Homework #6 Do problems 18.1, 18.2, 18.3, 18.4, 18.5 on page 417. CBEN 408 Spring 2016 -1- May 3, 2016 Solutions Problem #18.1, 18.2, & 18.3 (10 to points) How much HHV energy (in Btu or PJ) is contained in the cargo aboard a 145,000 m3 LNG carrier? Assume the LNG has a relative density of 0.45, a molar mass of 18 and a heating value of 1,000 Btu/scf (39.4 MJ/Nm3). What is the value of the cargo in Exercise 18.1 if the fuel is priced at $5.00 per MMBtu ($4.75/GJ)? What is the equivalent volume of gas (in scf [Nm3]) of the cargo in Exercise 18.1? Solution The table below shows all of the intermediate calculations using U.S. Customary units. The cargo has an HHV content of 3.0 TBtu (3.0 million MMBtu = 3.01012 Btu), has a value of $14 million, and is equivalent to 3.0Bscf (3.0109 scf). The calculation is converting from volume to number of moles. The value of relative density is for the density at the storage conditions but is related to the density of water its standard conditions (60°F & 1 atm), 63.3665 lb/ft3). So: 145000 m3 0.45 62.3665 lb 3 ft 3 m 0.3048 * ft V V NG w N lb M M 18 lb.mol 6 7.98 10 lb.mol All other values are derived from here. CBEN 408 Spring 2016 -2- May 3, 2016 Problem #18.4 (5 points) An LNG-receiving terminal sends gas to the pipeline at 1,000 psig (70 barg). The LNG is essentially pure methane and is stored in a tank at 2 psig. What is the pump energy (hp, MW) required to send out 400 MMscfd (10.7 × 106 Nm3/d) of gas to the pipeline at 40°F (4.4°C). Assume a pressure drop through the vaporizer of 20 psi (1.4 bar) and a pump efficiency of 70%. (See Chapter 2 for pumps). Solution The BFD for this process is shown below. Note that all of the pressure increase comes from pumping the cryogenic liquid. Sufficient pressure is required to overcome any of the other process pressure drops (i.e., the pressure drop across the Revaporizer). The results are shown in the following table. Liquid @ 1020 psig Gas @ 1000 psig Liquid @ 2 psig Storage Tank Revaporizer Pump Rather than trying to use the PH diagram for methane to do these calculations (since following lines for constant entropy is extremely difficult when dealing with a liquid) we will use the Bernoulli equation: P Wˆ s The values for the methane properties were obtained from Table B.21 of the text book. The actual values were obtained by linear interpolation of the appropriate values at the inlet pressure, 2 psig = 16.7 psia. For this pumping: lbf in2 1020 2 144 in2 ft 2 ft lbf P Wˆ s 5590 lb lbm 26.23 m2 ft Next, we need the mass flowrate to determine the total pumping power: CBEN 408 Spring 2016 -3- May 3, 2016 6 scf 400 10 day lbm lb lb 16.042 m NM 16.9 106 m 195.7 m lb.mol day sec 379.49 scf lb.mol So the required power @ 100% efficiency is: lb ft lbf Ws mWˆ s 195.7 m 5590 sec lbm ft lbf Btu 1,094,000 1,406 1,989 hp sec sec Since the pump efficiency is 70% then: Wact Ws 1,989 hp 2,841 hp 0.7 How do these calculations compare to the results for HYSYS? The PFD below shows a simple simulation using BWRS for the methane properties. The hand calculation is just 0.6% higher than that calculated in HYSYS. This corresponds to the 0.6% difference in the liquid densities. CBEN 408 Spring 2016 -4- May 3, 2016 Problem #18.5 (10 points) The LNG terminal in Exercise 18.4 uses seawater to heat LNG from storage temperature for send out. For a gas send out rate of 400 MMscfd (10.7 x 106Nm3/d) and using fresh water properties: a) What water flow rate (lbm/h, kg/h) is required to heat the LNG, assuming an inlet water temperature of 50°F (10°C) and an outlet water temperature of 40°F (4°C)? b) What is the hp (kW) required to lift the water 50 feet (15 m) above sea level to the vaporizer assuming a pump efficiency of 80%? Solution The BFD for this process is shown below. Note that the duty in the Revaporizer will depend on how hot the methane can be warmed; if we assume that the heat exchanger can be designed with a 10°F approach temperature then the outlet temperature will be 40°F (i.e., water inlet temperature minus the approach temperature). The results are shown in the following table. 40°F 50°F 40°F 50 ft Revaporizer Pump Methane: -258°F Sea water The methane properties are determined from the P-H diagram in the textbook, Figure B.24. We will use the Bernoulli equation to determine the amount of work required to lift the seawater up 50 ft: g Wˆ s h gc The rate of seawater needed is determined form an energy balance around the Revaporizer: CBEN 408 Spring 2016 -5- May 3, 2016 Q mgas mwater Hˆ gas,out Hˆ gas,in mwaterCˆ p ,water Tin Tout mwater mgas Hˆ gas,out Hˆ gas,in Cˆ p ,water Tin Tout Btu 6 lb 16.9 10 day 365 45 lb lb lb 541 106 6,260 day sec Btu 1 lb °F 50 40 °F For this pumping: g Wˆ s h 50 ft gc ft sec2 50 ft lbf lb ft lbm 32.2 m 2 lbf sec 32.2 So the required power @ 100% efficiency is: lb ft lbf Ws mWˆ s 6260 m 50 sec lbm ft lbf Btu 313,000 402 569 hp sec sec Since the pump efficiency is 80% then: Wact Ws 569 hp 712hp 0.8 How do these calculations compare to the results for HYSYS? The PFD below shows a simple simulation using BWRS for the methane properties & ASME steam tables for the water properties. The hand calculation is just 0.5% lower than that calculated in HYSYS. This is due to the difference in the Revaporizer duty; the major contribution to this is that the hand calculation has a duty that is 0.6% lower than that from HYSYS. Further note that HYSYS does not allow one to specify the hydraulic “head” on the pump; but, we can specify the pressure change necessary to overcome this head. This will be: ft 32.2 lb g sec2 P h 62.40 m3 50 ft gc ft 32.2 lbm ft lbf sec2 CBEN 408 Spring 2016 -6- 1 in2 144 ft 2 lb 21.67 2f . in May 3, 2016 CBEN 408 Spring 2016 -7- May 3, 2016