Introduction to Steam

  1. Effective Use of Steam and Steam Traps

     
    1. Effective Use of Condensate Heat

 

    1.  

      After the latent heat energy in the steam is released, steam is condensed, and changes to condensate. Condensate which is generated in various process equipment and heat transfer devices must be promptly discharged. If the condensate remains stagnant in this equipment, it may cause a decrease in heat-transfer efficiency and water-hammer when restarting operations. However, the discharged high temperature condensate has a lot of energy (sensible heat), and so is worth reusing.

       

      The use of condensate heat falls into the following three categories.

       
      • Use of flash steam

      • Use of sensible heat with thermostatic steam traps

      • Condensate recovery

 

 

        1. Use of flash steam

         

        As described in “Flash steam”, some condensate will re-evaporate when it enters a low-pressure environment from a high-pressure environment, and becomes flash steam. The flash steam and steam produced from the boiler remains steam and this can be used as latent heat. The condensate from a high temperature heat transfer device is led to a flash tank set to an appropriate pressure, create flash steam, which is often used in low temperature heat transfer devices. In addition, condensate discharged from steam traps partially re-evaporates, and is used in the same way as described previously.

         

        Figure 5.1 shows an example of a boiler factory. Condensate from a steam air pre-heater re-evaporates in a flash tank, and the created flash steam is provided to deaerator, with the rest of condensate being supplied to a low temperature feed water heater.

        Please refer to Table 5.1 and 5.2 for the rate and the volume of flash steam generated in flash tanks.

         

        Figure 5.1 Use of flash steam in boiler factory.png

         

        Figure 5.1 Use of flash steam in a boiler factory

         

        Table 5.1 The amount of flash steam (%)

        High-pressure side-pressure
        (MPa)

        Flash tank pressure (MPa)

        0

        0.03

        0.05

        0.1

        0.15

        0.2

        0.3

        0.4

        0.5

        0.6

        0.8

        1.0

        1.2

        1.4

        1.6

        1.8

        0.1

        3.7

        2.5

        1.7

        0.2

        6.2

        5.0

        4.2

        2.6

        1.2

        0.3

        8.1

        6.9

        6.1

        4.5

        3.2

        2.0

        0.4

        9.7

        8.5

        7.7

        6.1

        4.8

        3.6

        1.6

        0.5

        11.0

        9.8

        9.1

        7.5

        6.2

        5.0

        3.1

        1.4

        0.6

        12.2

        11.0

        10.3

        8.7

        7.4

        6.2

        4.3

        3.0

        1.3

        0.8

        14.2

        13.1

        12.3

        10.8

        9.5

        8.3

        6.4

        4.8

        3.4

        2.2

        1.0

        15.9

        14.8

        14.2

        12.5

        11.2

        10.8

        8.2

        6.6

        5.3

        4.0

        1.9

        1.2

        17.4

        16.3

        15.5

        14.0

        12.7

        11.6

        9.8

        8.2

        6.9

        5.7

        3.5

        1.7

        1.4

        18.7

        17.6

        16.9

        15.4

        14.1

        13.0

        11.2

        9.6

        8.3

        7.1

        5.0

        3.2

        1.5

        1.6

        19.0

        18.8

        18.1

        16.6

        15.3

        14.3

        12.4

        10.9

        9.6

        8.4

        6.3

        4.5

        2.9

        1.4

        1.8

        21.0

        19.9

        19.2

        17.7

        16.5

        15.4

        13.6

        12.1

        10.8

        9.6

        7.5

        5.7

        4.1

        2.7

        1.3

        2.0

        22.0

        20.9

        20.9

        18.8

        17.5

        16.5

        14.7

        13.2

        11.9

        10.7

        8.7

        6.9

        8.3

        3.8

        2.5

        1.2

         

        Table 5.2 The volume of re-evaporated steam (m3)

        High-pressure side-pressure
        (MPa)

        Pressures in flash tank (MPa)

        0

        0.03

        0.05

        0.1

        0.15

        0.2

        0.3

        0.4

        0.5

        0.6

        0.8

        1.0

        1.2

        1.4

        1.6

        1.8

        0.1

        61

        33

        20

        0.2

        103

        67

        50

        23

        9

        0.3

        135

        93

        72

        41

        23

        12

        0.4

        161

        115

        91

        55

        35

        22

        8

        0.5

        184

        133

        107

        68

        45

        31

        14

        5

        0.6

        203

        149

        122

        78

        54

        38

        20

        11

        4

        0.8

        237

        176

        145

        97

        70

        51

        30

        13

        11

        6

        1.0

        266

        199

        168

        113

        82

        62

        39

        25

        17

        11

        4

        1.2

        290

        219

        183

        126

        93

        72

        46

        31

        22

        16

        8

        3

        1.4

        312

        237

        199

        139

        103

        80

        53

        37

        27

        20

        11

        6

        2

        1.6

        332

        254

        214

        150

        112

        88

        59

        42

        31

        23

        14

        8

        4

        2

        1.8

        351

        269

        227

        160

        121

        95

        64

        46

        35

        27

        16

        10

        6

        4

        2

        2.0

        368

        279

        238

        170

        128

        102

        69

        50

        38

        30

        19

        12

        8

        5

        3

        1


         
        1. Use of sensible heat through the use of thermostatic steam traps

         

        A steam trap is a device that rapidly discharges generated condensate to outside of the system. Generally, the faster the condensate is discharged, the better its performance. We have found disadvantages, but no advantages to allowing condensate to remain in the system.

         

        In the early 1970s, MIYAWAKI INC. developed a thermostatic steam trap that actively utilizes the sensible heat of the condensate by letting it stay in the trap, even though that is contrary to common sense. This was a revolutionary steam trap at that time because steam traps have a mechanism for setting appropriate condensate discharging temperature (clearly lower than the saturation temperature) in advance, and not discharging the condensate while it is above that temperature. In the midst of the first oil crisis and the rapidly growing awareness of the need for "energy saving," this temperature control trap was adopted one after another for steam tracing lines in factories, or replaced disk traps, etc., and this established its existence as an "energy-saving trap" in no time.

         

        The main features of thermostatic steam traps are as follows.

         
        • Use condensate heat (sensible heat) effectively, especially for steam trace lines.

        • There is no steam leakage because a condensate seal is formed on the primary side of the steam trap body.

        • There is no (or little) flash steam because the temperature of condensate discharging is low.
          It has the following benefits for steam trap performance
          ・ Reduces the erosion in valves and it has good durability
          ・ The condensate flow passage area on the secondary side of the steam trap outlets becomes substantially larger, and the size of condensate line piping can be reduced accordingly

         

        Figure 5.2 shows the rate of steam saved by using latent heat.
        For instance, when the condensate discharging temperature is set to 70℃ in 0.5 MPa (saturated steam temperature is 159 ℃), the rate of steam saved is approximately 15 % compared to the case when discharging condensate at saturated steam temperature.

         

        Figure 5.2.png

         

        Figure 5.2 Condensate discharging temperature and the rate of steam saved

        1. Condensate recovery

         

        Condensate generated in steam system equipment is taken to the condensate discharging line. It is desirable both economically and environmentally that the condensate does not flow away, but is reused. There are several ways to reuse the condensate, and here we will discuss the recovery of the condensate into the boiler feedwater tank. The feature of this recovery and utilization is that the condensate itself is also reused.

         

        A boiler is a type of equipment for heating and evaporating water at high pressure and discharging the created condensate to steam transport lines. Water must always maintain sufficient quality to be used in the boiler, and this is treated with chemical materials used for processing. Then, the water quality is checked and recovery treatment is performed if a decrease in the quality of water is detected. This treatment is called blowdown.

         

        Thus steam creation in a boiler requires costs for fuel, as well as for water treatment agents and so on. The greater the number of blowdowns, the more boiler water and the other energy it contains will be disposed of. Condensate is virtually pure water after it has been treated and distilled. Thus, it is ideal for use as boiler water. Condensate should be actively recovered and this can bring the following benefits

         
        • Reduction in water supply costs

        • Reduction in fuel costs

        • Increasing the efficiency of steam creation from boilers

        • Reduction in boiler blow downs, and energy loss

        • Reduction of water treatment costs

        The actual amount of effect varies from factory to factory and must be estimated independently, but the following example is helpful for estimating the approximate effect.

         

        Set the prerequisites as follows:

         

        (Precondition)

         
        The amount of boiler steam created :10,000kg/h
        Operating time :24 hours /day(8,760 hours /year)
        Temperature of boiler water supply :15℃
        Condensate temperature :90℃(all of them are discharged, but not recovered)
        Boiler supply water costs :50 yen/m3
        Boiler operation efficiency :85%
        Fuel cost (gas price) :2,000 yen/GJ(gigajour)(1.1 yen/kWh)
        (1GJ=1,000,000kJ)
         

        (Fuel cost)

         

        First, 1 kg of new raw water is needed for every 1 kg of unrecovered condensate. Calculate the cost of heating this raw water to 90°C. (⊿T=90℃-15℃=75℃) The amount of heat for increasing raw water temperature can be calculated according to the following formula.

         

        Q=m×Cp×⊿T

         

        Here,

        Q :Amount of heat(kJ)
        m :Mass of material(kg)
        Cp :Specific heat of material(kJ/kg℃) (Specific heat of water is 4.19kJ/kg℃)
        ⊿T :Increased temperature of material(℃)
         

        In this example, m, Cp, ⊿T are 1kg, 4.19kJ/kg℃, 75℃, respectively. These values can be substituted in the formula as follows.

         

        Q=1kg×4.19kJ/kg℃×75℃=314kJ

         

        This is the amount of heat per unit mass.

         

        Since this is the amount of heat per unit mass, we can calculate the annual heat requirement as 314 kJ/kg.

         

        10,000kg/h×314kJ/kg×8,760h/year=27.506GJ

         

        As the boiler efficiency is 85%, the actual amount of required heat can be calculated as below

         

        27,506GJ/0.85=32,360GJ/year

         

        Using the fuel cost (gas price) of 2,000 yen per GJ, the annual fuel cost is

         

        32,360GJ/year ×2,000 yen/GJ=64,720,000 yen/year

         

        (raw water price)

         

        Next is the supplied water (raw water) cost. The price of water is determined by volume, and the density of ambient water is around 1,000kg/m3. Thus, the required annual amount of supplied water for which condensate is not recovered is as shown below.

         

        (8,760h/year ×10,000kg/h)/(1,000kg/m3)=87,600m3/year

         

        The annual cost is calculated by multiplying this by the boiler supplied water cost of 50 yen/ m3 as follows.

         

        87,600m3/year ×50 yen/m3=4,380,000 yen/year

         

        The sum of fuel cost and raw cost is as shown below.

         

        64,720,000+4,380,000=69,100,000 yen/year

         

        In this example, the costs saved in only fuel and water alone is nearly 70 million yen, and this is a significant amount. In addition, the efficiency of condensate recovery is much greater if we consider water treatment costs, blowdown reduction cost, and condensate discharge costs. However, in this example, as the calculation assumes 100% recovery efficiency for thermal energy, it is necessary to accurately estimate recovery efficiency.