Sage Journals: Discover world-class research

Abstract

Air-temperature vaporizer is the main equipment of LNG satellite station vaporization process, and the core equipment of the whole supply system, whose vaporization capacity decides the gas supply scale of LNG satellite station. The heat transfer effect of finned tube mostly affects the vaporization capacity of air-temperature vaporizer and also affected by many factors such as ambient temperature. Therefore, this research aims to study the heat transfer of finned tube in air-temperature vaporizer. With the actual case calculated and analyzed, the research has established the mathematical model of heat and mass transfer based on MATLAB program, with which the required length of finned tube is calculated. On comparing the results of simulation with actual ones, the reliability of the model is verified. According to the studies of the effects of air temperature, fin height, number of fins, and vaporization of LNG on the heat transfer process, the search sums up that the heat transfer performance of finned tube increases with the increase in air temperature, fin height, and vaporization of LNG although the effects are not obvious. The research has also calculated the length of finned tubes under different operating conditions. By comparing the outlet temperatures, the research summarizes that the most appropriate number of fins is 8.

Keywords

LNG satellite station air-temperature carburetor heat transfer effect MATLAB mathematical model

Introduction

Air-temperature vaporizer is the main equipment of LNG satellite station vaporization process, in which LNG goes through the gas–liquid two-phase area, namely, boiling heat transfer two-phase flow area. With the finned tube being one of the most important parts of air-temperature vaporizer, boiling heat transfer two-phase flow and vaporization capacity are critical factors that affect the heat transfer effect.

There are several studies on air-temperature vaporizer in LNG satellite stations while most of which mainly research the heat transfer area. Therefore, this research aims at studying the effects of boiling heat transfer two-phase flow and vaporization capacity of finned tubes.

Boiling heat transfer two-phase flow

The heat transfer process of boiling heat transfer two-phase flow is more complex, so it becomes a hot topic in the same research. At present, there are many researches on boiling heat transfer two-phase flow, and many experimental correlations are proposed. In 1966, Chen J C first studied the boiling heat transfer two-phase flow. Through experimental research and suitable calculation method, the heat transfer law of boiling heat transfer was obtained, and finally the Chen¹ relation was obtained. In 1986, KE Gungor and Winterton² analyzed the experimental data and summarized the characteristics and laws of the boiling heat transfer of organic medium, and got the Gungor–Winterton relation. In 2007, SL Qi et al.³ used liquid nitrogen as the object of study, conducted an experimental study on the horizontal tube boiling heat transfer, and analyzed that liquid nitrogen flow patterns were mainly wavy and slug flow; analysis of the relationship between Klimenko and Klimenko⁴ is a relatively accurate correlation, while Shah and Chen’s correlations show a low heat transfer coefficient. In 2000, L Cheng and Chen⁵ used kerosene as the research object, and the heat transfer process was studied by experimental method. Six different boiling heat transfer relations were analyzed, and finally the two relations with the lowest error were obtained, which is known as Shah and Kandlikar relation. In 2008, SM Wang et al.⁶ analyzed the mechanism of boiling heat transfer, modified the bubble parameter model in the supercooled boiling model, and obtained the subcooled boiling calculation model for liquid nitrogen. In 2009, M Gong et al.⁷ studied the heat transfer process of pool boiling by experimental method, and analyzed the effect of ethane and propane on the heat transfer effect, and compared the experimental results with the calculation results of existing relational formulas. In 2010, XD Li⁸ used liquid nitrogen as the object of study, and liquid nitrogen in the vertical tube flow boiling heat transfer established a two-fluid model, obtained by gas–liquid phase transmission law, and the numerical results coincide with Klimenko’s the experimental measurements. In 2010, the MUSIG model was used to calculate the subcooled boiling process of the cryogenic fluid. The subcooled boiling process of the liquid nitrogen in the vertical tube was simulated. The relationship between the size of the tube and the ratio of the void ratio and the instability of liquid nitrogen was studied.⁹ In 2011, Chen Shuping applied the multiphase mixture model to the simulation of the liquid nitrogen transformation process, and analyzed the heat transfer, pressure drop, and gas flow rate of the air-temperature carburetor with the inlet flow rate.¹⁰ In 2011, CC Yang¹¹ simulated the heat and mass transfer process of the LNG air-temperature carburetor, and calculated the heat transfer of the boiling heat transfer process with Klimenko’s heat transfer equation, and analyzed the effects of LNG and air temperature. Heat transfer process, the increase in methane content is conducive to air-temperature vaporizer heat transfer of the conclusion.

Finned tube heat transfer study

In 2007, with the longitudinal finned tube as the research object, the heat transfer process of natural convection was studied by numerical simulation and experiment. The structural parameters of finned tube and fin spacing were analyzed, which provides a theoretical basis for the design and construction of finned tube heat exchangers.¹² In 2009, M Wang et al.¹³ used the experimental method to study the heat transfer process of the circular finned tube heat exchanger installed in the wind tunnel, and the experimental results were fitted to obtain the heat transfer in a certain flow rate range. Coefficient and the resistance coefficient of the tube bundle provide the theoretical basis for the optimization design and selection of the finned tubes of the same type. In 2011, Li Dashu studied the heat transfer of longitudinal finned tubes, analyzed the calculation method of heat transfer coefficient under different heat transfer conditions, and put forward the design process of longitudinal finned tube heat exchanger. The case for the longitudinal finned tube heat exchanger design theory is to be verified.¹⁴

Through detailed study on heat and mass transfer process of air-temperature vaporizer, this research has acquired valuable conclusions, which will provide theoretical basis for design, construction, and operation of air-temperature vaporizers.

Theory

Analysis of heat and mass transfer process of air-temperature

The heat and mass transfer of the air cooled vaporizer is mainly divided into three parts: the natural convection heat transfer outside the tube, the heat conduction in the tube wall, and the convective heat transfer between the LNG and the finned tube, as shown in Figure 1. The heat and mass transfer in tube LNG and fin tube is a forced convection boiling heat transfer in the heat transfer process of the Zhang,¹⁵ and can be described as follows: LNG mixture enters at the bottom of the vaporizer, by constantly absorbing heat, the temperature gradually increases, when the temperature reaches the boiling point, liquid vaporization, the first is the low methane bubble group the air bubbles, then ethane and propane were vaporized, makes the liquid composition change; as the temperature continues to rise, when the mixture reaches the dew point, all liquid gasification gas after gasification, outflow from the upper part of the carburetor, the carburetor gas export and import of liquid components of the same. As can be seen in Figure 1, LNG in the finned tube gasification process consists of three parts, namely, liquid phase, gas–liquid two-phase region, and gas phase area.

Figure 1.

Schematic diagram of heat and mass transfer in finned tube.

Analysis of heat and mass transfer in gas/liquid phase

The single-phase gas/liquid region of LNG in finned tube can be considered as forced convection heat transfer without phase change.

Analysis of heat and mass transfer in gas–liquid two-phase region (boiling)

The gas–liquid two-phase flow in the finned tube of an air cooled vaporizer is a two-phase flow of boiling heat transfer. The heat transfer process of LNG is related to the flow pattern of fluid flow.^16–19 LNG from the bottom into the finned tube, along the length of the part to absorb external heat, continuous vaporization of bubbles, with the endothermic process continued, bubble formation and growth, gradually rising, jumping off, change the heat transfer process and the flow chart is shown in Figure 2.

Figure 2.

Heat transfer and flow pattern of forced convection boiling of cryogenic liquid in a vertical tube.

Figure 2 shows that when the fluid is in the A part, the temperature is lower than the bubble point temperature and the wall temperature is lower than the bubble point temperature; thus, no vaporization occurs, the fluid flow and single-phase liquid flow pattern for the same, forced convection heat transfer of the single-phase fluid, the heat transfer coefficient is relatively low; when the fluid is in the B part, the tube wall temperature is higher than the liquid bubble point temperature, on the wall of bubbles and gradually enter the mainstream region, this time in the subcooled boiling, the fluid flow pattern is a fine bubble, the heat transfer coefficient increases; when the fluid is in the C part, the temperature of the liquid reaches the saturation temperature, liquid vaporization bubble, the bubble is saturated boiling, fluid flow is still a fine bubble, the sudden increase in heat transfer coefficient; when the fluid is in the D part, the temperature of the liquid and the wall temperature are almost the same, the heat absorbed to the vaporization of liquid, so the percentage of bubbles increases, the flow pattern is slug flow, the main heat transfer for saturated bubble boiling heat transfer, heat transfer coefficient is relatively stable, but larger; when the fluid is in the E part, the temperature is the same as D part, the difference is that the fluid flow pattern for annular flow, heat transfer in forced convection heat transfer of liquid film; when the fluid is in the F part, temperature is the same as the D part, the difference is that the fluid flow pattern for entrainment-shaped annular flow, heat transfer in forced convection heat transfer of liquid film; when the fluid is in the G part, the liquid in the tube is almost completely evaporated, and the steam tube wall contact heat transfer, the tube wall temperature increases, air liquid by heating and evaporating, flow pattern as the mist, the heat transfer coefficient increases sharply; when the fluid is in the H area, all the droplet in the air evaporated, so the heat transfer in this area is a single-phase gas convection heat transfer, and the heat transfer coefficient is small.

Through the above analysis, the boundaries of the gas–liquid flow pattern and heat transfer mechanism are not completely consistent, the mechanism of heat tube popular transition region is the same, there is a close relationship between the changes of flow patterns and heat transfer coefficient of the fluid, the heat transfer coefficient of single-phase liquid zone is low, the heat transfer coefficient and large stable two-phase region, single-phase gas the minimum heat transfer coefficient.

Mathematical model of heat and mass transfer of air-temperature vaporizer

Before building the model, make assumptions about the model:

The composition and temperature of the natural gas in the carburetor are uniform everywhere;

It is considered that the heat transfer is fully developed;

The pressure is constant during the operation of the gasifier;

The fluid flow in a tube is approximated by a one-dimensional (1D) steady state;

The air outside the tube in the humid air, without considering the influence of frost.

The outside of the tube for the natural convection heat transfer of air, without considering the effect of the wind. Under the above assumptions, the overall model of heat and mass transfer of the air-temperature vaporizer is shown in Figure 3. The micro-model is shown in Figure 4.

Figure 3.

Heat transfer model of air-temperature vaporizer.

Figure 4.

The element model of air-temperature vaporizer.

Single-phase region

Convective heat transfer in tube

Energy conservation equation as shown in equation (1)

dQ = m c_{p} \frac{dT}{dx}

(1)

where dQ is the heat absorbed by micro-unit in unit time, W; m is the mass flow per unit time infinitesimal segment, kg/s; c_p is the specific heat capacity at constant pressure of fluid in tube, J/kg K; d_T is the fluid temperature inside the tube, K; and d_x is the length of the micro-element, m.

For forced convection heat transfer process, heat transfer equation for the Newton cooling formula, as shown in equation (2)

dQ = α dA (T_{w} - T_{f}) = α π D_{1} dx (T_{w} - T_{f})

(2)

dQ = 2 π λ dx \frac{({T'}_{w} - T_{w})}{\ln (D_{2} / D_{1})}

(3)

where α is the forced convection heat transfer coefficient, W/(m² K); D₁ is the diameter, m; T_w is the tube wall temperature, K; T_f is the fluid temperature, K.

Finned tube wall thermal conductivity

The heat conduction of the fin tube wall using Fourier’s law, where λ is the thermal conductivity of wall material, W/(m·K); $T'_{w}$ is the outer wall temperature of tube, K; D₂ is the outer diameter of tube, m.

Air side convection heat transfer

For air side convection heat transfer, Newton cooling formula, as shown in equation (4)

\begin{matrix} dQ = α_{0} dA (T_{0} - T'_{w}) \\ = α_{0} dx (T_{0} - T'_{w}) (π D_{2} - n δ_{1} + n (2 l + δ_{1}) w) \end{matrix}

(4)

where α₀ is air side natural convection heat transfer coefficient, W/(m² K); l is the fin height, m; δ₁ is the fin thickness, m; n is the number of single fin of finned tube; w is the fin efficiency; $T'_{w}$ is the inner wall temperature of tube, K; T₀ is the outside air temperature, K.

Two-phase region

The model of heat transfer and heat transfer in the air duct and tube wall of the two-phase region is basically the same as that of the single phase, but the heat transfer coefficient is different. For the gas–liquid two-phase convection heat transfer in the tube, it is more accurate to calculate the boiling heat transfer of Klimenko.

Boundary condition

Inlet fluid temperature

{T |}_{x = 0} = T_{in}

(5)

Outlet fluid temperature

{T |}_{x = L} = T_{out}

(6)

Inner wall temperature

{T' |}_{r = D_{1} / 2} = T_{w}

(7)

Outside wall temperature

{T' |}_{r = D_{2} / 2} = T'_{w}

(8)

Mathematical model of heat and mass transfer for air-temperature vaporizer

Discretization of equation

Convective heat transfer in tube

Q_{i} = m_{i} c_{pi} (T_{i + 1} - T_{i})

(9)

T_{fi} = \frac{T_{i + 1} + T_{i}}{2}

(10)

Q_{i} = α_{i} π D_{1} Δ l ({T_{w}}_{i} - T_{fi})

(11)

Finned tube wall heat conduction

Q_{i} = 2 π λ Δ l \frac{({T'}_{w}_{i} - {T_{w}}_{i})}{\ln (D_{2} / D_{1})}

(12)

Natural convection heat transfer

Q_{i} = {α_{0}}_{i} Δ l (T_{0} - {T'_{w}}_{i}) (π D_{2} - n δ_{1} + n (2 l + δ_{1}) w)

(13)

Computation method

Based on the mathematical model of heat and mass transfer process in air-temperature vaporizer, this section separates the process into three parts, namely gas phase flow, gas–liquid two-phase flow, and liquid phase flow and calculated them with block diagram (Figure 5).

Heat and mass transfer calculation of gas phase flow and liquid phase flow

Assume that the micro-segment outlet temperature is T1(i + 1);

Calculate the external convective heat transfer coefficient cx0(i) using the empirical formula of the outside air, assuming the temperature Tw0(i) of the tube outer wall of the micro-element segment;

Calculate the wall temperature Tw1(i) according to the heat transfer formula of tube wall;

Calculate the convective heat transfer coefficient cx(i) according to the convective heat transfer criterion;

Calculate the temperature Tw2(i) of the inner wall of the tube according to the heat flux and the temperature of the fluid in the tube;

Calculate the absolute value of Tw2(i) − Tw1(i), if less than 0.1, then the assumed tube wall temperature is appropriate; otherwise, repeat step (2) until the assumed temperature is appropriate;

Calculate the absolute value of T2(i) − T1(i) if the micro-segment outlet temperature T2(i + 1) is calculated from the heat transfer quantity Q(i) of the micro-segment, if <0.1, temperature, otherwise repeat step (1) until the temperature is assumed to be appropriate;

For liquid phase flow, when the fluid temperature is higher than the bubble point temperature (Ts), the program ends. While for gas phase flow, when the fluid temperature is higher than the outlet temperature (Tout), the program ends.

Figure 5.

Flow diagram of gas phase flow and liquid phase flow.

Heat transfer calculation of fluid flow in gas–liquid two phase

Assuming the temperature Tw0 of the tube outer wall of the micro-element segment, the external convective heat transfer coefficient cx0 is calculated using the empirical formula of the outside air of the tube;

Calculate the micro-element heat Q, calculate the tube wall temperature Tw1 according to the heat transfer formula of the tube wall;

Calculate the convective heat transfer coefficient cx according to the convective heat transfer criterion;

Calculating the temperature Tw2 of the inner wall of the tube based on the heat flux and the temperature of the fluid in the tube;

Calculate the absolute value of Tw2 − Tw1, if less than 0.1, the assumed tube wall temperature is appropriate; otherwise, repeat step (1) until the assumed temperature is appropriate;

According to the length of heat transfer unit, calculate the length of two-phase gas–liquid phase (Figure 6).

Figure 6.

Diagram of fluid flow and heat transfer in gas–liquid two-phase flow.

Case study

Basic parameters

The parameters of the air-temperature carburetor of a LNG satellite station are shown in Table 1. The finned tube is made of aluminum alloy and the structure of the fin tube is shown in Figure 7. In actual operation, the inlet temperature of the fin tube is −162°C, and the outlet temperature is not lower than the ambient temperature of 5°C.

Table 1.

The parameters of the air-temperature carburetor of a LNG satellite station.

Items		Data
Single design vaporization (N m³/h)		1250
Working pressure (MPa)		1
The fin tube	Outer diameter (mm)	14
	Length (m)	15
	Number	18
	Inner diameter (mm)	10
	Height (mm)	80
	Thickness (mm)	3

Figure 7.

Finned tube structure parameters (unit: mm).

Calculation results and analysis

Based on the block diagram and calculation step introduced above, this section calculates the process of fluid interchange of liquid phase flow using the MATLAB program. The results are analyzed as follows:

1. The heat transfer coefficient of convection tube along the length of the change.

It can be seen from Figure 8 that the length of the fin tube is 13.8 m and the convective heat transfer coefficient is 2571.2 W/(m² K) in the gas–liquid two-phase region, the heat transfer coefficient in the liquid region is second, the convective heat transfer coefficient in the gas phase region is the smallest.

Figure 8.

The convective heat transfer coefficient with tube length.

2. The natural convective heat transfer coefficients along the air side of the tube vary along the tube length.

It can be seen from Figure 9 that the natural convection heat transfer coefficient of the out-of-tube air is the largest in the liquid phase and is in the range of 10–12 W/(m² K), and the heat transfer coefficient in the gas–liquid two-phase region is 10.56 W/(m² K), the gas phase region is the smallest, which is less than 11 W/(m² K).

Figure 9.

Variation of natural convection heat transfer coefficient of air outside the tube.

3. The overall heat transfer coefficient of fin tube along the tube changes.

It can be seen from Figure 10 that the total heat transfer coefficient of the finned tube is in the range of 160 W/(m² K), the total heat transfer coefficient is 95.75 W/(m² K). The total heat transfer coefficient in the gas phase is about 60–150 W/(m² K).

Figure 10.

Variation of overall heat transfer coefficient of finned tube with fin tube length.

In summary, the finned tube length of 13.8 m, and the actual length of 15 m, due to the actual process design will take into account a certain margin, so greater than the calculated length, can explain that the model has a certain reliability.

Discussion

There are many factors that affect the heat transfer of the air-temperature carburetor. The main factors are the temperature of the air outside the tube, the height, and the number of fins.

Effect of air temperature on heat transfer

The influence of different air temperature on the heat transfer is studied. The influence of different air temperature on the heat transfer coefficient is studied at different temperatures: 10°C, 0°C, 10°C, and 20°C.

Figure 11(a) shows that with the increase in the temperature of the air outside the tube, the tube heat transfer coefficient increases gradually, but increased, so the air outside the tube temperature of the fluid in the tube heat transfer coefficient is insensitive.

Figure 11.

Effect of temperature on different parameters: (a) convective heat transfer coefficient, (b) natural convection heat transfer coefficient, and (c) overall heat transfer coefficient.

Figure 11(b) shows that the with the increase in the air outside the tube temperature obviously, liquid phase and two-phase tube of the air side natural convection heat transfer coefficient increases gradually, the gas phase section of the air outside the tube side of the natural convection heat transfer coefficient decreases gradually, and in fact, liquid phase and gas phase, two phases increase because of the length of the starting point of gas phase section of the location is not the same; if the starting point is set to the same location, we can observe the gas phase is increased, thus increasing the temperature of the air outside the tube so that the air outside the tube side of the natural convection heat transfer coefficient increases, thereby affecting the total change thermal coefficient.

As can be seen from Figure 11(c), with the increase in air temperature outside the tube, the total heat transfer coefficient increases gradually, and the amplitude is larger.

Figure 11 shows, when the air temperature was −10°C and 0°C, 10°C and 20°C, the fin tube lengths were 15.88, 14.74, 13.8, 13.04, the length change is not large; therefore, the heat transfer performance of finned tube increases with the increase in air temperature, but the effect is not obvious.

Effect of fin height on heat transfer

In this article, the height of finned tube is studied with 75, 80, and 85 mm.

Figure 12(a) shows that with the increase in the temperature of the air outside the tube, the tube heat transfer coefficient increases gradually, but increased, so the air outside the tube temperature of the fluid in the tube heat transfer coefficient is insensitive.

Figure 12.

Effect of fin height on different parameters: (a) convective heat transfer coefficient, (b) natural convection heat transfer coefficient, and (c) overall heat transfer coefficient.

Figure 12(b) shows that with the increase in fin height, tube of natural convection heat transfer coefficient decreases, but the decline was not obvious, so there is a little impact on the change of height of fin tube of natural convection heat transfer coefficient.

According to Figure 12(c), the total heat transfer coefficient increases with the increase in fin height in the three regions.

We can see from Figure 12, when the fin heights were 75, 80, and 85 mm, fin tube required lengths are 14.98, 13.8, and 12.8 m, respectively, the change range is not large, so the heat transfer performance of finned tube with fin height increased, but the increasing effect is not obvious.

Effect of number of fins on heat transfer

The number of fins has a great influence on the heat transfer efficiency. The number of fins discussed in this article is 4, 8, and 12.

Figure 13(a) shows that with the increase in the number of fin tube, tube fluid convective heat transfer coefficient increases gradually, but the increase rate is smaller, thus increasing the number of fin tube fluid convection heat transfer coefficient is not very sensitive.

Figure 13.

Effect of fin number on different parameters: (a) convective heat transfer coefficient, (b) natural convection heat transfer coefficient, and (c) overall heat transfer coefficient.

Figure 13(b) shows that with the increase in the number of fins, the natural convection of the air outside the tube heat transfer coefficient decreased, and the decrease rate is not very big, so the effect of increasing the number of fin tube air natural convection heat transfer coefficient is not very sensitive.

Figure 13(c) shows that with the increase in the number of fins, the total heat transfer coefficient of fin tube increases, and increases greatly, this is because the increase in the number of fin tube increases the heat transfer area, and the heat transfer of finned tube to enhance.

We can see from Figure 13, when the number of fins were 4, 8, and 12, the fin tube lengths were 23.88, 13.8, and 10.12 m, respectively, while from 4 to 8 when the amplitude is large, but from 8 to 12 when the change is not great, so we should choose the number of finned tube to be 8.

Conclusion

This research has analyzed the heat and mass transfer process and established the mathematical model based on MATLAB program, with which the required length of finned tube was calculated and analyzed. According to the actual cases, the reliability of the model was verified and we can popularize this method of analyzing into studies in relative fields.

This research has studied the effects of the air temperature, fin height, fin number, and LNG evaporation on the heat and mass transfer process, and calculated the required length of finned tube under different working conditions. According to the studies, the search has summed up that the heat transfer performance of finned tube increases with the increase in air temperature, fin height, and vaporization of LNG although the effects are not obvious. The research has also calculated that the total heat transfer coefficient of fin tube increases greatly with the increase in the number of fins. By comparing the outlet temperatures, the research summarizes that the most appropriate number of fins is 8.

Footnotes

Academic Editor: Jun Ren

Declaration of conflicting interests

The author(s) declared no potential conflicts of interest with respect to the research, authorship, and/or publication of this article.

Funding

The author(s) received no financial support for the research, authorship, and/or publication of this article.

References

Chen

JC.

Correlation for boiling heat transfer to saturated fluids in convective flow. Ind Eng Chem Proc Des Dev 1966; 5: 322–329.

Gungor

Winterton

RHS

. A general correlation for flow boiling in tubes and annuli. Int J Heat Mass Tran 1986; 29: 351–358.

Zhang

Wang

RZ.

Review of liquid nitrogen flow boiling heat transfer. Cryog Supercond 2007; 34: 417–423.

Klimenko

VV.

Heat transfer intensity at forced flow boiling of cryogenic liquids in tubes. Cryog 1982; 22: 569–576.

Cheng

Chen

Comparison of six typical correlations for upward flow boiling heat transfer with kerosene in a vertical smooth tube. Heat Transfer Eng 2000; 21: 27–34.

Wang

Wen

. Numerical simulation for subcooled boiling process of liquid nitrogen in vertical tube. Chem Eng 2008; 36: 17–20.

Gong

Nucleate pool boilings of liquid methane and its natural gas mixtures. Int J Heat Mass Tran 2009; 52: 2733–2739.

XD.

Study of flow boiling and frost formation in vertical cryogenic star shaped fin tube. Shanghai, China: Shanghai Jiao Tong University, 2010.

Wen

Wang

YZ.

Numerical simulation for subcooled boiling process of low temperature fluid with MUSIG model. Chem Eng 2010; 38: 22–26.

10.

Chen

Han

Xie

. Numerical simulation of phase change heat transfer and flow for fin-tube vaporizer. Cryog Supercond 2012; 39: 52–56.

11.

Yang

CC.

Study on heat transfer calculation of LNG air temperature gasifier. Harbin, China: Harbin Institute of Technology, 2011.

12.

Qiu

Study on natural convection heat transfer characteristics and structural optimization of vertical finned tube. Jinan, China: Shandong University, 2007.

13.

Wang

Guo

. Experimental study on heat transfer and resistance of finned tube heat exchanger. In: Li

Zhu

(eds) Proceedings of the 8th international symposium on heating, ventilation and air conditioning. Berlin: Springer, 2012, pp.645–652.

14.

Qiu

Zhao

. Study on heat transfer computation and industrial application of longitudinal finned tube. Ind Heat 2011; 40: 30–32.

15.

Zhang

XZ.

Discussion on the application of air temperature vaporizer in LNG satellite station. China Chem Trade 2014; 31: 108.

16.

Zhang

Numerical analysis of heat transfer process in LNG ambient air vaporizer. Shanghai Gas 2014; 5: 1–4.

17.

Guo

Zhang

Guo

. Numerical simulation in the course of heat progress for rib-tube of open rack vaporizer. Petrochem Equip 2013; 42: 50–53.

18.

Jiao

Wang

HC.

Mechanism and calculation of heat transfer of LNG-AAV under frosting condition. Nat Gas Ind 2015; 35: 117–122.

19.

Klimenko

VV.

A generalized correlation for two-phase forced flow heat transfer-second assessment. Int J Heat Mass Tran 1990; 33: 2073–2088.

Analysis on heat transfer effect of air-temperature vaporizer in LNG satellite station

Abstract

Keywords

Introduction

Boiling heat transfer two-phase flow

Finned tube heat transfer study

Theory

Analysis of heat and mass transfer process of air-temperature

Analysis of heat and mass transfer in gas/liquid phase

Analysis of heat and mass transfer in gas–liquid two-phase region (boiling)

Mathematical model of heat and mass transfer of air-temperature vaporizer

Single-phase region

Convective heat transfer in tube

Finned tube wall thermal conductivity

Air side convection heat transfer

Two-phase region

Boundary condition

Mathematical model of heat and mass transfer for air-temperature vaporizer

Discretization of equation

Computation method

Heat and mass transfer calculation of gas phase flow and liquid phase flow

Heat transfer calculation of fluid flow in gas–liquid two phase

Case study

Basic parameters

Calculation results and analysis

Discussion

Effect of air temperature on heat transfer

Effect of fin height on heat transfer

Effect of number of fins on heat transfer

Conclusion

Footnotes

Declaration of conflicting interests

Funding

References