9 multi stage regenerative cycles

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7/22/2019 9 Multi Stage Regenerative Cycles http://slidepdf.com/reader/full/9-multi-stage-regenerative-cycles 1/3 5.9 Multi–Stage Regenerative Cycles: 10 I  II  III  IV BOILER 9 8 7 11 6 7 5 12 3 4 5 m 1  (m 1 +m 2 ) m 1 m2  13  m 3  14 2  1 PUMP 2 (1-m 1 -m 2 -m 3 ) (m1+m2+m3) x 3 PUMP TURBINE  Fig.5.9(a). Three stage regenerative cycle T s 1 2 4 3 5 6 8 7 9  10 11 12 13 14 1 kg m 1 m 1 +m 2 (m 1 +m 2 +m 3 ) (1-m 1-m2-m3) (1-m 1 ) (1-m 1 -m 2 ) (1-m 1 -m 2 -m 3 ) 1 kg  Fig.5.9(b). T-s diagram

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Page 1: 9 Multi Stage Regenerative Cycles

7/22/2019 9 Multi Stage Regenerative Cycles

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5.9 Multi–Stage Regenerative Cycles:

10I   II   III   IV

BOILER

98

711

6

7

512

3

4

5

m1   (m1+m2)

m1 m2   13   m3  14

2   1

PUMP

2

(1-m1-m2-m3)

(m1+m2+m3)

x3

PUMP

TURBINE

 

Fig.5.9(a). Three stage regenerative cycle

T

s

1

2

4

3

5

6

8

7

9   10

11

12

13

14

1 kg

m1

m1+m2

(m1+m2+m3)

(1-m1-m2-m3)

(1-m1)

(1-m1-m2)

(1-m1-m2-m3)

1

kg

 

Fig.5.9(b). T-s diagram

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 Above figure shows an arrangement in which there are 3 stages of feed water heating

employing closed heaters. Steam to the 1st, 2nd and 3rd heaters is supplied at states 11,

12 and 13 respectively. The feed water leaving each heater is at the saturation

temperature corresponding to the pressure of bled steam supplied to that heater. The

corresponding T-s diagram for the cycle is shown above.

Considering one kg of steam leaving the boiler and entering the turbine at state 10.

Let, m1 = mass of steam supplied to 1st heater.

m2 = mass of steam supplied to 2nd heater.

m3 = mass of steam supplied to 3rd heater.

Heat balance for 1st heater gives,

1 11 7 7 6 7 5m (h - h ) = (h - h ) (h - h )≈  

7 51

11 7

(h - h )m

(h - h )=  

Heat balance for 2nd heater gives,

4 2 12 1 7 5 5 1 2h m h m h h h (m m )+ + = + +  

2 12 5 5 4 1 5 7m (h - h ) (h - h ) m (h - h )= +  

5 3 1 7 52 4 3

12 5

(h - h ) - m (h - h )m = ; (h h )

(h - h )

≈Q  

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 Also, heat balance for 3rd heater + drain cooler, gives,

3 13 1 2 5 2 1 2 3 2 3m h (m m )h h (m m m ) h h+ + + = + + +  

3 13 1 2 5 1 2 3 2 3m h (m m )h (1 - m - m - m )h h+ + + =  

3 13 2 3 2 1 2 5 2m (h - h ) (h - h ) - (m m )(h - h )= +  

3 13 1 3 1 1 2 5 1m (h - h ) (h - h ) - (m + m )(h - h )≈  

3 1 1 2 5 13

13 1

(h - h ) - (m m )(h - h )m

(h - h )

+=  

( )   ( )10 11 1 11 12 1 2 12 13

1 2 3 13 14

h - h 1 - m (h - h ) (1 - m - m )(h - h )Turbine work

(1 - m - m - m )(h - h )

⎧ ⎫+ +⎪ ⎪= ⎨ ⎬

+⎪ ⎪⎩ ⎭ 

10 14 1 11 14 2 12 14 3 13 14(h - h ) - m (h - h ) - m (h - h ) - m (h - h )=  

10 7Heat sup plied (h - h )=  

work done 

Heat supplied η =  

( ) ( )10 11 1 11 12 1 2 12 13

1 2 3 13 14

10 7

h - h 1 - m (h - h ) (1 - m - m )(h - h )

(1 - m - m - m )(h - h ) 

(h - h )

⎧ ⎫+ +⎪ ⎪⎨ ⎬

+⎪ ⎪⎩ ⎭η =