◊✲࡛ࡣධཱྀฟཱྀࡢᾮ⭷
ᗘఏ⇕⟶⾲㠃 ᗘࢆᇶ⇕ఏ㐩ಀᩘࢆヨ⟬ࡋ࡚࠸ࡿ㸬ࡇࡢࡁఏ⇕⟶⾲㠃 ᗘࡣᅗ4-6(a)㸪
ᅗ4.6(b)ࡢճ♧ࡍࡼ࠺࡞ఏ⇕⟶⾲㠃タ⨨ࡋࡓ⇕㟁ᑐࡼࡗ࡚ ᐃࡉࢀ࡚࠸ࡿ㸬ࡋࡋఏ
⇕⟶ࡢᾮ⭷ὶධཱྀ࠾ࡅࡿᾮ⭷ ᗘࡘࡲࡾᅗࡢձ♧ࡍୖ㒊ࣜࢨ࣮ࣂ࣮ෆࡢ྾ᾮ ᗘ
ࢆධཱྀᾮ⭷ ᗘࡍࡿධཱྀᾮ⭷ ᗘࡼࡾࡶධཱྀ⾲㠃 ᗘࡀ㧗࠸ ᗘ࡞ࡿ㸬ࡑࡢࡓࡵᾮ
⭷⟶እ✵Ẽࡢ㛫ࡢᑐᩘᖹᆒ ᗘᕪࡼࡾࡶ⟶⾲㠃⟶እ✵Ẽࡢ㛫ࡢᑐᩘᖹᆒ ᗘᕪࡀ
ࡁࡃヨ⟬ࡉࢀ࡚ࡋࡲ࠸㸪ᾮ⭷ᑐὶ⇕ఏ㐩ಀᩘࡀ㈇್࡞ࡿሙྜࡀ࠶ࡿ㸬ࡑࡇ࡛ᐇ㝿ᐇ 㦂୰ࡢఏ⇕⟶⾲㠃ࢆࢧ࣮ࣔࢢࣛࣇ࡛ᙳࡋ ᗘศᕸࢆぢ࡚ࡳࡓ㸬
ᗘ ᐃ⨨
ᅗ4-7(a)㸪ᅗ4-7(b)㸪ᅗ4-7(c) ࢫࣃࣛࣝ⟶ࢆ⏝࠸࡚Ẽ ᗘ60 Υ࡛ᐇ㦂ࢆ⾜ࡗࡓ㝿
ࡢఏ⇕⟶ ᗘศᕸᅗࢆ♧ࡍ㸬ࡲࡓᅗ4-8(a)㸪ᅗ4-8(b)㸪ᅗ34-8(c) ᖹ⟶ࢆ⏝࠸࡚Ẽ ᗘ 60Υ࡛ᐇ㦂ࢆ⾜ࡗࡓ㝿ࡢఏ⇕⟶ࡢ ᗘศᕸࢆ♧ࡍ㸬Ẽࢆ྾ࡋ,᪼ ࡋ࡞ࡀࡽὶୗࡋ࡚࠸
ࡃࡓࡵ,᭱㧗 ᗘࡣఏ⇕⟶ὶධ㒊ࡼࡾᑡࡋὶୗࡋࡓሙᡤ(ᾮ⭷ὶධཱྀࡼࡾ15cmୗ᪉)࡚ほ ࡉࢀࡿ㸬ࡑࡢࡓࡵẼ ᗘ60 Υࡢᐇ㦂࠾࠸࡚ࡣᅗ4-6(a) ࠾ࡼࡧᅗ 4-6(b) ࡢմ♧ࡍࡼ
࠺ఏ⇕⟶ෆ㒊ࡶ⇕㟁ᑐࢆタ⨨ࡋ㸪ࡇࡢ᭱㧗 ᗘࢆධཱྀᾮ⭷ ᗘࡋ࡚ᑐᩘᖹᆒ ᗘᕪ
ࢆᐃ⩏ࡋࡓ㸬ᅗ4-6(b) ࢫࣃࣛࣝ⟶㸪ᖹ⟶ࡑࢀࡒࢀࢆ⏝࠸࡚Ẽ ᗘ20Υ࡛ᐇ㦂ࢆࡋ ࡓ㝿ࡢఏ⇕⟶ ᗘศᕸᴫ␎ᅗࢆ㸪ᅗᅗ4-9(a)㸪ᅗ4-9(b)㸪ᅗ4-9(c) ࠾ࡼࡧᅗ4-10(a)㸪ᅗ4-10(b)㸪
ᅗ4-10(c)㸪ఏ⇕⟶ࡢ ᗘศᕸࢆ♧ࡍ㸬Ẽ ᗘࡀ20Υࡢሙྜ,Ẽ ᗘࡀ60 Υࡢሙྜ
ẚ྾ᛂ㏿ᗘࡀ⦆ࡸ࡞ࡿࡓࡵ㸪Ẽ ᗘ60 Υࡢࡼ࠺ఏ⇕⟶ධཱྀഃ࡛྾ࡢ㒊 ศࡀ⾜ࢃࢀࡿࡢ࡛ࡣ࡞ࡃ㸪ὶୗࡋ࡚࠸ࡃ㝿ࡶ྾ᛂࡀ⥆࠸࡚࠸ࡿ⪃࠼ࡽࢀࡿ㸬ࡑࡢࡓ
ࡵධཱྀഃࡀ᭱ࡶప ࡞ࡾฟཱྀഃࡀ᭱ࡶ㧗 ࡞ࡗ࡚࠸ࡿ㸬ࡲࡓᅗ 4-10(d) ఏ⇕⟶ୖ㒊 㸦ᾮ⭷ὶධཱྀࡼࡾ5~15 cm㸧ࢆ᥋ࡋࡓ ᗘศᕸᅗࢆ♧ࡍ㸬ୖ㒊ࣜࢨ࣮ࣂ࣮ෆࡢ྾ᾮࡼࡾ
ᗘࡣ㧗࠸ࡀ,Ẽ ᗘ60Υ࡛ධཱྀ ᗘࡋ࡚᥇⏝ࡋࡓ⨨ධཱྀ࡛ࡢ ᗘᕪࡣࢇ
ぢࡽࢀ࡞࠸㸬ࡑࡢࡓࡵẼ ᗘࡼࡽࡎྠࡌ⨨࡛ ᗘࢆ ᐃࡋᾮ⭷⟶ቨࡢᑐᩘᖹ ᆒ ᗘᕪࢆᐃ⩏ࡋࡓ㸬
௨ୖࡼࡾ㸪ධཱྀฟཱྀࡢ ᗘᕪࡣఏ⇕⟶ධཱྀฟཱྀ࡛ࡢ ᗘ࡛ࡣ࡞ࡃ྾ᾮࡢ᭱㧗,᭱ప ᗘ
ࢆࡾᐃ⩏ࡍࡿࡇࡋࡓ㸬ࡲࡓఏ⇕⟶ࡢ⾲㠃✚ࡣධཱྀ⾲㠃 ᗘࢆ ᐃࡋࡓ⨨ࡽฟཱྀ
⾲㠃 ᗘࢆ ᐃࡋࡓ⨨ࡲ࡛ࡢ㛗ࡉࢆᇶ‽ィ⟬ࡋࡓ㸬
⟬ฟ᪉ἲ
㛫࠾ࡅࡿẼ྾㔞ࡢ㐪࠸
ᅗ4-11ࢫࣃࣛࣝ⟶ࢆ⏝࠸ࡓẼ ᗘ60 Υࡢᐇ㦂࠾ࡅࡿྛ㒊 ᗘ/⨨㛫ᕪᅽࡢ⤒
ኚࢆ♧ࡍ㸬ࡲࡓᅗᅗ4-12ྛ ᐃ⨨ࡢᴫ␎ᅗࢆ♧ࡍ㸬ࢢࣛࣇ♧ࡍࡼ࠺ᐇ㦂㛤ጞ
┤ᚋࡣ ᗘࡀᏳᐃࡏࡎ,ᾮ⭷ࡢẼ྾㔞ࡤࡽࡘࡁࡀ⏕ࡌࡿ㸬ࡑࡢࡓࡵᐇ㦂๓ᚋࡢࢧࣥࣉ
ࣝ⃰ᗘࢆ⏝࠸࡚྾㔞ࢆ⟬ฟࡍࡿ⇕ఏ㐩ಀᩘࡸ≀㉁⛣ືಀᩘࡢ್ࡀᐇ㝿ࡢᐃᖖ≧ែ࠾
ࡅࡿ್ࡁࡃ㐪ࡗ࡚ࡃࡿྍ⬟ᛶࡀ࠶ࡿ㸬ࡑࡢࡓࡵᮏ◊✲࡛ࡣᅗᅗ4-13ࡢࣇ࣮ࣟࢳ࣮ࣕࢺ
♧ࡍィ⟬᪉ἲࢆ⏝࠸࡚㠀ᐃᖖ≧ែ,ᐃᖖ≧ែ࠾ࡅࡿྛ✀್ࢆ௨ୗࡢࡼ࠺Ỵᐃࡋࡓ㸬ᅗ 4-13♧ࡍhaࡣ⟶እ⮬↛ᑐὶ⇕ఏ㐩⋡ࢆ♧ࡍ㸬ࡲࡓX2ࡣᐇ㦂⤊ୗ㒊ࣜࢨ࣮ࣂ࣮⁀
ࡲࡗ࡚࠸ࡿ⁐ᾮࡢ⃰ᗘࢆィ⟬ࡼࡗ࡚⟬ฟࡋࡓ್࡛࠶ࡾ㸪Xeࡣᐇ㝿ᐇ㦂⤊ୗ㒊ࣜ
ࢨ࣮ࣂ࣮⁀ࡲࡗ࡚࠸ࡿ⁐ᾮࡢࢧࣥࣉࣝࢆ᥇ྲྀࡋ ᐃࡋࡓ⃰ᗘࢆ♧ࡍ㸬
ᐇ ್௨እࡢྛ✀್⟬ฟ᪉ἲ
ࡲࡎᅗᅗ4-14♧ࡍఏ⇕ࣔࢹࣝᴫ␎ᅗࢆཧ↷ᚤᑠ㛫tiЍti+dt࠾ࡅࡿ࢚ࢿࣝࢠ࣮ࣂࣛࣥ
ࢫࢆ⪃࠼ࡿ㸬
⟶እࡢ⮬↛ᑐὶ⇕ఏ㐩⋡ࡀ୍ᐃ௬ᐃࡍࡿᘧ(4-1)ࡼࡾఏ⇕⟶ࢆ㏻ࡋ࡚ࡢ⇕㔞 Qiࡀồࡵࡽ
ࢀࡿ㸬
) (
1a
Q
i/ A Δ T
lnih
(4-1)ࡲࡓᑐᩘᖹᆒ ᗘᕪࡣ௨ୗࡢࡼ࠺ᐃ⩏ࡉࢀࡿ㸬
∆Tln1i=ሾሺTs1i-Taiሻ-ሺTs2i-TaiሻሿΤlnሾሺTs1i-Taiሻ ሺTΤ s2i-Taiሻሿ (4-2)
ࡓࡔࡋAࡣఏ⇕⟶እഃࡢ⾲㠃✚࡛࠶ࡾ,Ts1,Ts2,Taiࡣᐇ ್࡛ࡑࢀࡒࢀධཱྀ⾲㠃 ᗘ㸪ฟཱྀ⾲
㠃 ᗘ㸪⟶እẼ ᗘࢆ♧ࡍ㸬ࡲࡓQiࡣᘧ(4-3) ࡽࡶồࡵࡽࢀࡿ㸬
dQi=Qidt= G1iqf1i-G2iqf2i dt+dmiLei (4-3)
G2i-G1i=mi (4-4)
G1iࡣᐇ ್࡛࠶ࡾࡑࢀࡒࢀධཱྀഃࡢ྾ᾮ㔞⁐ᾮࡀ྾ࡍࡿẼࡢ₯⇕ࢆ♧ࡋ࡚
࠸ࡿ㸬ࡲࡓG2imiࡣฟཱྀഃࡢ྾ᾮ㔞Ẽ྾㔞ࢆ♧ࡍ㸬ࡇࡢࡁධཱྀฟཱྀࡢ྾
ᾮ࢚ࣥࢱࣝࣆ࣮qf1iqf2iࡣ௨ୗࡢᘧ(4-5)㸪(4-6) ♧ࡍࡼ࠺྾ᾮࡢ⃰ᗘ ᗘࡽồࡵ
ࡽࢀࡿ㸬
qf1i=f X1,Tf1i (4-5)
qf2i=f X2i,Tf2i (4-6)
ࡓࡔࡋX1 ,Tf1,Tf2ࡣᐇ ್࡛ࡑࢀࡒࢀධཱྀ྾ᾮ⃰ᗘ㸪ධཱྀ྾ᾮ ᗘ,ฟཱྀ྾ᾮ ᗘࢆ♧
ࡍ㸬ࡲࡓX2iࡣฟཱྀ྾ᾮ⃰ᗘࢆ♧ࡋ௨ୗࡢࡼ࠺ồࡵࡽࢀࡿ㸬
X2i=ሺX1G1iΤG1i+miሻ (4-7)
ࡇࡇ࡛ᘧ(4-1) ࡢQi ᘧ(4-3) ࡢQiࡀ୍⮴ࡍࡿࡼ࠺Ẽ྾㔞miࢆỴᐃࡍࡿࡇ࡛X2iࡀ
⟬ฟࡉࢀࡿ㸬
ࡲࡓᘧ(4-8)♧ࡍࡼ࠺྾㔞ࢆᐇ㦂㛫ࢃࡓࡗ࡚✚ศࡍࡿ㸬ࡲࡓᘧ(4-9) ࠾ࡼࡧᘧ(4-10) ࢆ⏝࠸࡚ᐇ㦂⤊ୗ㒊ࣜࢨ࣮ࣂ࣮⁀ࡲࡗ࡚࠸ࡿ⁐ᾮࡢ⃰ᗘX2ࢆ⟬ฟࡍࡿ㸬
=σimidt
(4-8)
G1idt+M= G2idt
i i
X2=ሺX1G1ΤG2ሻ (4-10)
ࡑࡢᚋᘧ(4-11) ♧ࡍࡼ࠺ᐇ㝿ᐇ㦂⤊ୗ㒊ࣜࢨ࣮ࣂ࣮⁀ࡲࡗ࡚࠸ࡿ⁐ᾮࡢࢧ
ࣥࣉࣝࢆ᥇ྲྀࡋ ᐃࡋࡓ⃰ᗘ࡛࠶ࡿ Xeᘧ(4-10) ࡛ồࡵࡽࢀࡓ X2ࡀ୍⮴ࡍࡿࡲ࡛ᘧ(4-1)
ࡽᘧ(4-10) ࢆ⧞ࡾ㏉ࡋィ⟬ࡋhaࢆỴᐃࡍࡿࡇ࡛ᐇ ࡛ࡁ࡚࠸࡞࠸್ࢆ⟬ฟࡋࡓ㸬
X2=X (4-11)
⇕ఏ㐩࣭≀㉁⛣ືಀᩘࡢ⟬ฟ
ᅗ4-15♧ࡍఏ⇕ࣔࢹࣝᴫ␎ᅗࢆཧ↷㸪 ᘧ (4-12) ♧ࡍᚤᑠ㛫tiЍti+dt࠾ࡅࡿ
⇕㏻㐣⋡ࢆ⪃࠼ࡿ㸬
Ui= QiΤሺA∆T 2iሻ (4-12)
ࡲࡓᑐᩘᖹᆒ ᗘᕪࡣ௨ୗࡢࡼ࠺ᐃ⩏ࡉࢀࡿ㸬
∆Tln2i= Tf1i-Tai - Tf2i-Tai Τln Tf1i-Tai Tf2i-Tai (4-13)
ᐃᖖ≧ែࡢ㛫ࢆmЍn⪃࠼ࡿࡑࡢ㛫ࡢᖹᆒࡢ⇕㏻㐣⋡ࡣᘧ(4-14)ࡢࡼ࠺ồࡵࡽࢀ
ࡿ㸬
(4-9)
ᘧ(4-13) ࠾ࡼࡧᘧ(3-1) ࡼࡾồࡵࡽࢀࡓ⇕㏻㐣⋡U࠾ࡼࡧ⟶እ⮬↛ᑐὶ⇕ఏ㐩⋡haࢆ⏝࠸
࡚ᖹᆒࡢᾮ⭷⇕ఏ㐩⋡ࢆᘧ(4-15) ࡢࡼ࠺ồࡵࡓ㸬
1Τhf=ሾሺ1ΤUሻെሺ1ΤhaሻሿሺA' AΤ ሻ (4-15)
ࡓࡔࡋAࡣఏ⇕⟶እഃ⾲㠃✚, A’ࡣఏ⇕⟶ෆഃ⾲㠃✚࡛࠶ࡿ㸬ࡲࡓࢫࣃࣛࣝ⟶࠾࠸࡚
ఏ⇕㠃✚ࡣᖹ⟶┦ᙜ࡛㏆ఝࡋ࡚࠾ࡾ㸪ఏ⇕⟶ቨࡢ⇕ᢠࡣ㠀ᖖᑠࡉ࠸ࡓࡵ↓どࡋ࡚࠸
ࡿ㸬
ᅗ4-15♧ࡍ⇕࣭≀㉁⛣ື࠾ࡅࡿ྾ჾෆࣔࢹࣝᴫ␎ᅗࢆཧ↷4.2.2㡯࡛ồࡵࡓẼ
྾㔞ࢆᇶ≀㉁⛣ືಀᩘࢆồࡵ࡚࠸ࡃ㸬ࡲࡎᾮ⭷⏺㠃ࡢẼᅽࡣ྾ᾮ⃰ᗘ ᗘᑐ ࡍࡿ㣬Ẽᅽ➼ࡋ࠸௬ᐃࡋࡓሙྜ, Ẽ྾㔞ࡣᘧ (4-16) ࡢࡼ࠺♧ࡍࡇࡀ࡛ࡁ
ࡿ㸬
mi=βgiڄA'ڄΔPlni (4-16)
ࡓࡔࡋβgi,ΔPlniࡣࡑࢀࡒࢀ࢞ࢫഃ≀㉁⛣ືಀᩘ,ᑐᩘᖹᆒᅽຊᕪࢆ♧ࡍ㸬
ࡇࡇ࡛࢞ࢫഃ≀㉁⛣ືಀᩘࡣỈẼࡢ㣬ᅽຊධཱྀฟཱྀࡑࢀࡒࢀࡢᾮ⭷⏺㠃Ẽᅽຊ ᕪࡢᑐᩘᖹᆒࢆ᥎㐍ຊࡋ࡚㸪ḟᘧࡢࡼ࠺Ỵᐃࡋࡓ㸬
ΔΡlni = Pvi-Pf1i - Pvi-Pf2i / ln (Pvi-Pf1i)⁄(Pvi-Pf2i) (4-17)
ࡓࡔࡋPvi, Pf1i, Pf2iࡣࡑࢀࡒࢀỈẼࡢ㣬ᅽຊ,ධཱྀᾮ⭷⏺㠃Ẽᅽ㸪ฟཱྀᾮ⭷⏺㠃Ẽ
U= U
idt Τ ሺm+n+1ሻ
n (4-14)
ᅽࢆ♧ࡍ㸬ᐃᖖ≧ែࡢ㛫ࢆmЍn⪃࠼ࡿࡑࡢ㛫ࡢᖹᆒࡢ࢞ࢫഃ≀㉁⛣ືಀᩘࡣᘧ (4-18)ࡢࡼ࠺ồࡵࡽࢀࡿ㸬
βg= gi Τሺm+n+1ሻ
n
i=m
ࡲࡓ,ὶୗᾮ⭷࠾ࡅࡿẼᾮ⏺㠃ࡣჾෆᅽຊᖹ⾮⪃࠼ࡓሙྜ㸪Ẽ྾㔞ࡣᘧ (4-19) ࡢࡼ࠺♧ࡍࡇࡀ࡛ࡁࡿ㸬
mi=βciڄ ڄA'ڄΔ lni (4-19)
ࡓࡔࡋβ i, ,Δ lniࡣᾮഃ≀㉁⛣ືಀᩘ,ᾮ⭷ࡢᐦᗘ㸪ᑐᩘᖹᆒ⃰ᗘᕪࢆ♧ࡍ㸬
ࡇࡇ࡛ᾮഃ≀㉁⛣ືಀᩘࡣධཱྀฟཱྀࡢẼᾮ⏺㠃ࡢᖹ⾮⃰ᗘὶୗᾮ⭷ࡢᖹᆒ⃰ᗘࡢᑐ
ᩘᖹᆒ⃰ᗘᕪࢆ᥎㐍ຊࡋ࡚ḟᘧࡢࡼ࠺Ỵᐃࡋࡓ㸬
Δ lni = f1i- i - f2i- i / ln (ξf1i- i)/( f2i- i) (4-20)
ࡓࡔࡋ f1i, f2i, iࡣᾮ⭷ࡢH2O㉁㔞⃰ᗘ࡛࠶ࡾ,ࡑࢀࡒࢀධཱྀᾮ⭷ᖹ⾮⃰ᗘ,ฟཱྀᾮ⭷ᖹ⾮
⃰ᗘ,ὶୗᾮ⭷ࡢᖹᆒ⃰ᗘࢆ♧ࡍ㸬ᐃᖖ≧ែࡢ㛫ࢆmЍn⪃࠼ࡿࡑࡢ㛫ࡢᖹᆒࡢᾮഃ
≀㉁⛣ືಀᩘࡣᘧ(4-21)ࡢࡼ࠺ồࡵࡽࢀࡿ㸬
βc= ci Τሺm+n+1ሻ
n
i=m
(4-18)
(4-21)
ࡲࡓࣞࣀࣝࢬᩘࡣᘧ(4-22) ♧ࡍ༢ࢀࡪࡕᙜࡓࡾࡢ྾ᾮὶ㔞ࢆ⏝࠸࡚ᘧ(4-23) ࡢ
ࡼ࠺ồࡵࡿࡇࡀ࡛ࡁࡿ㸬
Γ=G Τ2πr (4-22)
Reൌ ͶΓΤ (4-23)
ࡓࡔࡋrμࡣࡑࢀࡒࢀఏ⇕⟶ࡢෆഃ༙ᚄᾮ⭷⢓ᗘࢆ♧ࡍ㸬ࡲࡓ≀ᛶ್ࡣᩥ⊩(23)ࢆཧ⪃
ࡋࡓ㸬
⤖ᯝ⪃ᐹ
ᾮ⭷⇕ఏ㐩ಀᩘࣞࣀࣝࢬᩘࡢ㛵ಀ
ᅗ4-16Ẽ ᗘ20Υ࠾ࡅࡿ⤖ᯝࢆ,ᅗ4-17Ẽ ᗘ60Υ࠾ࡅࡿ⤖ᯝࢆ♧ࡍ㸬
ࡕࡽࡢẼ ᗘ࡛ࡶᖹ⟶࠾࠸࡚ࣞࣀࣝࢬᩘࡀቑຍࡍࡿᾮ⭷ᑐὶ⇕ఏ㐩⋡ࡣῶᑡ ࡋ࡚࠸ࡃࡀ㸪ࢫࣃࣛࣝ⟶࡛ࡣࣞࣀࣝࢬᩘࡶቑຍࡋ࡚࠸ࡃഴྥࡀぢࡽࢀࡓ㸬ὶ㔞 ࡀቑຍࡍࡿᾮ⭷ࡀཌࡃ࡞ࡾᾮ⭷ࡢ⇕ఏ㐩ಀᩘࡣᑠࡉࡃ࡞ࡿࡇࡀ⪃࠼ࡽࢀࡿ㸬ࡋࡋ᪤
ࡢ◊✲11,12)࡛ࡣᒙὶᇦ࠾࠸࡚ὶ㔞ࡢቑຍక࠸ᾮ⭷ࡀཌࡃ࡞ࡾᑐὶ⇕ఏ㐩⋡ࡣῶᑡ
ࡋ㸪ὶᇦ࡛ࡣᾮ⭷ࡢࢀࡼࡗ࡚ୖ᪼ࡍࡿࡇࡀ☜ㄆࡉࢀ࡚࠸ࡿ㸬ࡇࡢࡇࡽᒙὶᇦ
࠾࠸࡚ࢫࣃࣛࣝ⟶ࡢ⤖ᯝࡀὶᇦࡢഴྥࡀぢࡽࢀࡓࡢࡣࢫࣃࣛࣝ⟶ࡼࡿὶಁ㐍
ຠᯝࡼࡗ࡚ᾮ⭷ࡀࡉࢀࡓࡽࡔ⪃࠼ࡽࢀࡿ㸬
≀㉁⛣ືಀᩘࣞࣀࣝࢬᩘࡢ㛵ಀ
ᅗ4-18ᅗ4-19ࡑࢀࡒࢀẼ ᗘ20Υ࠾ࡼࡧ60Υ࠾ࡅࡿ࢞ࢫഃ≀㉁⛣ືಀᩘࣞ
ࣀࣝࢬᩘࡢ㛵ಀࢆ㸪ࡲࡓᅗᅗ4-20ᅗ4-21ࡑࢀࡒࢀẼ ᗘ20Υ࠾ࡼࡧ60Υ࠾ࡅ
ࡿᾮഃ≀㉁⛣ືಀᩘࣞࣀࣝࢬᩘࡢ㛵ಀࢆ♧ࡍ㸬
ࢫࣃࣛࣝ⟶࠾࠸࡚ࡕࡽࡢẼ ᗘ࡛ࡶࣞࣀࣝࢬᩘࡢቑຍࡶ࢞ࢫഃ≀㉁⛣
ືಀᩘ㸪ᾮഃ≀㉁⛣ືಀᩘࡕࡽࡶቑຍࡋ࡚࠸ࡗࡓ㸬ࡇࢀࡣࢫࣃࣛࣝ⟶ࡼࡗ࡚ᾮ⭷ࡀ
ࡉࢀࡿࡓࡵ྾ಁ㐍ࡀ⾜ࢃࢀࡓ⪃࠼ࡽࢀࡿ㸬ࡲࡓᖹ⟶࡛ࡣࣞࣀࣝࢬᩘࡢቑຍᑐࡋ
20Υ࡛ࡣቑຍഴྥࢆ 60Υ࡛ࡣῶᑡഴྥࢆ♧ࡋࡓ㸬Ẽ ᗘࡀ㧗࠸ሙྜ㸪ὶධ┤ᚋࡽᾮ⭷
ࡣᛴ⃭Ẽ྾ࢆ⾜࠺ࡓࡵᾮ⭷⾲㠃ࡢ⁐ᾮ⃰ᗘࡣࡁࡃୗࡀࡾ㣬ᅽຊࡀࡁࡃୖࡀࡿ㸬 ࢫࣃࣛࣝ⟶ࡢࡼ࠺ᾮ⭷ࡀࡉࢀࢀࡤẼ྾ࡣࡑࡢᚋࡶ⥆ࡃࡀ,ᖹ⟶ࡢࡼ࠺ᾮ⭷ࡀ
ࢀࡎὶୗࡍࡿẼᾮ⭷ࡢᅽຊᕪࡀᑠࡉࡃ࡞ࡾ྾ᛂࡀ㕌ࡃ࡞ࡿ⪃࠼ࡽࢀࡿ㸬ࡑ ࡢ≧ែ࡛ὶ㔞ࡀቑຍࡍࡿࡇࡼࡾ༢ὶ㔞ᙜࡓࡾࡢẼ྾㔞ࡀᑠࡉࡃ࡞ࡿࡇ࡛≀㉁
⛣ືಀᩘࡀῶᑡࡋ࡚࠸ࡿ⪃࠼ࡽࢀࡿ㸬
⁐ᾮ⃰ᗘኚࣞࣀࣝࢬᩘࡢ㛵ಀ
ᅗ4-22ᅗ 4-23ࡑࢀࡒࢀẼ ᗘ20Υ࠾ࡼࡧ 60Υ࠾ࡅࡿࣞࣀࣝࢬᩘ⁐ᾮ⃰ᗘ ࡢ㛵ಀࢆ♧ࡍ㸬Ẽ ᗘࡸఏ⇕⟶ࡢᙧ≧ࡼࡽࡎࣞࣀࣝࢬᩘࡢቑຍక࠸⁐ᾮࡢ⃰ᗘᕪ ࡣῶᑡഴྥ࠶ࡿ㸬ὶ㔞ࡀ㧗ࡃ࡞ࡿ⃰ᗘᕪࡀᑠࡉࡃ࡞ࡿࡢࡣ༢ᾮ㔞ᙜࡓࡾࡢ྾㔞 ࡀᑠࡉࡃ࡞ࡿࡽࡔ⪃࠼ࡽࢀࡿ㸬ࡲࡓ㸪ࡕࡽࡢẼ ᗘ࠾࠸࡚ࡶࣞࣀࣝࢬᩘࡀప࠸
ሙྜࡣᖹ⟶ࢫࣃࣛࣝ⟶ࡼࡿ㐪࠸ࡣ࠶ࡲࡾぢࡽࢀ࡞ࡗࡓࡀ㸪ࣞࣀࣝࢬᩘࡀ㧗࠸
ሙྜࢫࣃࣛࣝ⟶ࡢ᪉ࡀᖹ⟶ࡼࡾࡶ⃰ᗘᕪࡀࡁ࠸⤖ᯝ࡞ࡗࡓ㸬ࡇࢀࡣᖹ⟶࡛ࡣᆶ
┤ὶୗࡍࡿᾮ⭷ࡀࢫࣃࣛࣝ⟶ࡢሙྜ⼺᪕≧ὶࢀ࡚࠸ࡃࡇ࡛㸪ᖹ⟶ẚ⁐ᾮࡀ ఏ⇕⟶ෆ␃ࡲࡗ࡚࠸ࡿ㛫ࡀ㛗ࡃ࡞ࡿࡇ࡛Ẽࢆ྾ࡍࡿ㛫ࡀ㛗ࡃ࡞ࡿࡓࡵࡔ⪃
࠼ࡽࢀࡿ㸬ࡲࡓࢫࣃࣛࣝ⟶࡛ࡣᾮ⭷ࡀࡉࢀࡿࡇࡼࡗ࡚྾ࡀಁ㐍ࡉࢀࡿࡇࡶ୍
ᅉ࡛࠶ࡿ⪃࠼ࡽࢀࡿ㸬
↓ḟඖᩚ⌮
4.4.1 㡯࡛♧ࡋࡓᾮ⭷⇕ఏ㐩ಀᩘࢆᘧ(4-24) ♧ࡍࢾࢭࣝࢺᩘ࡛↓ḟඖࡋࡓ㸬ࡇࡢࡁ ௦⾲㛗ࡉLfࡣจ⦰ᩘࡢ௦⾲㛗ࡉࢆྲྀࡾ㸪ᘧ(4-25)ࡢࡼ࠺ồࡵࡓ㸬
Nu=hfLfΤk (4-24)
Lf=ሺμ2Τρf2gሻ1 3Τ (4-25)
ᅗ4-24ࢫࣃࣛࣝ⟶ࢆ⏝࠸ࡓᐇ㦂ࡢࢾࢭࣝࢺᩘࣞࣀࣝࢬᩘࡢ㛵ಀࢆ♧ࡍ㸬
Ẽ ᗘࡢ㐪࠸ࡼࡗ࡚ࣞࣀࣝࢬᩘᑐࡍࡿࢾࢭࣝࢺᩘࡢ㛵ಀ࠾࠸࡚ഴࡁ㐪࠸ࡀ࡛
࡚ࡋࡲࡗ࡚࠸ࡿ㸬ࡑࡢࡓࡵ⁐ᾮࡢ⢓ᗘࡢᙳ㡪ࢆ⪃៖ࡍࡿࡓࡵࣉࣛࣥࢺࣝᩘࡢ㛵ಀᛶࡶ⪃
࠼ࡓ㸬ࣉࣛࣥࢺࣝᩘࢆ௨ୗࡢࡼ࠺ᐃ⩏ࡍࡿ㸬
Pr=μCpΤk (4-26)
ࡇࡇ࡛ȣ, Cp, kࡣᾮ⭷ࡢ⢓ᗘ,ẚ⇕,⇕ఏᑟಀᩘ࡛,ᩥ⊩(23)ࢆཧ⪃ࡋ࡚⟬ฟࡋࡓ㸬ࢾࢭࣝࢺᩘ
ࣉࣛࣥࢺࣝᩘࡢ㛵ಀࢆぢ࡚ࡳࡿNu҃Pr0.27࡛࠶ࡗࡓࡓࡵ㸪ᅗ4-24ࡢ⦪㍈Pr0.27ࢆ⪃៖
ࡋᶓ㍈ᾮ⭷ࡢࣞࣀࣝࢬᩘࢆྲྀࡗ࡚ᩚ⌮ࡋࡓ㸬ᅗ4-25ࢾࢭࣝࢺᩘࣉࣛࣥࢺࣝᩘ,ࣞ
ࣀࣝࢬᩘࡢ㛵ಀࢆ♧ࡍ㸬ᾮ⭷ࡢ⢓ᗘࢆ⪃៖ࡋࡓ⤖ᯝࢾࢭࣝࢺᩘࣞࣀࣝࢬᩘ┦㛵ᛶࡀ ぢࡽࢀࡓ㸬
ࡲࡓᮏᐇ㦂ࡼࡾࢫࣃࣛࣝ⟶࠾࠸࡚Ẽ྾ࢆక࠸࡞ࡀࡽὶୗࡍࡿ㝿ࡢᾮ⭷ఏ⇕⟶
ቨࡢ㛫࠾ࡅࡿ⇕ఏ㐩㛵ࡋ࡚௨ୗࡢᐇ㦂ᘧࢆᚓࡓ㸬
Nu=ͲǤͲͲͶͶRe0.79Pr0.27 (4-27)
ᮏ❶ࡢࡲࡵ
ࡇࢀࡲ࡛LiBr/Ỉ⣔྾ᘧࣄ࣮ࢺ࣏ࣥࣉࡼࡾ80Υࣞ࣋ࣝࡢ ᗫ⇕ࡽ120Υ௨ୖࡢ㧗
✵Ẽࢆ⏕ᡂࡍࡿࢩࢫࢸ࣒ࢆ㛤Ⓨࡋ࡚ࡁࡓ㸬ࡇࡢࣄ࣮ࢺ࣏ࣥࣉ࡛ࡣ㸪✵Ẽࡣ྾ჾෆࡢఏ⇕⟶
ࡢ㛫ࢆὶࢀ࡞ࡀࡽ┤᥋ຍ⇕ࡉࢀ྾ᾮࡣఏ⇕⟶ෆഃࢆᾮ⭷≧ὶࢀ࡚࠸ࡿ㸬ࡑࡢ㝿ᾮ⭷ࡢ ᗘࡣⓎჾࡽ㏦ࡽࢀࡿẼࢆ྾ࡍࡿࡇ࡛ୖ᪼ࡋ㸪ᾮ⭷✵Ẽࡢ⇕ࡣఏ⇕⟶ࢆ
㏻ࡋ࡚⾜ࢃࢀࡿ㸬ࡋࡋ྾ჾෆࡢࡇࡢࡼ࠺࡞⇕࣭≀㉁⛣ືࡢ࣓࢝ࢽࢬ࣒ࡸᾮ⭷✵Ẽࡢ㛫
࠾ࡅࡿ⥲ᣓ⇕ఏ㐩ಀᩘࢆồࡵࡿࡓࡵࡢ ᗘᕪࢆᐃ⩏ࡍࡿᚲせࡀ࠶ࡿࡀ㸪ࡑࡢ᪉ἲㄽࡣ᫂
☜ࡉࢀ࡚࠸࡞࠸㸬ࡑࡇ࡛ᮏ◊✲࡛ࡣὶ㔞0.1㹼0.7kg/min,྾ᾮ⃰ᗘ56㹼58%ࡢ⠊ᅖ࠾࠸
࡚㸪Ẽ ᗘ20Υ60Υࡢ2᮲௳࡛㸪ఏ⇕⟶ࡣ㖡〇ࢫࣃࣛࣝ༢⟶ᖹ⟶ࢆ⏝࠸࡚ఏ⇕
ヨ㦂ࢆ⾜࠸ఏ⇕⟶ࡢ⇕࣭≀㉁⛣ື≉ᛶࢆ◊✲࠾ࡼࡧẚ㍑ࢆ⾜ࡗࡓ㸬
㸯㸧ᾮ⭷⇕ఏ㐩ಀᩘ
࣭ࢫࣃࣛࣝ⟶࠾࠸࡚ὶ㔞ࡢቑຍక࠸ᾮ⭷⇕ఏ㐩ಀᩘࡶቑຍࡋ࡚࠸ࡗࡓ㸬
࣭ᖹ⟶࠾࠸࡚ὶ㔞ࡢቑຍక࠸ᾮ⭷⇕ఏ㐩ಀᩘࡣῶᑡࡋ࡚࠸ࡗࡓ㸬
࣭ᖹ⟶ẚࢫࣃࣛࣝ⟶ࡢ࠺ࡀ㧗࠸ఏ⇕ᛶ⬟ࢆ♧ࡋࡓ㸬 㸰㸧≀㉁⛣ືಀᩘ
࣭ࢫࣃࣛࣝ⟶࠾࠸࡚ὶ㔞ࡢቑຍక࠸≀㉁⛣ືಀᩘࡶቑຍࡋ࡚࠸ࡗࡓ㸬
࣭ᖹ⟶࠾࠸࡚Ẽ ᗘࡀప࠸ሙྜࡣὶ㔞ඹቑຍࡋ࡚࠸ࡃࡀ㸪Ẽ ᗘࡀ㧗࠸ሙྜὶ 㔞ࡢቑຍࡣᑐῶᑡࡋ࡚࠸ࡗࡓ㸬
㸱㸧⁐ᾮ⃰ᗘኚ
࣭ࢫࣃࣛࣝ⟶㸪ᖹ⟶ࡕࡽࡶὶ㔞ࡢቑຍక࠸⁐ᾮ⃰ᗘኚࡣᑠࡉࡃ࡞ࡗࡓ㸬
࣭ὶ㔞ࡀᑠࡉ࠸ሙྜࢫࣃࣛࣝ⟶ᖹ⟶࡛⃰ᗘᕪࡢ㐪࠸ࡣ࠶ࡲࡾぢࡽࢀ࡞ࡗࡓࡀὶ㔞 ࡀࡁ࠸ሙྜࢫࣃࣛࣝ⟶ࡢ࠺ࡀᖹ⟶ࡼࡾࡶ⃰ᗘᕪࡀࡁࡗࡓ㸬
㸲㸧↓ḟඖᩘᩚ⌮
࣭ᮏᐇ㦂⤖ᯝࡼࡾࢫࣃࣛࣝ⟶ࢆ⏝࠸ࡓሙྜࡢ⇕ఏ㐩ಀᩘ,ὶ㔞,⢓ᗘࡢ㛵ಀࡋ࡚௨ୗ♧
ࡍࡼ࠺࡞↓ḟඖᐇ㦂ᘧࢆ⟬ฟࡋࡓ㸬
Nu=ͲǤͲͲͶͶRe0.79Pr0.27
Fig.4-1(a) Experimental apparatus Fig.4-1(b) Schematic diagram of experimental apparatus
Fig.4-2Thermocouple installation position Fig.4-3 Structure of upper of equipment
Fig.4-4 Schematic diagram of structure of evaporator
Fig.4-5 Schematic diagram of lower reservoir
Fig.4-6(a) Schematic diagram of liquid film temperature distribution on inlet of heat transfer tube (vapor temp. 60°C)
Fig.4-6(b) Schematic diagram of liquid film temperature distribution on inlet of heat transfer tube (vapor temp. 20°C)
Fig.4-7(a) Temperature distribution map in whole spiral tube (vapor temp. 60°C)
Fig.4-7(b)㸦㸦left㸧Temperature distribution map on upper of spiral tube (vapor temp. 60°C) Fig.4-7(c)㸦right㸧Temperature distribution map of lower part of spiral tube (vapor temp. 60°C)
Fig.4-8(a) Temperature distribution map in whole smooth tube (vapor temp. 60°C)
Fig.4-8(b) (left㸧㸧Temperature distribution map on upper of smooth tube (vapor temp. 60°C) Fig.4-8(c)㸦right㸧 Temperature distribution map of lower part of smooth tube (vapor temp. 60°C)
Fig.4-9(a) Temperature distribution map in whole spiral tube (vapor temp. 20°C)
Fig.4-9(b) (left㸧㸧Temperature distribution map on upper of spiral tube (vapor temp. 20°C)㸧 Fig.4-9(c) (right㸧Temperature distribution map of lower part of spiral tube (vapor temp. 20°C)
Fig.4-10(a) Temperature distribution map in whole smooth tube (vapor temp. 20°C)
Fig.4-10(b) (left㸧㸧Temperature distribution map on upper of smooth tube (vapor temp. 20°C) Fig.4-10(c) (right㸧Temperature distribution map of lower part of smooth tube (vapor temp. 20°C)
Fig.4-10(d) Temperature distribution map on upperpart expansion of smooth tube (vapor temp. 20°C)
Fig.4-11 Changes of each part temperature and differential pressure with time (example)
Fig.4-12 Measurement point of temperature and differential pressure
Fig.4-13 Flow chart of the calculation algorithm
Fig.4-14 Schematic diagram of heat transfer model on steam absorption in absorber
Fig.4-15 Schematic diagram of heat and mass transfer model in absorber
Fig.4-16 Relationship of solution film convective heat transfer coefficient and Reynolds number (vapor temp. 20°C)
Fig.4-17 Relationship of solution film convective heat transfer coefficient and Reynolds number (vapor temp. 60°C)
100 1000 10000
10 100 1000
Convective heat transfer coefficient [W/m2࣭K]
Re [-]
spiral tube smooth tube
100 1000 10000
10 100 1000
Convective heat transfer coefficient[W/m2࣭K]
Re [-]
spiral tube smooth tube
Fig.4-18 Relationship of gas-side mass transfer coefficient and Reynolds number (vapor temp. 20°C)
Fig.4-19 Relationship of gas-side mass transfer coefficient and Reynolds number (vapor temp. 60°C)
1.0E-07 1.0E-06 1.0E-05
10 100 1000
Mass-transfer coefficient [kg/(s㺃m2㺃Pa)]
Re [-]
spiral tube smooth tube
1.0E-07 1.0E-06 1.0E-05
10 100 1000
Mass-transfer coefficient [kg/(s㺃m2㺃Pa)]
Re [-]
spiral tube
Fig.4-20 Relationship of solution-side mass transfer coefficient and Reynolds number (vapor temp. 20°C)
Fig.4-21 Relationship of solution-side mass transfer coefficient and Reynolds number (vapor temp. 60°C)
1.0E-08 1.0E-07 1.0E-06
10 100 1000
Mass-transfer coefficient [m/s]
Re [-]
spiral tube
1.0E-08 1.0E-07 1.0E-06 1.0E-05
10 100 1000
Mass-transfer coefficient [m/s]
Re [-]
spiral tube smooth tube
Fig.4-22 Relationship of concentration difference and Reynolds number (vapor temp. 20°C)
Fig.4-23 Relationship of concentration difference and Reynolds number (vapor temp. 60°C㸧 0.1
1 10
10 100 1000
Concentration difference [%]
Re [-]
spiral tube smooth tube
1 10 100
10 100 1000
Concentration difference [%]
Re [-]
spiral tube smooth tube
Fig.4-24 Relationship of Nusselt number and Reynolds number (Spiral tube)
Fig.4-25 Relationship of Nusselt number, Prandtl number and Reynolds number (Spiral tube) 0.01
0.1 1
10 100 1000
Nu [-]
Re [-]
vapor temperature 60Υ vapor temperature 20Υ
0.01 0.1 1
10 100 1000
Nu ࣭ Pr
-0.27[-]
Re[-]
グ グྕ
A = equivalent heat transfer area of the tube outside wall to a smooth tube [m2] A’ = equivalent heat transfer area of the tube inside wall to a smooth tube [m2]
g = gravitational acceleration [m/s2]
G = mass flow rate [kg/s]
= mass flow rate of falling liquid per perimeter [kg/m㺃s]
m=Vapor absorption amount [kg]
ha = convection heat transfer coefficient on the outside of tube [W/m2㺃K]
hf = solution film convective heat transfer coefficient [W/m2㺃K]
U = overall heat transfer coefficient [W/m2㺃K]
k = thermal conductivity of solution [W/m㺃K]
βg= gas-side mass transfer coefficient [kg/s㺃m2㺃Pa]
βc= solution-side mass transfer coefficient [m/s]
l = length of the heat transfer tube [m]
Lf= characteristic length [m]
Q= enthalpy through the heat exchanger tubes [J]
qf = enthalpy of solution [J/kg]
r = inner radius of the heat transfer tube [m]
Tf = solution temperature [K]
Ts = wall temperature [K]
Ta = atmospheric temperature [K]
P= pressure [Pa]
= viscosity of solution [Pa㺃s]
f= solutiuon density [kg/m3]
X= solution concentration [LiBr wt %]
Xe=measured solution concentration at the end of the experiment [LiBr wt %]
f=solution concentration [H2O wt %]
=average solution concentration [H2O wt %]
Cp=specific heat of LiBr solution [J/kg࣭K]
↓↓ḟඖᩘ
Nu = Nusselt number [-]
Re = Reynolds number [-]
Pr = Prandtl number [-]
ῧᏐ 1=upper part 2=lower part i=minute time
➨
➨㸳❶ 㐣㣬ᚤ⣽⤖ᬗࢫ࣮ࣛࣜࡼࡿ AHP ࡢᛶ⬟ྥୖຠᯝ
ᖜ࡞Ⅳ㓟࢞ࢫฟ๐ῶࢆᅗࡿୖ࡛㸪ᖜᗈ࠸ศ㔝࡛ᮍ⏝࡛࠶ࡗࡓప࢚ࣞ࣋ࣝࢿࣝࢠ࣮
ᅇࡀྍḞ࡞ࡗ࡚࠸ࡿ㸬྾ᘧࣄ࣮ࢺ࣏ࣥࣉࡣ㸪⇕㥑ືᆺࡢ෭ᶵࡋ࡚ࡍ࡛ከࡃࡢ ᐇ⏝ࡀᅗࡽࢀ㸪ၟ⏝ჾࡋ࡚ᕷ㈍⮳ࡗ࡚࠸ࡿ㸬ࡇࡢࡼ࠺࡞྾ᘧࣄ࣮ࢺ࣏ࣥࣉࢆ࡛ࡁࡿ
ࡔࡅప ᗫ⇕࡛ࡶຠ⋡ࡼࡃ㥑ືࡍࡿࡼ࠺㸪ࡉࡽ࡞ࡿ㧗ᛶ⬟ᢏ⾡ࢆ㛤Ⓨࡍࡿࡇࡣ㸪▷ᮇⓗ
┬࢚ࢿࣝࢠ࣮ຠᯝࢆྥୖࡉࡏࡿࡓࡵࡶ㔜せㄢ㢟࡛࠶ࡿ㸬
྾ᘧࣄ࣮ࢺ࣏ࣥࣉࡣ㸪྾ᾮసືὶయࡢ࠸ࡃࡘࡢ⤌ྜࢃࡏࡀᥦࡉࢀ࡚࠸ࡿࡀ㸪
ࣥࣔࢽ࣭Ỉ⣔ࡲࡓࡣ⮯ࣜࢳ࣒࣭࢘Ỉ⣔ࡀ୍⯡ࡼࡃ⏝࠸ࡽࢀ࡚࠸ࡿ(9)(10)㸬ࣥࣔࢽ࣭
Ỉ⣔྾ᘧࣄ࣮ࢺ࣏ࣥࣉࡣ㸪ẚ㍑ⓗప ᗫ⇕ࡢ⏝ྥ࠸࡚࠸ࡿࡀ㸪ࡑࡢ㧗ᛶ⬟ࡣỈ
ࣥࣔࢽࢆศ㞳ࡍࡿ⏕ჾ㒊ศࡢ␃ᛶ⬟ࡁࡃ౫Ꮡࡋ࡚࠸ࡿ㸬୍᪉㸪⌧Ⅼ࡛ᐇ⏝ࡉ
ࢀ࡚࠸ࡿᚋ⪅ࡢ⮯ࣜࢳ࣒࣭࢘Ỉ⣔྾ᘧࣄ࣮ࢺ࣏ࣥࣉࡢ⇕※ࡣ㸪100 °C ࣞ࣋ࣝ௨ୗࡢ ప ᗫ⇕ࢆ⏝ࡍࡿࢱࣉࡣࡲࡔᑡ࡞ࡃ㸪ࢇࡣ⇞ᩱࡢ⇞↝ࡼࡿ㧗 ࢞ࢫࡀ⏕ჾ
⇕※⏝ࡉࢀ࡚࠸ࡿ㸬ࡇࡢࡼ࠺࡞ࣞ࣋ࣝࡢప ᗫ⇕⏝ᆺ⮯ࣜࢳ࣒࣭࢘Ỉ⣔྾ᘧࣄ࣮
ࢺ࣏ࣥࣉࡢ⏝ᣑࢆᅗࡿୖ࡛㸪⏕ჾࡢ⇕ᛶ⬟྾ᾮࡢ྾‵ᛶࢵࣉࡀせồࡉࢀ
ࡿ㸬
྾ᾮᛶ⬟㛵ࡋ࡚ࡣ㸪ỈẼ྾క࠸྾ᾮࡀᕼ㔘ࡉࢀᖹ⾮Ẽᅽࡀ㧗ࡃ࡞ࡾ㸪྾‵
ᛶࡀపୗࡍࡿࡇࡀ㸪྾ჾᛶ⬟పῶࡢせᅉ࡞ࡿ㸬ࡇࡢࡓࡵ㸪⮯ࣜࢳ࣒࣭࢘Ỉ⣔྾ᾮ
➨ 3 ᡂศࢆῧຍࡋ࡚ΰྜࡉࡏࡿࡇࡼࡾ㸪྾‵ᛶቑࡸẼ྾క࠺ᕼ㔘⇕ప ῶࢆᅗࡿ◊✲ࡀ⾜ࢃࢀ࡚࠸ࡿ(11)(12)(13)(14)(15) 㸬
ࡇࢀࡽᑐࡋ࡚ Itaya et al. (2010) ࡣ㸪྾ᾮ྾╔ᚤ⢏Ꮚࢆศᩓࡋࡓࢫ࣮ࣛࣜࢆ྾
ᾮ⏝ࡍࡿ᪉ᘧࢆᥦࡋࡓ(16)㸬྾ᾮ྾╔ࢆศᩓࡋࡓሙྜ㸪⁐㉁࡛࠶ࡿLiBrࡀ྾╔
྾⬺╔ࡍࡿຠᯝࡼࡾ㸪Ẽ྾క࠺⁐ᾮ⃰ᗘపῶక࠺྾‵ᛶ⬟పୗࢆᢚไ࡛ࡁ
ࡿࡇࢆሗ࿌ࡋࡓ㸬ⴭ⪅ࡽࡣ㸪ࡇࡢࡼ࠺࡞᪉ᘧࢆ᳨ウࡍࡿ㐣⛬࡛㸪྾ᾮࡀ㐣㣬㐩ࡍࡿ
྾╔ࡀ⤖ᬗ᰾ࡢࡼ࠺࡞స⏝࡛㸪ᚤ⣽࡞LiBr⤖ᬗࡀᯒฟࡍࡿࡇࢆぢฟࡋࡓ㸬ࡇࡢ㐣㣬
ᚤ⣽⤖ᬗࢫ࣮ࣛࣜࢆ⏝ࡍࡿ㸪྾㐣⛬࠾࠸࡚ࡇࡢ⤖ᬗࡢ⁐ゎ࡛྾╔ࡢ྾⬺╔ຠ
ᯝ௨ୖࡢᕼ㔘పῶຠᯝࡀᚓࡽࢀࡿ⪃࠼ࡽࢀࡿ㸬
㐣㣬⁐ᾮࡣ㸪⤖ᬗ᰾ࡀ࡞ࡅࢀࡤ⤖ᬗ⏕ᡂࡋ࡞࠸‽Ᏻᐃ㡿ᇦࡢᏑᅾࡀ▱ࡽࢀ࡚࠸ࡿ㸬ࡇ
ࢀࡣ⁐ゎᗘ᭤⥺௨ୖࡘ㐣⁐ゎᗘ᭤⥺௨ୗࡢ㡿ᇦ࠶ࡿ㸬ࡇࢀࡲ࡛㸪ప㐣㣬⁐ᾮࡢ⤖ᬗ⏕
ᡂ᪉ἲࡀ࠸ࡃࡘᥦࡉࢀ࡚࠸ࡿ㸬࠼ࡤ㸪㏻ᖖ࡛ࡣ᰾Ⓨ⏕ࡋ࡞࠸ప㐣㣬⁐ᾮ㸪✀⤖ᬗ
ࢆῧຍࡋ࡚⤖ᬗᡂ㛗ࡉࡏࡿ᪉ἲ㸦17㸧㸪㉸㡢Ἴࡸ࣮ࣞࢨ࣮ࢆ↷ᑕࡍࡿࡇࡼࡾ⤖ᬗ᰾ࢆㄏⓎ
ࡍࡿ◊✲(18)(19)(20)࡞ࡀぢཷࡅࡽࢀ㸪㐺ษ࡞᮲௳࡛᧯సࡍࡿࡇ࡛㸪ప㐣㣬⁐ᾮࡽࡶ⤖
ᬗ᰾ࡀⓎ⏕ࡍࡿࡇࡀሗ࿌ࡉࢀ࡚࠸ࡿ㸬
୍᪉㸪྾ᾮ୰྾╔ࢆศᩓࡋࡓሙྜࡣ㸪⣽Ꮝෆ⮯ࣜࢳ࣒࢘ࡀᚤ⣽࡞⤖ᬗ≧ែ࡛
྾╔ࡉࢀࡿ⪃࠼ࡽࢀ㸪ࡇࢀࡀ⤖ᬗ᰾࡞ࡾᾮ┦ࡀ‽Ᏻᐃ㡿ᇦ࡛ࡶ྾╔࿘ࡾ⤖ᬗᡂ㛗 ࡀ⏕ࡌࡿ⪃࠼ࡽࢀࡿ㸬ᐇ㝿྾╔ࢆῧຍࡋ࡞࠸ሙྜࡣ㸪㧗㐣㣬≧ែ㐩ࡋ࡚ึࡵ࡚
ᛴ㏿⤖ᬗᡂ㛗ࡍࡿࡓࡵ㸪ࡁ࡞⤖ᬗࡀ⏕ᡂࡍࡿ㸬྾╔⢏Ꮚ᭷↓ࡼࡿLiBr㐣㣬⤖ᬗ
ࢆᅗᅗ5-1♧ࡍ㸬
ᮏ❶࡛ࡣ㸪 LiBr-H2O⣔྾ᾮ྾╔ᚤ⢏Ꮚࢆศᩓࡉࡏࡿࡇࡼࡾ⏕ᡂࡍࡿᚤ⣽࡞㐣 㣬⤖ᬗࢫ࣮ࣛࣜࡢ≉ᛶࢆ᫂ࡽࡍࡿࡓࡵ㸪ࡲࡎᚤ⣽⤖ᬗࡢ⢏ᗘศᕸ࠾ࡼࡧ⤖ᬗࢫࣛ
࣮ࣜࡢ⢓ᗘ➼ࡢ≀ᛶィ ࢆ⾜࠺㸬ࡲࡓ㸪ࡇࡢࡼ࠺࡞ࢫ࣮ࣛࣜࢆ྾ᘧࣄ࣮ࢺ࣏ࣥࣉᛂ⏝ࡍ
ࡿ࠺࠼࡛㸪㔜せ࡞せᅉ࡞ࡿఏ⇕ᛶ⬟ࡘ࠸࡚ᾮ⭷ఏ⇕ᐇ㦂ࢆ⾜࠺ࡶ㸪LiBr ⤖ᬗࡢ
⁐ゎຠᯝࡼࡿ྾ᾮ⃰ᗘኚࡢᢚไ࡞ࡽࡧỈẼ྾ᛶ⬟పୗᢚไຠᯝࢆ㸪⇕࣭≀㉁⛣
ືࣔࢹࣝゎᯒᇶ࡙ࡁᇶ♏ⓗほⅬࡽᐃ㔞ⓗホ౯ࢆ⾜࠺㸬
ᐇ㦂᪉ἲ
⤖ᬗࢫ࣮ࣛࣜ≀ᛶ ᐃ
㏻ᖖࡢ྾ᾮ࡛࠶ࡿ྾╔ࢆศᩓࡉࡏ࡚࠸࡞࠸LiBr⁐ᾮࡀ㐣㣬≧ែ࡞ࡿ㸯ࡘࡢ
ࡁ࡞ᅛࡲࡾ࡞ࡿࡼ࠺⤖ᬗࡀᯒฟࡍࡿࡓࡵ㸪ὶ㊰ࡢ㛢ሰక࠺ࢺࣛࣈࣝࡀⓎ⏕ࡍࡿ⪃
࠼ࡽࢀࡿ㸬ࡋࡋ㸪྾╔ᚤ⢏Ꮚࢆศᩓࡉࡏࡿࡇ࡛྾╔ࡀ⤖ᬗ᰾࡞ࡾከᩘࡢᚤ⣽࡞⤖
ᬗࡀᯒฟࡋࢫ࣮ࣛࣜ≧ែ࡞ࡿ㸬ࡑࡇ࡛㸪ὶ㊰ࡢὶࢀᙳ㡪ࢆ࠼ࡿ⪃࠼ࡽࢀࡿ⤖ᬗࢫࣛ
࣮ࣜࡢ⤖ᬗ⢏ᗘศᕸཬࡧ⢓ᗘࡢ ᐃࢆ⾜ࡗࡓ㸬
ᚤ⣽⤖ᬗ⢏ᗘศᕸ ᐃ ᐃ⨨ࡋ࡚㸪࣮ࣞࢨ࣮ᅇᢡ/ᩓᘧ⢏ᗘศᕸ ᐃ
⨨㸦ᇼሙ㸪LA-920ᆺ㸧ࢆ⏝ࡋࡓ㸬྾╔ࡣᮾࢯ࣮〇ࢮ࢜ࣛࢺHSZ-320-NAAࢆ⏝
ࡋࡓ㸬⤖ᬗࢫ࣮ࣛࣜࡣ㧗 ≧ែ㸦80 °C㸧࡛LiBr⃰ᗘ63.4 wt%㸦⁐ᾮᇶ‽㸧ࡢLiBr⁐ᾮ
ࢮ࢜ࣛࢺ5.56 wt%ࢆศᩓࡉࡏ㸪 ᗘࢆ25 °Cࡲ࡛ୗࡆࡿࡇ࡛సᡂࡋࡓ㸬ࡇࡢ⤖ᬗࢫࣛࣜ
࣮୰ࡢᚤ⣽⤖ᬗࢮ࢜ࣛࢺ⢏Ꮚࡢ⢏ᗘศᕸࢆ⢏ᗘศᕸ ᐃ⨨ࡢࣂࢵࢳᘧࢭ࡛ࣝ ᐃࡋ ࡓ㸬ࡲࡓ㸪 ᐃ୰ࡢ ᗘࡶ25.0 °Cࡋࡓ㸬࡞࠾㸪 ᅗ5-1ࡣୖグྠ᮲௳࡛ㄪ〇ࡋࡓࢫࣛ
࣮ࣜ⤖ᬗᡂ㛗≧ែࢆ♧ࡋ࡚࠸ࡿ㸬
⤖ᬗࢫ࣮ࣛࣜ⢓ᗘ ᐃ ᐃ⨨ࡋ࡚㸪ᅇ㌿⢓ᗘィࢆ⏝ࡋࡓ㸬⤖ᬗࢫࣛࣜ
࣮ࡢ⢏ᗘศᕸ ᐃྠ᮲௳㸦LiBr⃰ᗘ63.4 %ࠊࢮ࢜ࣛࢺศᩓ⃰ᗘ5.56 %㸧࡛ࢫ࣮ࣛࣜࢆ
ㄪ〇ࡋࡓ㸬ࡇࡢ⤖ᬗࢫ࣮ࣛࣜࡢ ᗘࢆ20㸪35㸪50 °Cኚࡉࡏࡿࡇ࡛⤖ᬗࢫ࣮ࣛࣜ୰ࡢ ᅛయ⤖ᬗ㔞ࢆኚ࠼㸪⢓ᗘ ᐃࢆ⾜ࡗࡓ㸬
ᾮ⭷ఏ⇕ᐇ㦂᪉ἲ
྾ᘧࣄ࣮ࢺ࣏ࣥࣉࡢᛶ⬟ホ౯ࢆ⾜࠺ୖ࡛㸪྾ᾮ⇕፹య㛫ࡢ⇕ఏ㐩ಀᩘࢆ᫂ࡽ
ࡋ࡚࠾ࡃᚲせࡀ࠶ࡿ㸬ᮏ◊✲࡛ࡣ㸪⏕ჾࡋ࡚᧯సࡋࡓሙྜࢆᐃࡋ㸪༢୍ࣉ࣮ࣞࢺ⾲㠃
ࢆὶୗࡍࡿ྾╔ศᩓ྾ᾮ⇕፹య㛫ࡢ⥲ᣓ⇕ఏ㐩ಀᩘࢆィ ࡋ㸪྾╔ࡀ⥲ᣓ⇕ఏ㐩 ಀᩘ࠼ࡿᙳ㡪ࡘ࠸᳨࡚ウࢆ⾜ࡗࡓ㸬
ᅗᅗ5-2ᾮ⭷ఏ⇕ᐇ㦂⨨ᴫ␎ᅗࢆ♧ࡍ㸬྾ᾮࡣୖ㒊ᐜჾࡽఏ⇕ᐇ㦂ࢲࢡࢺࡢఏ⇕ࣉ
࣮ࣞࢺ⾲㠃ᐃ㔞౪⤥ࡉࢀ㸪ᾮ⭷≧ែ࡛ὶୗࡉࡏࡿ㸬ࢲࢡࢺฟཱྀࡽࡢ྾ᾮࡣୗ㒊ᐜჾ
㈓ࡵࡽࢀࡿ㸬྾ᾮࡣ྾╔ศᩓLiBr⁐ᾮࢆ⏝࠸ࡓ㸬྾╔ࡣᮾࢯ࣮〇ࢮ࢜ࣛࢺ
HSZ-320-NAAࢆ⏝㸬୍᪉㸪⇕፹యࡣࢩࣜࢥࣥ࢜ࣝ㸦ಙ㉺Ꮫ〇 KF-96-100CS㸧ࢆ⏝࠸㸪
୍ᐃࡢ ᗘຍ⇕ࡉࢀࡓ࢜ࣝࢆࢲࢡࢺୗ㒊ഃࡽ౪⤥ࡋ㸪྾ᾮ⭷ࡢὶࢀ᪉ྥࡣྥὶ ᪉ᘧࡋࡓ㸬ࡲࡓ㸪ࡑࡢ㛫ࡢఏ⇕ࣉ࣮ࣞࢺࡣSUS329J4Lࢫࢸࣥࣞࢫᯈ㸦㛗ࡉ1008 mm㸪
ᖜ102 mm㸪ཌࡉ3 mm㸧ࢆ⏝ࡋ㸪྾ᾮഃ⾲㠃ࡣᆒ୍ᾮ⭷ࡢᙧᡂࢆᐜ᫆ࡉࡏࡿࡓࡵ
ぶỈᛶฎ⌮㸦㸦ᰴ㸧ఙࡼࡿ࣋ࣛࢫࢥ࣮ࢺຍᕤ㸧ࡀࡉࢀ࡚࠸ࡿ㸬⣔యࢆῶᅽୗࡋ㸪
ࢲࢡࢺࢆ4.57°ഴᩳࡉࡏࡓᾮ⭷ὶࢀ࡛ఏ⇕ᐇ㦂ࢆ⾜ࡗࡓ㸬
ᐇ㦂ᡭ㡰ࡣ㸪௨ୗࡢ㏻ࡾ࡛࠶ࡿ㸬
㸯㸬ᡤᐃࡢ ᗘタᐃࡉࢀࡓࢩࣜࢥࣥ࢜ࣝࢆఏ⇕ᐇ㦂ࢲࢡࢺࡢ⇕፹యഃὶ㏻ࡉࡏ࡚㸪
⇕ⓗᏳᐃࡍࡿࡲ࡛ᚅᶵࡍࡿ㸬ࡇࡇ࡛ࡣ㸪ᜏ ᵴෆࢩࣜࢥࣥ࢜ࣝ ᗘࢆ90 °C ୍࡛ᐃ
ࡋࡓ㸬
㸰㸬ఏ⇕ᐇ㦂ࢲࢡࢺ྾ᾮ⭷ഃ㸪ୖ㒊ᐜჾ㸪ୗ㒊ᐜჾ㸪จ⦰ჾ㸪จ⦰Ỉᐜჾࢆ┿✵࣏ࣥࣉ
࡛ῶᅽࡉࡏࡿ㸬
㸱㸬྾ᾮ㈓ⶶ⏝ࡢୖ㒊ᐜჾࡽࢲࣖࣇ࣒ࣛᘧᐃ㔞࣏ࣥࣉ࡛ὶ㔞ࢆㄪ⠇ࡋࡘࡘ྾ᾮ
ࢆヨ㦂ࢲࢡࢺ౪⤥ࡋ㸪ఏ⇕㠃ᾮ⭷≧ὶ㏻ࡉࡏࡿ㸬
㸲㸬྾ᾮࡢฟධཱྀ ᗘࡀᏳᐃࡋࡓࡽ㸪྾ᾮฟධཱྀ ᗘLiBr⃰ᗘ㸪ࢩࣜࢥࣥ࢜ࣝฟ ධཱྀ ᗘࢆ ᐃࡍࡿ㸬
㸳㸬྾ᾮࡢLiBr⃰ᗘࡣ㸪ᾮࡢ୍㒊ࢆ200 °Cࡢ⇱ᶵෆ࡛⇱ࡉࡏ㸪LiBrࡢ㉁㔞ࡶ
ࡢ⁐ᾮ㉁㔞ࡽỴᐃࡍࡿ㸬
྾ᾮ࡛࠶ࡿLiBr⁐ᾮࡢὶ㔞࠾ࡼࡧ྾╔⃰ᗘࢆኚࡉࡏ㸪 ᐃࡋࡓ྾ᾮࡢฟධཱྀ
ᗘLiBr⃰ᗘ㸪ࢩࣜࢥࣥ࢜ࣝฟධཱྀ ᗘࡽ⥲ᣓ⇕ఏ㐩ಀᩘࢆ⟬ฟࡋࡓ㸬ࡓࡔࡋ㸪྾╔
⃰ᗘࡣ2.66㸪4.04㸪4.99㸪9.90 wt%ࡋࡓ㸬ࡲࡓ㸪྾ᾮࡢධཱྀLiBr⃰ᗘࡣ54.8ࠥ58.0 %
࡛㸪ࡇࡇ࡛ࡣ࠸ࡎࢀࡶ㐣㣬⃰ᗘ௨ୗࡋࡓ㸬ࡇࢀࡣ㸪 ⇕⏝ࡢࣄ࣮ࢺ࣏ࣥࣉ࡛ࡣ྾
ᾮࡢ⏕㐣⛬ࡢఏ⇕ಁ㐍ࡶࡁ࡞ㄢ㢟࡞ࡿࡇ㸪80 °C⛬ᗘࡢ⏕ ᗘ࡛ࡣ LiBr ࡢ⁐
ゎᗘࡀ㧗ࡃ㸪ᚤ⣽⤖ᬗࡢࢇࡀ⁐ゎࡍࡿࡇࡽ㸪㐣㣬⃰ᗘ௨ୗࡢ྾╔ศᩓ⣔྾
ᾮࡘ࠸࡚ఏ⇕≉ᛶࡢィ ࢆ⾜ࡗࡓࡓࡵ࡛࠶ࡿ㸬
⌮ㄽゎᯒ
྾ᘧࣄ࣮ࢺ࣏ࣥࣉ࠾ࡅࡿ⤖ᬗࢫ࣮ࣛࣜࡢᛶ⬟ྥୖຠᯝ㸪ࡍ࡞ࢃࡕỈẼ྾㔞ྥୖ
ຠᯝࡘ࠸࡚⌮ㄽゎᯒࡼࡿ᳨ウࢆ⾜ࡗࡓ㸬ᅗ5-3ࡣ྾ჾࢆࡋࡓሙྜࡢゎᯒࣔࢹࣝࢆᅗ
♧ࡋࡓࡶࡢ࡛㸪⇕ჾࡢఏ⇕㠃ࢆᣳࢇ࡛㸪྾ᾮࡀᾮ⭷≧࡛㸪⇕፹యࡀὶ㊰యࢆὶ㏻ࡍ
ࡿࡋࡓ㸬⏕ჾ࡛ࡣ㸪෭༷⏝⇕፹యࡢ௦ࢃࡾຍ⇕⏝⇕፹యࡀὶ㏻ࡋ㸪ỈẼࡢ྾௦
ࢃࡾⓎࡋ࡚⇕࣭≀㉁⛣ື᪉ྥࡀ㏫㸦㈇㸧᪉ྥ࡞ࡿⅬࡀ␗࡞ࡿࡔࡅ࡛㸪ࡃྠᵝ⾲グࡍ
ࡿࡇࡀ࡛ࡁࡿ㸬ࡲࡓ㸪ゎᯒࡣ௨ୗࡢ௬ᐃࢆ࠾ࡃ㸬 1㸧 ྾ჾཬࡧ⏕ჾࡣᆶ┤᪉ྥὶ㏻ࡍࡿ⇕᪉ᘧ㸬 2㸧 ྾ᾮࡣ⇕ჾఏ⇕㠃⾲㠃ࢆ୍ᵝ࡞ཌࡉࡢᾮ⭷࡛ὶୗ㸬 3㸧ᾮ⭷ཌࡉ᪉ྥࡢὶ㏿㸪 ᗘཬࡧ⃰ᗘศᕸࡣ୍ᵝ㸬
4㸧ᾮ⭷⾲㠃ࡢẼᅽࡣᾮ⭷ࡢ⃰ᗘ ᗘᑐࡍࡿ྾ᾮࡢ㣬Ẽᅽ㸬
5㸧 ᾮ⭷⾲㠃࡛ࡢỈศࡢⓎࡲࡓࡣ྾㏿ᗘࡣ㸪ᾮ⭷≧㠃ࡢẼᅽจ⦰ჾࡲࡓࡣⓎჾෆ
Ẽᅽࡢᕪࢆ᥎㐍ຊࡍࡿ≀㉁⛣ື࡛࠼ࡽࢀࡿ㸬
6㸧 Ⓨჾཬࡧจ⦰ჾෆẼᅽࡣࡑࢀࡒࢀࡢ ᗘ࠾ࡅࡿ⣧Ỉࡢ㣬Ẽᅽ࡛㏆ఝ㸬 7㸧 ෭༷ࡲࡓࡣຍ⇕ࡢࡓࡵࡢ⇕፹యࡣᾮ⭷ࡢὶୗ᪉ྥᑐࡋ࡚ྥὶࡲࡓࡣ୪ὶ࡛ὶ㏻㸬 8㸧ఏ⇕ࡣ⇕፹యᾮ⭷㛫ࡢ ᗘᕪࢆ᥎㐍ຊࡍࡿ⥲ᣓ⇕ఏ㐩࡛࠼ࡽࢀࡿ㸬
9㸧 ྾ᾮ⤖ᬗࢫ࣮ࣛࣜࢆ⏝࠸ࡿሙྜ㸪ỈẼ྾క࠸ LiBr ⤖ᬗࡀ⁐ゎࡍࡿࡓࡵ྾
ᾮ⃰ᗘࡣᖖ㣬⃰ᗘ୍࡛ᐃࡋ㸪⁐ゎ㏿ᗘࡶ༑ศ㏿࠸㸬
10㸧 ྾ᾮࡢ ᗘ࠾ࡅࡿ㣬⃰ᗘ௨ୖ࡞ࡿ⤖ᬗࡀᯒฟࡋ㸪྾ᾮ⃰ᗘࡣ㣬⃰ᗘ㸬 11㸧 ࿘ᅖࡢᨺ⇕㔞ࡣ↓どᑠ㸬
12㸧྾ᾮ⭷ཬࡧ⇕፹యࡢὶࢀ᪉ྥࡢఏ⇕ࡣ↓どᑠ㸬 13㸧྾ᾮ୰ࡢ྾╔ࡢLiBr྾╔⇕ࡣ↓どᑠ㸬
௬ᐃ 3)࡛ࡣࣆࢫࢺࣥὶࢀࡲࡓࡣᾮ⭷ཌࡉ᪉ྥࡢΰྜὶࢀࢆ௬ᐃࡋ㸪ࡇࡇ࡛ࡣࣔࢹࣝ
ࡢ⡆᫆ࡢࡓࡵ㐠ື᪉⛬ᘧࡣ⪃៖ࡋ࡚࠸࡞࠸ࡀ㸪⌮ㄽⓗ᭱ຠ⋡ࢆゎᯒࡍࡿࣔࢹࣝ࡞
ࡿ㸬ࡲࡓ㸪ᐇ⌧㇟ࡢ⿵ṇࡣ㸪௬ᐃ5)ࡢ≀㉁⛣ືಀᩘࢆࣇࢵࢸࣥࢢࣃ࣓࣮ࣛࢱࡍࡿࡇ
࡛ᑐᛂࡀྍ⬟⪃࠼ࡽࢀࡿ㸬ࡲࡓ㸪௬ᐃ6)ࡣ᧯స୰ࡢ྾ᾮ࣑ࢫࢺࡢΰධࡣ↓どᑠࡋ㸪 ỈẼ⛣ືᢠࡣỈẼὶ㊰ࡀᚊ㏿ࡍࡿⓎჾจ⦰ჾෆࡣࡑࢀࡒࢀࡢ ᗘ࠾ࡅࡿ
⣧Ỉࡢ㣬Ẽᅽ➼ࡋ࠸௬ᐃ࡛ࡁࡿ㸬
௨ୖࡢ௬ᐃᇶ࡙ࡁ㸪ࡑࢀࡒࢀࡢ⇕ཬࡧ≀㉁ᨭᘧࡣ㸪௨ୗࡢ㏻ࡾ࠼ࡽࢀࡿ㸬
LiBrᨭ
dA wC d dA
wc d ad LiBr 㸦5-1㸧
Ỉᨭ
dA m C w
d 1 LiBr
㸦5-2㸧
࢚ࢿࣝࢠ࣮ᨭ
w cond ad
c LiBr c
pa
s q q
dA
T w c T w c w h
d 㸦5-3㸧
ࡇࡇ࡛㸪wcࡣ྾ᾮ୰ࡢ྾╔㉁㔞ὶ㔞 [kg-adsorbent/s]㸪 adࡣ྾╔⾲㠃ࡢ LiBr ⤖ᬗ㔞 [kg-LiBr/kg-adsorbent]㸪Aࡣఏ⇕㠃✚ [m2]㸪wࡣ྾ᾮὶ㔞 [kg-solution/s]㸪CLiBrࡣ྾ᾮ୰
ࡢ LiBr⃰ᗘ [kg-LiBr/kg-solution]㸪mࡣỈẼ྾㏿ᗘ [kg-water/(m2·s)]㸪hsࡣ྾ᾮ࢚ࣥ
ࢱࣝࣆ࣮ [J/kg-solution]㸪cpacLiBrࡣࡑࢀࡒࢀ྾╔LiBrࡢẚ⇕[J/(kg·K)]㸪Tࡣ ᗘ [K]㸪 qcondࡣ┦ኚక࠺₯⇕࢚ࣥࢱࣝࣆ࣮[W/m2]㸪qwࡣ⇕፹య྾ᾮ㛫ࡢ⇕ఏ㐩㏿ᗘ [W/m2]
ࢆ⾲ࡍ㸬
⇕ཬࡧ≀㉁㏿ᗘᘧࡣ㸪ࡑࢀࡒࢀḟᘧ࡛⾲ࡏࡿ㸬
⇕ఏ㐩㏿ᗘ
w w
w h T T
q 㸦5-4㸧
ỈẼ྾㏿ᗘ
s evap
m p p
k
m 㸦5-5㸧
ࡇࡇ࡛㸪hwࡣ⥲ᣓ⇕ఏ㐩ಀᩘ [W/(m2·K)]㸪Tࡣ྾ᾮ ᗘ [K]㸪Twࡣ⇕፹య ᗘ [K]㸪kmࡣ ᅽຊᕪᇶ࡙ࡃ≀㉁⛣ືಀᩘ [kg/(m2·s·Pa)]㸪pevapࡣⓎჾࡲࡓࡣจ⦰ჾෆẼᅽ [Pa]㸪ps
ࡣ྾ᾮ⾲㠃ࡢ㣬Ẽᅽ [Pa]࡛࠶ࡿ㸬
ࡲࡓ㸪qcomdࡣmࢆ⏝࠸࡚㸪௨ୗࡢࡼ࠺࠼ࡽࢀࡿ㸬
e cond mL
q 㸦5-6㸧
ࡇࡇ࡛LeࡣỈࡢⓎ₯⇕ [J/kg]࡛࠶ࡿ㸬
྾ᾮ୰ࡢLiBr⃰ᗘࡣ㸪⤖ᬗᏑᅾୗ࡛ࡣ௨ୗࡢࡼ࠺࠼ࡽࢀࡿ㸬
LiBr*
LiBr C
C 㸦5-7㸧
ࡇࡇ࡛CLiBr*ࡣLiBr㣬⃰ᗘ [kg-LiBr/kg-solution]࡛࠶ࡿ㸬㣬⁐ゎᗘ௨ୗ࡛ࡣ㸪྾╔
ࡢLiBrᖹ⾮྾╔㔞⁐ᾮ⃰ᗘࡢ㛵ಀࢆ㸪ḟᘧࡢࡼ࠺࠼ࡓ(30)㸬 b
aC
q LiBr 㸦5-8㸧
ࡇࡇ࡛ q*ࡣ LiBr ᖹ⾮྾╔㔞 [kg-LiBr/kg-adsorbent]㸪a ࡣ྾╔ᖹ⾮ࣃ࣓࣮ࣛࢱ࣮ [kg-solution/kg-adsorbent]࡛࠶ࡿ㸬
ᇶ♏ᘧEq. (5-1)ࠥ(5-3)ࡣ㸪ࡑࢀࡒࢀ྾ჾཬࡧ⏕ჾࡈఏ⇕㠃✚ἢࡗ࡚㞳ᩓࡋ࡚
ᩘ್✚ศࡍࡿࡇࡼࡾゎ࠸ࡓ㸬྾ᾮ㛵ࡍࡿㅖ≀ᛶ್ࡣᩥ⊩್(23)(24)(25)(30)ࢆ⏝࠸ࡓ㸬ࡲ
ࡓ㸪྾ᾮࡢ࢚ࣥࢱࣝࣆ࣮ཬࡧ㣬ỈẼᅽࡘ࠸࡚ࡣ㸪 ᗘ⃰ᗘࡢ㛵ᩘ࡛࠼ࡽࢀ㸪ᩥ
⊩(31)࡚࠼ࡽࢀ࡚࠸ࡿ┦㛵㛵ಀࢆ⏝࠸ࡓ㸬Ⓨჾཬࡧจ⦰ჾࡘ࠸࡚ࡣ㸪ࡑࢀࡒࢀᡤᐃࡢ ᗘ୍࡛ᐃࡋࡓ㸬
⤖ᯝཬࡧ⪃ᐹ
ᚤ⣽⤖ᬗ⢏ᗘศᕸ⢏ᗘศᕸࡢ ᐃ⤖ᯝࢆᅗᅗ 5-4 ♧ࡍ㸬ᐇ⥺ࡣ⤖ᬗࢫ࣮ࣛࣜ㸪Ⅼ⥺ࡣࢮ࢜ࣛࢺࡢ⢏ᗘศ ᕸࢆ⾲ࡋ࡚࠸ࡿ㸬ࢮ࢜ࣛࢺ⢏ᗘࡣ2ࠥ10 m࡛࠶ࡿࡢᑐࡋ࡚㸪⤖ᬗࢫ࣮ࣛࣜࡢ⤖ᬗ⢏ᗘ
ࡣ 9ࠥ200 m ࡢ⠊ᅖ࡛ศᕸࡋ࡚࠸ࡓ㸬⤖ᬗࢫ࣮ࣛࣜࡣ㸪ࢮ࢜ࣛࢺࡢ⢏ᗘ⠊ᅖࢇ
Ꮡᅾࡋ࡞࠸ࡇࡽ㸪ࢮ࢜ࣛࢺࡀ⤖ᬗ᰾࡞ࡾࡑࡢ࿘ࡾLiBr⤖ᬗࡀᯒฟࡋ࡚࠸ࡿ⪃
࠼ࡽࢀࡿ㸬ࡑࡇ࡛㸪ࢮ࢜ࣛࢺࡢ࣓ࢪࣥᚄ7.09 mࡢ༢୍⢏Ꮚ࿘ࡾLiBrࡀ⌫≧⤖ᬗ ᡂ㛗ࡋࡓ௬ᐃࡋ࡚㸪⤖ᬗࢫ࣮ࣛࣜࡢ⢏Ꮚᚄࢆヨ⟬ࡋࡓࡇࢁ7.45 m࡛࠶ࡗࡓ㸬ィ ࡉࢀ
ࡿ⤖ᬗࢫ࣮ࣛࣜࡢ࣓ࢪࣥᚄࡀ57.0 m࡛࠶ࡗࡓࡢẚ㍑ࡍࡿ㸪ⴭࡋࡃᑠࡉ࠸⤖ᯝ࡞ࡗ ࡓ㸬ࡇࢀࡣ⤖ᬗᵓ㐀ⓗᆒ୍࡞⌫≧ࡣ⤖ᬗᡂ㛗ࡋ࡚࠸࡞࠸㸪ࡲࡓࡣ࠶ࡿ⛬ᗘࡢ」ᩘࡢ⤖ᬗ
⢏Ꮚࡀจ㞟ࡋࡓࡓࡵ⪃࠼ࡽࢀࡿ㸬ࡋࡋ㸪᭱⢏Ꮚᚄ࡛ࡶ200 m௨ୗ࡞ࡿࡇ㸪ᩘ
ࣨ᭶㟼⨨ࡋࡓሙྜࡶࢫ࣮ࣛࣜ≧ែࢆ⥔ᣢࡋࡓࡇࡽ㸪྾ᘧࣄ࣮ࢺ࣏ࣥࣉ⏝ࡋࡓ
ࡋ࡚ࡶὶ㊰ࡢ㛢ሰ࡞ࡢၥ㢟ࡣᑡ࡞࠸ࡇࡀᮇᚅࡉࢀࡿ㸬ࡓࡔࡋ㸪ࡇࡢⅬࡘ࠸࡚ࡣᚋ ࡉࡽヲ⣽࡞᳨ウࢆせࡍࡿ㸬
⤖ᬗࢫ࣮ࣛࣜ⢓ᗘ
⤖ᬗࢫ࣮ࣛࣜࡢ⢓ᗘ⤖ᬗ⃰ᗘࡢ㛵ಀࢆᅗᅗ5-5♧ࡍ㸬グྕڦࡣ㣬⁐ゎᗘࡀ㧗ࡃ⤖ᬗ ࡀᏑᅾࡋ࡞࠸ ᗘ50 °C࡛ࡢࢮ࢜ࣛࢺศᩓࡋࡓ⁐ᾮ㸦LiBr⃰ᗘ63.4 %ࠊࢮ࢜ࣛࢺศᩓ
⃰ᗘ5.56 %㸧ࡢ⢓ᗘ㸪یࡢࣉࣟࢵࢺࡣ ᗘࢆ3520 °Cపୗࡉࡏࡿࡇ࡛⤖ᬗࢆᯒฟࡉ
ࡏ࡚ࡑࡢྜࢆቑຍࡉࡏࡓሙྜࡢ⢓ᗘࢆ⾲ࡍ㸬ࡲࡓ㸪୍Ⅼ㙐⥺ࡣࢮ࢜ࣛࢺࢆྵࡲ࡞࠸
50 °C 㸪63.4%ࡢLiBr⁐ᾮ㸪◚⥺ࡣ20 °Cࡢ⣧Ỉ⢓ᗘࡢᩥ⊩್(23)ࢆ⾲ࡍ㸬㣬⁐ゎᗘ௨ୗ࡛
྾ᾮ⃰ᗘ ᗘࡀྠ୍࡛ࡶ㸪ࢮ࢜ࣛࢺ⢏Ꮚࡢศᩓࡼࡾ⢓ᗘࡀ⣙50%㧗ࡃ࡞ࡿ㸬ࡲࡓ㸪
⤖ᬗࢫ࣮࡛ࣛࣜࡣ⤖ᬗ⃰ᗘࡢቑຍక࠸⢓ᗘࡶቑຍࡍࡿഴྥࡀㄆࡵࡽࢀࡿࡀ㸪ᮏᐇ㦂⠊ᅖ
࡛᭱ࡶ⢓ᗘࡀ㧗ࡃ࡞ࡿ20 °C㸪0.024 kg-LiBr/kg-solutionࡢࢫ࣮࡛ࣛࣜࡶ྾ᾮ༢⊂ࡢ2.7ಸ
⛬ᗘ࡛࠶ࡾ㸪༑ศ࡞ὶືᛶࢆ᭷ࡍࡿࡇࡀ᫂ࡽ࡞ࡗࡓ㸬
ᾮ⭷ࡢ⥲ᣓ⇕ఏ㐩ಀᩘ
ᐃࡋࡓ྾ᾮࡢฟධཱྀ ᗘLiBr⃰ᗘ㸪ࢩࣜࢥࣥ࢜ࣝฟධཱྀ ᗘࡽఏ⇕㔞ᖹᆒ
ᗘᕪࢆồࡵ㸪ḟᘧࡼࡾ⥲ᣓ⇕ఏ㐩ಀᩘhwࢆ⟬ฟࡋࡓ㸬
ΔTlm
A h
Q w 㸦5-9㸧
1 c2 2 c1
1 c2 2
lm ln c1T T T T
T T T
ΔT T 㸦5-10㸧
ࡇࡇ࡛㸪Qࡣఏ⇕㔞 [W]㸪 Tlmࡣᑐᩘᖹᆒ ᗘᕪ [K]ࢆ⾲ࡍ㸬ࡲࡓ㸪Eq. (5-10)ࡢ ᗘࡣᅗ 5-2♧ࡍ⨨ࡢ ᗘᑐᛂࡍࡿ㸬ఏ⇕㔞ࡣ྾ᾮࡢฟධཱྀ⃰ᗘᕪࡽồࡵࡓⓎ₯⇕㔞࠾ࡼ
ࡧࡑࢀࡒࢀࡢ ᗘ⃰ᗘᑐࡍࡿ࢚ࣥࢱࣝࣆ࣮ᕪࡽồࡵࡽࢀࡿ(31)㸬
ᅗᅗ5-6ࡣ㸪⥲ᣓ⇕ఏ㐩ಀᩘὶ㔞ࡢ㛵ಀࢆ♧ࡋࡓࡶࡢ࡛࠶ࡿ㸬ὶ㔞ࡀ30 ml/s௨ୖ࡛ࡣ㸪 ᐃ⢭ᗘୖࡤࡽࡘࡁࡀࡁ࠸ࡶࡢࡢ㸪࠾࠾ࡴࡡὶ㔞ࡀቑຍࡍࡿᚑ࠸⥲ᣓ⇕ఏ㐩ಀᩘࡶቑ ຍࡍࡿഴྥࡀぢࡽࢀ㸪ᮏὶ㔞⠊ᅖ࡛ࡣ100ࠥ900 W/(m2·K)ࡢ⠊ᅖ࡛ኚࡋࡓ㸬ࡲࡓ㸪ࡤࡽࡘ ࡁࡀᑠࡉ࠸30 ml/s௨ୗࡢపὶ㔞ᇦ࡛ẚ㍑ࡍࡿ㸪⇕ఏ㐩ಀᩘ࠼ࡿࢮ࢜ࣛࢺศᩓ⃰ᗘ ࡢᙳ㡪ࡣ㸪ᮏᐇ㦂⠊ᅖ࡛ࡣᑠࡉ࠸ࡇࡀ♧ࡉࢀࡓ㸬ὶ㔞ࡀࡁ࠸㡿ᇦ࡛ࡣ㸪྾ᾮฟධཱྀ㛫 ࡢỈẼⓎࡼࡿ⃰ᗘኚࡀᑠࡉࡃ㸪ࡇࡢ⃰ᗘィ ㄗᕪࡀ⇕ఏ㐩ಀᩘࡁࡃᙳ㡪ࢆ
࠼ࡿࡓࡵ㸪ࡤࡽࡘࡁࡀࡁࡃ࡞ࡿ㸬
ఏ⇕ヨ㦂ゎᯒࣔࢹࣝࡢẚ㍑
ゎᯒࣔࢹࣝࡢጇᙜᛶࢆ᳨ドࡍࡿࡓࡵ㸪ᾮ⭷ఏ⇕ᐇ㦂ࡼࡾᚓࡽࢀࡓ྾ᾮࡢ ᗘ⃰ᗘ
ࡘ࠸࡚ゎᯒ⤖ᯝẚ㍑ࡋࡓ㸬ᅗᅗ5-7ࡣ㸪྾╔ศᩓ⃰ᗘ2.65 %㸪ὶ㔞9.0 ml/s࡛⾜ࡗࡓఏ
⇕ᐇ㦂ྠ୍᮲௳࡛ゎᯒࡋࡓ⤖ᯝᐇ㦂⤖ᯝࢆ♧ࡍ㸬ࡓࡔࡋ㸪จ⦰ჾ ᗘ280K㸪≀㉁⛣ື
ಀᩘ2.0 kg/(m2·s·Pa)㸪4.0 kg-LiBr/kg-adsorbentࡋࡓ㸬ࡲࡓ㸪ࡇࡇ࡛ࡢゎᯒ࡛ࡣ⇕፹యỈ ࡢ⇕≀ᛶ್ࢆ⏝࠸࡚࠸ࡿࡀ㸪⇕ᐜ㔞㏿ᗘࢆ྾ᾮẚ࡚༑ศࡁࡃ࡞ࡿࡼ࠺タᐃࡋ࡚㸪 ฟධཱྀ ᗘᕪࡣࡰྠ⛬ᗘᑠࡉࡃ࡞ࡿࡼ࠺ࡋࡓࡓࡵ㸪ᐇ㦂ࡢẚ㍑ၥ㢟ࡣ⏕ࡌ࡞࠸
⪃࠼ࡽࢀࡿ㸬ᅗࡢゎᯒ⤖ᯝࡣ⁐ᾮࡀᾮ⭷ὶୗࡍࡿఏ⇕㠃✚᪉ྥࡢLiBr⃰ᗘ ᗘศᕸࢆ
♧ࡋ࡚࠸ࡿ㸬ఏ⇕ᐇ㦂࡛ࡣ0.1 m2ࡢఏ⇕㠃✚࡛⾜ࡗࡓࡓࡵ㸪ࡇࡢ㠃✚࡛ࡢゎᯒ್ᐇ㦂࡛ࡢ ᐃ್ࢆẚ㍑ࡍࡿ ᗘ㸪⃰ᗘࡶⰋዲ࡞୍⮴ࡀᚓࡽࢀࡓ㸬
྾╔ศᩓ⃰ᗘ2.66 %ࡢࡁ㸪ࡑࡢࡢὶ㔞ࡘ࠸࡚ࡶఏ⇕ᐇ㦂ゎᯒ⤖ᯝࢆẚ㍑ࡋࡓ㸬 ᅗ
ᅗ5-8ࡣ୧⪅ࡢ┦ᑐㄗᕪࢆ♧ࡋࡓࡶࡢ࡛࠶ࡿ㸬ࡓࡔࡋ㸪┦ᑐㄗᕪࡣḟᘧ࡛ᐃ⩏ࡋࡓ㸬
100
n e n
A M
R A 㸦5-11㸧
ࡇࡇ࡛㸪Rࡣ┦ᑐㄗᕪ [%]㸪Anࡣゎᯒ್㸪Meࡣᐇ㦂 ᐃ್ࡢ ᗘࡲࡓࡣ⃰ᗘࢆ⾲ࡍ㸬ྛὶ 㔞࡛ࡢ┦ᑐㄗᕪࡣ࠾࠾ࡴࡡ1 %⛬ᗘ࡛࠶ࡾ㸪ࡁࡃ࡚ࡶ3 %௨ෆ࡞ࡗࡓ㸬௨ୖࡢࡇࡽ
ᮏゎᯒࣔࢹࣝࡣ㸪༑ศጇᙜ࡞⢭ᗘ⪃࠼ࡽࢀࡿ㸬
⤖ᬗࢫ࣮ࣛࣜࡼࡿᛶ⬟ྥୖຠᯝ
๓⠇ࡢᮏゎᯒࣔࢹࣝࡢጇᙜᛶᇶ࡙ࡁ㸪⤖ᬗࢫ࣮ࣛࣜ㸪྾╔ศᩓ྾ᾮ㸪྾ᾮ༢⊂ࡢ 3ࡘࡢ᮲௳ࡘ࠸࡚㸪྾ჾࡢᛶ⬟ྥୖຠᯝࢆ᳨ウࡋࡓ㸬ᮏゎᯒ᮲௳ࢆ⾲⾲ 5-1♧ࡍ㸬⤖ᬗ ࢫ࣮ࣛࣜࡣỈẼ྾ࡋ࡚ࡶ⤖ᬗ⁐ゎࡢຠᯝࡼࡾ⃰ᗘࡀኚࢃࡽ࡞࠸ࡓࡵ୍ᐃࡋ㸪྾╔
ศᩓ྾ᾮࡣ྾╔ࡢ⬺╔ຠᯝࡼࡾỈẼ྾ࡼࡿ⃰ᗘపୗྜࢃࡏ࡚LiBrࡀ⬺╔
ࡍࡿࡋࡓ㸬
ᮏゎᯒࣔࢹࣝࡼࡾ⤖ᬗࢫ࣮ࣛࣜࡢᛶ⬟ྥୖຠᯝࡘ࠸࡚ゎᯒࡋࡓ⃰ᗘศᕸ࣭ỈẼ྾
㔞ࡢ⤖ᯝࢆᅗᅗ5-8♧ࡍ㸬⤖ᬗࢫ࣮࡛ࣛࣜࡣ⃰ᗘ୍ᐃ௬ᐃࡋ࡚࠸ࡿࡓࡵኚࡣ࡞࠸ࡀ㸪
྾╔ศᩓ྾ᾮ࡛ࡣ྾╔ࡢLiBr⬺╔ຠᯝࡼࡾࢃࡎ࡞ࡀࡽ⃰ᗘపୗࢆᢚไࡋࡓ㸬ࡲ
ࡓ㸪ỈẼ྾㔞ࡣ㸪྾ᾮࡀఏ⇕㠃✚1 m2ὶୗࡍࡿࡲ࡛྾ᾮ༢⊂࡛2.58×10-3 kg-water/s
࡛࠶ࡗࡓࡀ㸪྾╔ศᩓ྾ᾮ࡛ࡣ3.13×10-3 kg-water/sࡢ⣙20 %㸪ࡉࡽ⤖ᬗࢫ࣮࡛ࣛࣜ
ࡣ5.05×10-3 kg-water/sࡢ⣙100 %ቑຍࡋ㸪ỈẼ྾⬟ຊࡢⴭࡋ࠸ྥୖຠᯝࢆᮇᚅ࡛ࡁࡿ⤖
ᯝࡀᚓࡽࢀࡓ㸬
ᮏ❶ࡢࡲࡵ
྾ᘧࣄ࣮ࢺ࣏ࣥࣉࡼࡾప ⇕ࢆᅇࡋ෭⇕ࢆᚓࡿ⨨ࡢ㧗ᛶ⬟ࢆ┠ᣦࡋ㸪྾ᾮ
㐣㣬ᚤ⣽⤖ᬗࢫ࣮ࣛࣜࢆ⏝࠸ࡿ᪉ᘧࢆᥦࡋ㸪௨ୗࡢ⤖ᯝࡀᚓࡽࢀࡓ㸬
㸯㸧LiBr⃰ᗘ63.4 %㸪྾╔ศᩓ⃰ᗘ5.56 %㸪 ᗘ25 °Cࡢ㐣㣬ᚤ⣽⤖ᬗࢫ࣮ࣛࣜࡢ⤖
ᬗ⢏ᗘࡣ10ࠥ200 m㸪࣓ࢪࣥᚄࡣ57.0 m࡛࠶ࡗࡓ㸬
㸰㸧㐣㣬ᚤ⣽⤖ᬗࢫ࣮ࣛࣜࡢ⢓ᗘࡣ㸪LiBr⃰ᗘ63.4 %㸪྾╔ศᩓ⃰ᗘ5.56 %ࡢ⁐ᾮࢆ
ᗘไᚚࡍࡿࡇ࡛⤖ᬗ㔞ࢆኚࡉࡏࡓ⤖ᯝ㸪⤖ᬗ㔞ࡀቑຍࡍࡿࡘࢀ⢓ᗘࡶቑຍࡍࡿ
ࡶࡢࡢ㸪ᮏᐇ㦂⠊ᅖ࡛᭱⢓ᗘࡣ1.67×10-2 Pa·s࡛࠶ࡾ㸪༑ศ࡞ὶືᛶࢆ᭷ࡍࡿࡇࡀ᫂
ࡽࡉࢀࡓ㸬
㸱㸧ᾮ⭷ఏ⇕ᐇ㦂ࡼࡾ㸪྾ᾮ୰ࡢ྾╔㸦ࢮ࢜ࣛࢺHSZ-320NAA㸧ࡀ⥲ᣓ⇕ఏ㐩ಀ
ᩘ࠼ࡿᙳ㡪ࡣᑠࡉ࠸㸬ࡲࡓ㸪྾ᾮὶ㔞ࡢቑຍᚑ࠸⥲ᣓ⇕ఏ㐩ಀᩘࡣቑຍࡍࡿ㸬 㸲㸧ᾮ⭷ఏ⇕ᐇ㦂ẚ㍑ࡋ㸪ᮏゎᯒࣔࢹࣝࡣ3 %௨ෆࡢ⢭ᗘ࡛ጇᙜᛶࡀ☜ㄆࡉࢀࡓ㸬 㸳㸧ゎᯒࣔࢹࣝࡼࡾỈẼ྾⬟ຊྥୖຠᯝࡘ࠸࡚ゎᯒࡋࡓ⤖ᯝ㸪྾ᾮ༢⊂ẚ㍑
ࡋ྾╔ศᩓ྾ᾮࡣ20 %㸪㐣㣬ᚤ⣽⤖ᬗࢫ࣮ࣛࣜࡣ100 %ቑຍࡍࡿྥୖຠᯝࡀ♧ࡉ
ࢀࡓ㸬
(a) Fine particle slurry of LiBr
(b) LiBr crystal lump grown Fig. 5-1 Pictures of supersaturated crystal
Fig.5-2 Heat-transfer device of liquid film
Fig. 5-3 Outline of analysis model in absorber
Fig. 5-4 Particle size distribution of supersaturated fine particle crystal
Fig. 5-5 Viscosity of LiBr slurry solution against crystal concentration
Fig. 5-6 Relation between heat transfer coefficient and flow rate
Fig. 5-7 LiBr conc. and temperature profiles
Fig. 5-8 Relative error of the measured value and analysis
Table 5-1 Analysis conditions
Condition Slurry Adsorbent suspension Solution
Flow rate [kg/(m2·s)]
Inlet temp. [K]
Inlet conc. [kg/kg-sol.]
Adsorbent conc. [kg/kg-sol.]
Heat transfer fluid flow rate [kg/(m2·s)]
Heat transfer fluid temp. [K]
Condenser temp. [K]
Mass transfer coeff. [kg/(m2·s·Pa)]
Heat transfer coef. [W/(m2·K)]
Equilibrium adsorption parameter [kg/kg-sol.]
Heat transfer area [m2]
0.01 310 0.64 0.2 0.5 290 280 2.0 400 4.0 1.0
0.01 310 0.64 0.2 0.5 290 280 2.0 400 4.0 1.0
0.01 310 0.64 0.0 0.5 290 280 2.0 400 - 1.0
Fig. 5-9 LiBr conc. and water absorption profiles
0.40 0.45 0.50 0.55 0.60 0.65 0.70
0E+0 1E-3 2E-3 3E-3 4E-3 5E-3 6E-3
0 0.2 0.4 0.6 0.8 1
LiBr crystal slurry Solution slurry Solution
LiB r conc. [k g-LiBr/ kg-sol] Abs o rbed wat e r x 10
3[kg- w a te r/ s]
Surface area [m
2]
hc: 400 W/(m2 K) km: 2 kg/(m2 s Pa)
グ グྕ
A = heat transfer surface area [m2]
a = equilibrium adsorption parameter define by Eq. (5-8) [kg-solution/kg-adsorbent]
An = analysis value
b = parameter defined by Eq. (5-8) [kg-LiBr/kg-adsorbent]
CLiBr= LiBr concentration in solution [kg-LiBr/kg-solution]
cLiBr = specific heat of Lithium Bromide [J/(kg͌K)]
cpa = specific heat of adsorption [J/(kg͌K)]
hs = enthalpy of solution [J/kg-solution]
hw = overall heat transfer coefficient [W/(m2͌K)]
km = mass transfer coefficient [kg/(m2͌s͌Pa)]
Le = latent heat of water vapor [J/kg]
m ˙ = rate of absorption or evaporation [kg-water/(m2͌s)]
Me = measured value
pevap = vapor pressure in evaporator or condenser [kg/(m2͌s͌Pa)]
ps = equilibrium vapor pressure [kg/(m2͌s͌Pa)]
Q = amount of heat transfer [W]
qcomd= phase change enthalpy per unit heat transfer surface area [W/m2] qw = heat transfer rate between heat transfer fluids and solution [W/m2] q* = LiBe amout adsorbed in adsorbent [kg-LiBr/kg-adsorbent]
R = relative error [%]
T = solution temperature [K]
T1 = entrance temperature of solution [K]
T2 = exit temperature of solution [K]
Tc1 = entrance temperature of heat transfer fluid [K]
Tc2 = exit temperature of heat transfer fluid [K]
Tw = heat transfer fluid temperature [K]
Tlm= log-mean temperature difference [K]
w = flow rate of solution [kg-solution/s]
wc = flow rate of adsorbent in solution [kg-adsorbent/s]
ad = amout of LiBr crystal [kg-LiBr/kg-adsorbent]
➨
➨㸴❶ /L%U ᚤ⣽⤖ᬗࢫ࣮ࣛࣜࡢㄪ〇ỈẼ྾≉ᛶ
ᮏ❶࡛ࡣ㸪AHPࡢ྾ᾮࡋ࡚ࡢLiBrᚤ⣽⤖ᬗࢫ࣮ࣛࣜࡢ≉ᛶ᭷ຠᛶࢆホ౯ࡍࡿ㸬ࢫ
࣮ࣛࣜࡢ⤖ᬗࢧࢬࢆணࡵ ᐃࡋ࡚ࢫ࣮ࣛࣜᙧᡂࡢᣲືࢆゎ᫂ࡍࡿ㸬AHPࡢᛶ⬟ᑐࡍࡿ
྾╔࠾ࡼࡧLiBrᚤ⣽⤖ᬗࢫ࣮ࣛࣜࡢຠᯝࢆ㸪㐣ཤࡢࣔࢹ࡛ࣝᚓࡽࢀࡓ⤖ᯝࣛ࣎ࢫࢣ
࣮ࣝᐇ㦂⤖ᯝࡢẚ㍑᳨ウࡼࡾ᳨ドࡍࡿ㸬