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TK4552 - EVAPORASI DAN KRISTALISASI
Program Studi Teknik Kimia
Fakultas Teknik Universitas Sebelas Maret 2020
Aida Nur Ramadhani, S.T., M.T.
PERHITUNGAN
EVAPORATOR SINGLE EFFECT
Sub-CPMK 3 : Mahasiswa mampu menerapkan konsep perhitungan evaporator
• Ketepatan menganalisis neraca massa dan panas di sekitar evaporator
• Ketepatan menganalisis apa saja yang menjadi faktor yang
mempengaruhi proses evaporasi
PERHITUNGAN EVAPORATOR SINGLE EFFECT
PERHITUNGAN EVAPORATOR SINGLE EFFECT
EVAPORATOR
KOEFISIEN TRANSFER PANAS OVERALL
Diagram – single effect evaporator
feed, F
TF , xF , hF.
steam, S
TS , HS
concentrated liquid, L
T1 , xL , hL
condensate, S
TS , hS
vapor, V to condenser
T1 , yV , HV
P1
T1
heat-exchanger
tubes
 Umpan F (biasanya encer) masuk pada suhu TF
 Uap jenuh masuk pada suhu TS
 Larutan dalam evaporator diasumsikan tercampur sempurna dan memiliki
komposisi yang sama
Neraca massa dan panas
 Persamaan dasar:
dengan,
∆𝑇 = beda suhu antara steam terkondensasi dengan cairan mendidih dalam
evaporator (K).
q = kerja (Btu/h)
𝑞 = 𝑈𝐴(∆𝑇)
Menghitung
 Laju alir fase vapor, V dan fase liquid, L.
 Luas perpindahan panas, A
 Koefisien transfer panas overall, U.
 Fraksi mol solute, xL.
Diagram – single effect evaporator
Steam, S
PS, TS, HS
Feed, F
xF, TF, hF
Condensate, S
PS, TS, hS
Vapour, V
yV, T1, HV
Concentrate, L
xL, T1, hL
P
T1
Feed:
F – mass flow rate
xF – mass fraction of solute in feed
TF – temperature of feed
hF – enthalpy of feed
Vapour leaving the evaporator:
V – mass flow rate
yV – mass fraction of solute in vapour
T1 – temperature of vapour
HV – enthalpy of vapour
Steam, S
PS, TS, HS
Feed, F
xF, TF, hF
Condensate, S
PS, TS, hS
Vapour, V
yV, T1, HV
Concentrate, L
xL, T1, hL
P
T1
Concentrate leaving the evaporator:
L – mass flow rate
xL – mass fraction of solute in concentrate
T1 – temperature of concentrate
hL – enthalpy of concentrate
Steam:
S – mass flow rate
PS – steam pressure
TS – steam temperature
HS – enthalpy of steam
hS – enthalpy of condensate
P – pressure in the evaporator
T1 – temperature in the evaporator
Neraca Massa
Overall material balance:
F = L + V
Solute balance:
F xF = L xL + VyV
If the vapour is free ofsolute:
F xF = LxL
Steam, S
PS, TS, HS
Feed, F
xF, TF, hF
Condensate, S
PS, TS, hS
Vapour, V
yV, T1, HV
Concentrate, L
xL, T1, hL
P
T1
Neraca Panas
Maka,
F hF + S HS = L hL + V HV + ShS
F hF + S (HS - hS) = L hL + V HV
F hF + S λ = L hL + VHV
where λ = HS –hS = heat latent
Heat in feed + heat in steam = heat in concentrated liquid + heat in vapor
+ heat in condensed steam
S
F
S
V
L
S
TS, HS
F
S
TS, hS
V
L
P
T1
Energy lost by thesteam
q = S λ = S (HS –hS)
Jika tidak ada energi yang hilang
ke lingkungan, jumlah energi akan
ditransfer dari uap ke larutan
melalui dinding tabung area A dan
koefisien perpindahan panas
overall U.
Maka,
q = U AΔT = U A (TS – T1)
Operasi – single effect evaporator
 Panas dari steam saat Ts bisa didapatkan dari steam table.
 Entalpi dari umpan feed (F) – larutan dengan konsentrasi X – dalam tabel, jika
tidak tersedia:
Asumsi:
 Bahwa feed sangat dilute (encer) sehingga panas laten penguapan 1 kg
massa air dari larutan berair (aqueous) dapat diperoleh dari steam table
menggunakan suhu larutan mendidih T1 (suhu evaporator).
 Jika kapasitas panas (cp) dari liquid feed (umpan cair) diketahui  dapat
digunakan untuk menghitung entalpi (abaikan panas pelarutan).
Contoh:
A continuous single-effect evaporator concentrates 9072 kg/h of a 1.0 wt % salt
solution entering at 38ºC to a final concentration of 1.5 wt %.
The vapor space of the evaporator is at 101.325 kPa (1.0 atm abs) and the steam
supplied is saturated at 150 kPa. The overall coefficient U = 1704 W/m2.K.
Calculate the amounts of vapor and liquid products and the heat-transfer area
required. Assumed that, since it its dilute, the solution has the same boiling point
as water.
Data:
The latent heat of steam at 150 kPa 383.2 K = 2230 kJ/kg (958,8 Btu/h)
The latent heat of water at 101.325 kPa 373,2 K= 2257 kJ/kg (970,3 Btu/h)
Penyelesaian
Diketahui:
F = 9.072 kg/h
xF = 1 wt % = 0,01 kg solute / kgfeed
TF =38°C =
xL = 1,5 wt%
= 0,015 kg solute / kg liquid product
P = 101,325 kPa (1.0 atm abs)
PS = 150kPa
U = 1704 W/m2.K
T1 = saturated temperature at P (= 101,325 kPa) = 100°C
TS = saturated temperature at 150 kPa = 111,4°C
Penyelesaian
Steam, S
PS, TS, HS
Feed, F
xF, TF, hF
Condensate, S
PS, TS, hS
Vapour, V
yV, T1, HV
Concentrate, L
xL, T1, hL
P
T1
Ditanya:
V=?
L=?
A=?
Penyelesaian
NM total,
F = L + V
9.072 = L + V
NM solute,
F xF = L xL
9.072 (0,01) = L (0,015)
L = 6.048 kg/h of liquid
Maka,
V = 3.024 kg/h of vapor
Penyelesaian
Asumsi: larutan sangat encer (as water);
cpF = 4,14 kJ/kg. K (Table A.2-5)
Dari soal:
At P1 = 101,325 kPa, T1 = 373,2 K (100°C) (datum temperature).
HV = 2.257 kJ/kg.
At PS = 143,3 kPa, TS = 383,2 K (110°C).
 = 2.230 kJ/kg.
Maka, entalpi umpan dapat dihitung,
hF = cpF (TF – T1)
hF = 4,14 (311,2 – 373,2)
= -256,68 kJ/kg.
Penyelesaian
F hF + S  = L hL + V HV
with hL = 0, karena T datum adalah 373.2 K.
9.072 (-257,508) + S (2.230) = 6.048 (0) + 3.024 (2.257)
S = 4.108 kg steam /h
Panas (q) yang dipindahkan melalui luas permukaan panas A,
q = S ()
q = 4.108 (2.230) (1.000 / 3.600) = 2.544.000 W
Luas permukaan panas (A);
q = U A T = U A (TS – T1)
2.544.000 = 1704 A (383,2 – 373,2)
A = 149,3 m2
Neraca Panas
Penyelesaian
Maka,
V = 3.024 kg/h of vapor
L = 6.048 kg/h of liquid
A = 149,3 m2
Pengaruh variable proses terhadap operasional evaporator
 Suhu aliran umpan memiliki efek besar pada operasi evaporator.
 Saat umpan tidak berada pada titik didihnya, uap pertama-tama diperlukan
untuk memanaskan umpan ke titik didihnya lebih dahulu, baru kemudian
mengalami proses penguapan.
 Pemanasan awal umpan dapat mengurangi besarnya area perpindahan panas
evaporator akibat hal tersebut.
suhu umpan:
 Tekanan dalam evaporator menentukan titik didih larutan (T1).
 Tekanan uap menentukan suhu uap (Ts)
 Karena q = U A (TS - T1), maka semakin besar selisih (TS - T1) akan membantu
mengurangi area perpindahan panas yang dibutuhkan  mengurangi biaya.
 Dapat dilakukan dengan memanfaatkan efek tekanan.
Tekanan:
Boiling Point Rise
 Dalam contoh 1, larutan diasumsikan cukup encer sehingga dianggap memiliki
sifat termal yang sama dengan air.
 Hal tersebut tidak selalu benar.
 Untuk larutan dengan konsentrasi tinggi  terdapat kenaikan titik didih larutan
 Aturan Duhring (Duhring Law) adalah hukum empiris hubungan antara titik
didih larutan dan titik didih pelarut pada tekanan yang berbeda untuk tiap
konsentrasi larutan – perkiraan kenaikan titik didih larutan.
Contoh
 Pressure in an evaporator is given as 25,6 kPa (3,72 psia) and a solution of 30%
NaOH is being boiled.
 Determine the boiling temperature of the NaOH solution and the boiling-
point rise (BPR) of the solution over that of water at the same pressure.
Penyelesaian:
 Cari titik didih air pada P soal  25,6 kPa (3,72 psia)
 Steam table, boiling point of water at 25,6 kPa is 65,6°C (Tsat)
 Dari TD air, dicari titik didih untuk larutan 30% NaOH di fig.8-4
 Untuk TD air 65,6°C (150°F) and 30% NaOH  titik didih larutan NaOH
tersebut adalah 79,5°C (175°F).
 Menghitung BPR
 The boiling-point rise = 79,5°C – 65,6°C = 13,9°C (25°F)
Enthalpy-Concentration Chart
Heat of solution – Panas pelarutan
 Panas yang dihasilkan atau diserap ketika suatu zat melarut (terbentuk sebuah
larutan).
 Jumlah panas yang terlibat ketika satu mol atau satu gram larut dalam pelarut
mengalami pelarutan.
 Jumlah panas bergantung pada jenis senyawa, dan jumlah air yang digunakan
untuk melarutkan.
 Contoh pada proses pelarutan pellet NaOH.
Latihan!
An evaporator is used to concentrate 4.536 kg/h of a 20 % solution of NaOH
in water entering at 60ºC to a product of 50 % solid. The pressure of the
saturated steam used is 172,4 kPa and the pressure in the vapor space of
the evaporator is 11,7 kPa. The overall heat-transfer coefficient is 1.560
W/m2.K.
Calculate the steam used, the steam economy in kg vaporized/kg steam
used, and the heating surface area in m2.
Latihan!
Buatlah diagramnya terlebih dahulu!
U = 1560 W/m2
T1 A = ?
P1 = 11,7 kPa
F = 4.536 kg/h
TF = 60°C
xF = 0,2
hF.
S = ?
TS , HS
PS = 172,4 kPa
L, T1 , hL
xL = 0,5
S, TS , hS
V, T1 , yV , HV
Penyelesaian?
NM total,
F = L + V
4.536 = L + V
NM solute,
F xF = L xL
4.536 (0,2) = L (0,5)
L = 1.814 kg/h of liquid
Maka,
V = 2.722 kg/h of vapor
Penentuan T1 = Tsat + BPR of the 50% concentrate product.
 Tsat air dari steam table.
Pada 11.7 kPa, Tsat = 48,9ºC.
 Dari grafik Duhring (Fig. 8.4-2), untuk Tsat = 48,9 ºC and 50 % NaOH , titik
didih dari larutan adalah T1 = 89,5ºC.
BPR = T1 - Tsat = 90 – 48,9 = 40,6ºC
 From the enthalpy-concentration chart (Fig.8.4-3), for
TF = 60ºC and xF = 0,2 get hF = 214 kJ/kg.
T1 = 90ºC and xL = 0,5 get hL = 505 kJ/kg.
Penyelesaian?
Penyelesaian?
 For saturated steam at 172,4 kPa, from steam table, we get
TS = 115,6 ºC and  = 2.214 kJ/kg.
 To get HV for superheated vapor, first we obtain the enthalpy at Tsat = 48,9ºC and P1
= 11,7 kPa, get Hsat = 2.590 kJ/kg. Then using heat capacity of 1.884 kJ/kg.K for
superheated steam.
HV = Hsat + cp.BPR
= 2.590 + 1,884 (40,6) = 2.667 kJ/kg.
 Substituting into heat balance equation and solving for S,
F hF + S  = L hL + V HV
4.535 (214) + S (2.214) = 1.814 (505) + 2.722 (2667)
S = 3.255 kg steam /h.
Atau bisa langsung cari Hv di
steam table untuk
superheated;
T1 = 89,5ºC P = 11,7 kPa
Penyelesaian?
 The heat q transferred through the heating surface area, A is
q = S ()
q = 3.255 (2.214) (1.000 / 3.600) = 2.002.000 W
 Solving for capacity single-effect evaporator equation;
q = U A T = U A (TS – T1)
2.002.000 = 1.560 A (115,6 – 89,5)
 Solving,
A = 49,2 m2
Steam economy = 2.722/3.255
= 0,836
Tugas

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Bab 4 - Perhitungan Single effect evaporator.pptx

  • 1. TK4552 - EVAPORASI DAN KRISTALISASI Program Studi Teknik Kimia Fakultas Teknik Universitas Sebelas Maret 2020 Aida Nur Ramadhani, S.T., M.T. PERHITUNGAN EVAPORATOR SINGLE EFFECT
  • 2. Sub-CPMK 3 : Mahasiswa mampu menerapkan konsep perhitungan evaporator • Ketepatan menganalisis neraca massa dan panas di sekitar evaporator • Ketepatan menganalisis apa saja yang menjadi faktor yang mempengaruhi proses evaporasi PERHITUNGAN EVAPORATOR SINGLE EFFECT
  • 3. PERHITUNGAN EVAPORATOR SINGLE EFFECT EVAPORATOR KOEFISIEN TRANSFER PANAS OVERALL
  • 4. Diagram – single effect evaporator feed, F TF , xF , hF. steam, S TS , HS concentrated liquid, L T1 , xL , hL condensate, S TS , hS vapor, V to condenser T1 , yV , HV P1 T1 heat-exchanger tubes
  • 5.  Umpan F (biasanya encer) masuk pada suhu TF  Uap jenuh masuk pada suhu TS  Larutan dalam evaporator diasumsikan tercampur sempurna dan memiliki komposisi yang sama Neraca massa dan panas  Persamaan dasar: dengan, ∆𝑇 = beda suhu antara steam terkondensasi dengan cairan mendidih dalam evaporator (K). q = kerja (Btu/h) 𝑞 = 𝑈𝐴(∆𝑇)
  • 6. Menghitung  Laju alir fase vapor, V dan fase liquid, L.  Luas perpindahan panas, A  Koefisien transfer panas overall, U.  Fraksi mol solute, xL.
  • 7. Diagram – single effect evaporator Steam, S PS, TS, HS Feed, F xF, TF, hF Condensate, S PS, TS, hS Vapour, V yV, T1, HV Concentrate, L xL, T1, hL P T1 Feed: F – mass flow rate xF – mass fraction of solute in feed TF – temperature of feed hF – enthalpy of feed Vapour leaving the evaporator: V – mass flow rate yV – mass fraction of solute in vapour T1 – temperature of vapour HV – enthalpy of vapour
  • 8. Steam, S PS, TS, HS Feed, F xF, TF, hF Condensate, S PS, TS, hS Vapour, V yV, T1, HV Concentrate, L xL, T1, hL P T1 Concentrate leaving the evaporator: L – mass flow rate xL – mass fraction of solute in concentrate T1 – temperature of concentrate hL – enthalpy of concentrate Steam: S – mass flow rate PS – steam pressure TS – steam temperature HS – enthalpy of steam hS – enthalpy of condensate P – pressure in the evaporator T1 – temperature in the evaporator
  • 9. Neraca Massa Overall material balance: F = L + V Solute balance: F xF = L xL + VyV If the vapour is free ofsolute: F xF = LxL Steam, S PS, TS, HS Feed, F xF, TF, hF Condensate, S PS, TS, hS Vapour, V yV, T1, HV Concentrate, L xL, T1, hL P T1
  • 10. Neraca Panas Maka, F hF + S HS = L hL + V HV + ShS F hF + S (HS - hS) = L hL + V HV F hF + S λ = L hL + VHV where λ = HS –hS = heat latent Heat in feed + heat in steam = heat in concentrated liquid + heat in vapor + heat in condensed steam S F S V L
  • 11. S TS, HS F S TS, hS V L P T1 Energy lost by thesteam q = S λ = S (HS –hS) Jika tidak ada energi yang hilang ke lingkungan, jumlah energi akan ditransfer dari uap ke larutan melalui dinding tabung area A dan koefisien perpindahan panas overall U. Maka, q = U AΔT = U A (TS – T1)
  • 12. Operasi – single effect evaporator  Panas dari steam saat Ts bisa didapatkan dari steam table.  Entalpi dari umpan feed (F) – larutan dengan konsentrasi X – dalam tabel, jika tidak tersedia: Asumsi:  Bahwa feed sangat dilute (encer) sehingga panas laten penguapan 1 kg massa air dari larutan berair (aqueous) dapat diperoleh dari steam table menggunakan suhu larutan mendidih T1 (suhu evaporator).  Jika kapasitas panas (cp) dari liquid feed (umpan cair) diketahui  dapat digunakan untuk menghitung entalpi (abaikan panas pelarutan).
  • 13. Contoh: A continuous single-effect evaporator concentrates 9072 kg/h of a 1.0 wt % salt solution entering at 38ºC to a final concentration of 1.5 wt %. The vapor space of the evaporator is at 101.325 kPa (1.0 atm abs) and the steam supplied is saturated at 150 kPa. The overall coefficient U = 1704 W/m2.K. Calculate the amounts of vapor and liquid products and the heat-transfer area required. Assumed that, since it its dilute, the solution has the same boiling point as water. Data: The latent heat of steam at 150 kPa 383.2 K = 2230 kJ/kg (958,8 Btu/h) The latent heat of water at 101.325 kPa 373,2 K= 2257 kJ/kg (970,3 Btu/h)
  • 14. Penyelesaian Diketahui: F = 9.072 kg/h xF = 1 wt % = 0,01 kg solute / kgfeed TF =38°C = xL = 1,5 wt% = 0,015 kg solute / kg liquid product P = 101,325 kPa (1.0 atm abs) PS = 150kPa U = 1704 W/m2.K T1 = saturated temperature at P (= 101,325 kPa) = 100°C TS = saturated temperature at 150 kPa = 111,4°C
  • 15. Penyelesaian Steam, S PS, TS, HS Feed, F xF, TF, hF Condensate, S PS, TS, hS Vapour, V yV, T1, HV Concentrate, L xL, T1, hL P T1 Ditanya: V=? L=? A=?
  • 16. Penyelesaian NM total, F = L + V 9.072 = L + V NM solute, F xF = L xL 9.072 (0,01) = L (0,015) L = 6.048 kg/h of liquid Maka, V = 3.024 kg/h of vapor
  • 17. Penyelesaian Asumsi: larutan sangat encer (as water); cpF = 4,14 kJ/kg. K (Table A.2-5) Dari soal: At P1 = 101,325 kPa, T1 = 373,2 K (100°C) (datum temperature). HV = 2.257 kJ/kg. At PS = 143,3 kPa, TS = 383,2 K (110°C).  = 2.230 kJ/kg. Maka, entalpi umpan dapat dihitung, hF = cpF (TF – T1) hF = 4,14 (311,2 – 373,2) = -256,68 kJ/kg.
  • 18. Penyelesaian F hF + S  = L hL + V HV with hL = 0, karena T datum adalah 373.2 K. 9.072 (-257,508) + S (2.230) = 6.048 (0) + 3.024 (2.257) S = 4.108 kg steam /h Panas (q) yang dipindahkan melalui luas permukaan panas A, q = S () q = 4.108 (2.230) (1.000 / 3.600) = 2.544.000 W Luas permukaan panas (A); q = U A T = U A (TS – T1) 2.544.000 = 1704 A (383,2 – 373,2) A = 149,3 m2 Neraca Panas
  • 19. Penyelesaian Maka, V = 3.024 kg/h of vapor L = 6.048 kg/h of liquid A = 149,3 m2
  • 20. Pengaruh variable proses terhadap operasional evaporator  Suhu aliran umpan memiliki efek besar pada operasi evaporator.  Saat umpan tidak berada pada titik didihnya, uap pertama-tama diperlukan untuk memanaskan umpan ke titik didihnya lebih dahulu, baru kemudian mengalami proses penguapan.  Pemanasan awal umpan dapat mengurangi besarnya area perpindahan panas evaporator akibat hal tersebut. suhu umpan:
  • 21.  Tekanan dalam evaporator menentukan titik didih larutan (T1).  Tekanan uap menentukan suhu uap (Ts)  Karena q = U A (TS - T1), maka semakin besar selisih (TS - T1) akan membantu mengurangi area perpindahan panas yang dibutuhkan  mengurangi biaya.  Dapat dilakukan dengan memanfaatkan efek tekanan. Tekanan:
  • 22. Boiling Point Rise  Dalam contoh 1, larutan diasumsikan cukup encer sehingga dianggap memiliki sifat termal yang sama dengan air.  Hal tersebut tidak selalu benar.  Untuk larutan dengan konsentrasi tinggi  terdapat kenaikan titik didih larutan  Aturan Duhring (Duhring Law) adalah hukum empiris hubungan antara titik didih larutan dan titik didih pelarut pada tekanan yang berbeda untuk tiap konsentrasi larutan – perkiraan kenaikan titik didih larutan.
  • 23.
  • 24. Contoh  Pressure in an evaporator is given as 25,6 kPa (3,72 psia) and a solution of 30% NaOH is being boiled.  Determine the boiling temperature of the NaOH solution and the boiling- point rise (BPR) of the solution over that of water at the same pressure.
  • 25. Penyelesaian:  Cari titik didih air pada P soal  25,6 kPa (3,72 psia)  Steam table, boiling point of water at 25,6 kPa is 65,6°C (Tsat)  Dari TD air, dicari titik didih untuk larutan 30% NaOH di fig.8-4  Untuk TD air 65,6°C (150°F) and 30% NaOH  titik didih larutan NaOH tersebut adalah 79,5°C (175°F).  Menghitung BPR  The boiling-point rise = 79,5°C – 65,6°C = 13,9°C (25°F)
  • 26. Enthalpy-Concentration Chart Heat of solution – Panas pelarutan  Panas yang dihasilkan atau diserap ketika suatu zat melarut (terbentuk sebuah larutan).  Jumlah panas yang terlibat ketika satu mol atau satu gram larut dalam pelarut mengalami pelarutan.  Jumlah panas bergantung pada jenis senyawa, dan jumlah air yang digunakan untuk melarutkan.  Contoh pada proses pelarutan pellet NaOH.
  • 27.
  • 28. Latihan! An evaporator is used to concentrate 4.536 kg/h of a 20 % solution of NaOH in water entering at 60ºC to a product of 50 % solid. The pressure of the saturated steam used is 172,4 kPa and the pressure in the vapor space of the evaporator is 11,7 kPa. The overall heat-transfer coefficient is 1.560 W/m2.K. Calculate the steam used, the steam economy in kg vaporized/kg steam used, and the heating surface area in m2.
  • 29. Latihan! Buatlah diagramnya terlebih dahulu! U = 1560 W/m2 T1 A = ? P1 = 11,7 kPa F = 4.536 kg/h TF = 60°C xF = 0,2 hF. S = ? TS , HS PS = 172,4 kPa L, T1 , hL xL = 0,5 S, TS , hS V, T1 , yV , HV
  • 30. Penyelesaian? NM total, F = L + V 4.536 = L + V NM solute, F xF = L xL 4.536 (0,2) = L (0,5) L = 1.814 kg/h of liquid Maka, V = 2.722 kg/h of vapor
  • 31. Penentuan T1 = Tsat + BPR of the 50% concentrate product.  Tsat air dari steam table. Pada 11.7 kPa, Tsat = 48,9ºC.  Dari grafik Duhring (Fig. 8.4-2), untuk Tsat = 48,9 ºC and 50 % NaOH , titik didih dari larutan adalah T1 = 89,5ºC. BPR = T1 - Tsat = 90 – 48,9 = 40,6ºC  From the enthalpy-concentration chart (Fig.8.4-3), for TF = 60ºC and xF = 0,2 get hF = 214 kJ/kg. T1 = 90ºC and xL = 0,5 get hL = 505 kJ/kg. Penyelesaian?
  • 32. Penyelesaian?  For saturated steam at 172,4 kPa, from steam table, we get TS = 115,6 ºC and  = 2.214 kJ/kg.  To get HV for superheated vapor, first we obtain the enthalpy at Tsat = 48,9ºC and P1 = 11,7 kPa, get Hsat = 2.590 kJ/kg. Then using heat capacity of 1.884 kJ/kg.K for superheated steam. HV = Hsat + cp.BPR = 2.590 + 1,884 (40,6) = 2.667 kJ/kg.  Substituting into heat balance equation and solving for S, F hF + S  = L hL + V HV 4.535 (214) + S (2.214) = 1.814 (505) + 2.722 (2667) S = 3.255 kg steam /h. Atau bisa langsung cari Hv di steam table untuk superheated; T1 = 89,5ºC P = 11,7 kPa
  • 33. Penyelesaian?  The heat q transferred through the heating surface area, A is q = S () q = 3.255 (2.214) (1.000 / 3.600) = 2.002.000 W  Solving for capacity single-effect evaporator equation; q = U A T = U A (TS – T1) 2.002.000 = 1.560 A (115,6 – 89,5)  Solving, A = 49,2 m2 Steam economy = 2.722/3.255 = 0,836
  • 34. Tugas