Performance Evaluation of Heat Transfer and Friction Factor Characteristics of Pipe in Pipe Fitted with Helical Screw Tape Insert of different Material. #1 Hemant P.Gawade, PG Student: Mechanical Engineering Department Padmabhooshan Vasantdada Patil Institute of Technology, Bavdhan, Pune-21(India) hemantgawade123@gmail.com Abstract— Experimental investigation on heat transfer and friction factor characteristics of circular tube fitted with helical screw inserts of equal length of different material twist ratio have been presented. The experimental data obtained were compared with those obtained from plain tube published data. In the present study would encompass all necessary activities for benchmarking the existing application like solar power plant with the current performance level and performance standards to be set for arriving at the objectives of the dissertation work. Recommendation of the best alternative would follow the comparison of the results. Data over Testing to be shared through a Test report for the experimentation phase. Key Words: Screw tapes; Thermal performance; Heat Transfer Performance. Introduction A heat exchanger is a device that is used to transfer thermal energy (enthalpy) between two or more fluids, between a solid surface and a fluid, or between solid particulates and a fluid, at different temperatures and in thermal contact. In heat exchanges, there are usually no external heat and work interactions. The basic concept of a heat exchanger is based on the premise that the loss of heat on the high temperature side is exactly the same as the heat gained in the low temperature side after the heat and mass flows through the exchanger. Heat exchanger simply exchangers the heat between those two sides, as a result it is decreasing the temperature of higher side and increasing the temperature of lower temperature side. Heat exchangers are used in different processes ranging from conversion, utilization & recovery of thermal energy in various industrial, commercial & domestic applications. Some common examples include steam generation, condensation in power & cogeneration plants, sensible heating & cooling in thermal processing of chemical, pharmaceutical & agricultural products, fluid heating in manufacturing & waste heat recovery etc. Increase in Heat exchanger’s performance can lead to more economical design of heat exchanger which can #2 Prof(Dr.). Rajendra K. Patil Professor: Mechanical Engineering Department Padmabhooshan Vasantdada Patil Institute of Technology, Bavdhan, Pune-21(India) rkpvpit@gmail.com help to make energy, material & cost savings related to a heat exchange process. The need to increase the thermal performance of heat exchangers, thereby effecting energy, material & cost savings have led to development & use of many techniques termed as Heat transfer Augmentation. These techniques are also referred as Heat transfer Enhancement or Intensification. Augmentation techniques increase convective heat transfer by reducing the thermal resistance in a heat exchanger. The technique of improving the performance of heat transfer system is referred to as heat transfer augmentation or intensification. This leads to reduce the size and cost of the heat exchanger. Heat transfer enhancement technology has been developed and widely applied to heat exchanger applications; for example, refrigeration, automotives, process industry, chemical industry etc. Many techniques of active and passive techniques are available for augmentation. Also heat augmentation techniques play a vital role for laminar flow, since the heat transfer coefficient is generally low in plain tubes. Vast literature is available on heat transfer augmentation studies in tube fitted with twisted tape in laminar flow. Helical screw-tape swirl flow generators shown in Fig. 1 is a modified form of a twisted tape wound on a single rod gives single way smooth direction of flow like screw motion. The present paper reports the heat transfer and friction factor characteristics of turbulent flow through a circular tube fitted with full length helical screw inserts (twist) of various twist ratio, and regularly spaced helical screw inserts with different spacer length. Technical details of helical screw-tape insert The geometrical configuration of helical screw-tape inserts is shown in Fig. 1a. The helical screw-tape inserts with various twist ratio is made by winding uniformly a strip of 5 mm width over a 8 mm rod. These sheets wounded with pitch values 20, 30, 40 mm. Due to these specifications we get helical screw tapes of two different materials. Fig 1a : Copper Insert with Pitch 20 mm Fig 1b:Copper Insert with Pitch 30 mm water. Similarly a rotameters is provided to control the flow rate of hot water from the inlet hot water tank. Cold water flow rate is kept constant at 60,120LPH. Two pressure tapings- One just before the test section and the other just after the test section are attached to the U-tube manometer for pressure drop measurement. Mercury (Hg) is used as the manometric fluid. Four thermocouples measure the inlet & outlet temperature of hot water & cold water (T1, T4,T7,T10,T11) through a multipoint digital temperature indicator. Procedure Fig 1c:Copper Insert with Pitch 40 mm Fig: 1 Helical Screw Tape Insert of copper Material Fig 2 a: Steel Insert with Pitch 20 mm Fig 2 b :Steel Insert with Pitch 30 mm Fig 2 c:Steel Insert with Pitch 40 mm Fig:2 Helical Screw Tape Insert of Steel Material Connect the plug pins to 220 V A.C stable electric supply. Switch on the heater power supply. Heater is put on to heat the water to 60 to 650C in a constant temperature water tank of capacity 60litres. The tank is provided with a centrifugal pump & a bypass valve for recirculation of hot water to the tank & to the experimental setup. Start the pump and water at about 55°C is allowed to pass through the tube side of heat exchanger at desired flow rate. Cold water is now allowed to pass through the annulus side of heat exchanger in counter flow direction at a 60,120LPH (mc=0.01657,0.033146 Kg/sec). The water inlet and outlet for both hot water & cold water temperatures are recorded only after temperature of both the fluids attains a constant value. The procedure was repeated for different Hot water flow rates ranging from 60 to 300 LPH. The manometer reading is noted for each observation. Calculations Experimental set-up and procedure The following photographs shows the experimental A) Calculation for Reynolds Number set up. Reynolds Number (Re) = × v × di B) Calculation For Heat Transfer Coefficient And Nusselt Number Heat transfer coefficient hInner = Nusselt Number (Nu) = Fig 3: Experimental Set Up Photographs show the experimental setup. It is a double pipe heat exchanger consisting of test section, rotameters and water tank for supplying hot water with in-built two heaters, pump & the measuring system. The test section is a Plain copper tube with dimensions of 1000mm length, Inner tube-22 mm ID, and 25 mm OD; Outer MS pipe- 44mm ID, and 47 mm OD. The outer pipe is well insulated using 100 mm diameter glass wool to reduce heat losses to the atmosphere. Two calibrated rotameters, with the flow range 30 to 300 LPH, are used to measure the flow of cold & hot water. The water, at room temperature is drawn from tap of cold q A * LMTD h × di k C) Pressure Drop and Friction Factor Calculation 1) Friction factor f = Where Δp in N/m2 p × di × 2 L × × v2 =h in mm of hg × 133.33 Results and discussion Results were discussed on the basis of heat transfer performance different types Material used for screw tape.The experimental system was validated by performing experiments using pure water. The following results were obtained for different Materials i.e. copper And M.S. shown as graphically. Plain tube Results Fig 5b: Variation of Friction factor Vs Reynolds Number Above graph indicates variation of Friction factor Vs Reynolds Number for cold water flow rate which is constant at 60,120LPH for Copper screw tape with 20 mm pitch. Fig 4a: Variation of Nusselt Number Vs Reynolds Number. Above graph indicates variation of Nusselt Number Vs Reynolds Number for cold water flow rate which is constant at 60,120LPH for plain tube. Fig4b : Variation of Friction factor Vs Reynolds Number. Above graph indicates variation of Friction factor Vs Reynolds Number for cold water flow rate which is constant at 60,120 LPH for plain tube. Material: Steel Fig 6a: Variation of Nusselt Number Vs Reynolds Number Above graph indicates variation of Nusselt Number Vs Reynolds Number for cold water flow rate which is constant at 60,120 LPH for Steel Screw tape with 20mm pitch. Helical Screw Tape Results Material: Copper Fig6b : Variation of Friction factor Vs Reynolds Number. Above graph indicates variation of Friction factor Vs Reynolds Number for cold water flow rate which is constant at 60, 120 LPH for Steel screw tape with 20 mm pitch. Fig5a: Variation of Nusselt Number Vs Reynolds Number. Above graph indicates variation of Nusselt Number Vs Reynolds Number for cold water flow rate which is constant at 60,120LPH for Copper screw tape with 20mm pitch. As like this there are different readings have been taken and on those results we comparing that for different material having different pitch value i.e. 30 mm and 40 mm Following graph show the variation for different Pitch value and material. Effect of Pitch Value Fig7a: Variation of Nusselt Number Vs Reynolds Number. Above graph indicates variation of Nusselt Number Vs Reynolds Number for cold water flow rate which is constant at 60LPH, for Copper Screw Tape with pitch values 20,30 and 40 mm respectively. Above graph clearly indicates that as pitch Value increases the Nusselt No. Decreases for different Reynolds no. It shows maximum Nusselt no for 20 mm pitch is 26.44. Fig7b: Variation of Pressure Drop Vs Reynolds Number. Above graph indicates variation of Pressure Drop Vs Reynolds Number for cold water flow rate which is constant at 60LPH, for Copper screw tape with pitch values 20, 30, 40 mm respectively. Above graph clearly indicates that as pitch Value increases the Pressure drop increases for different Reynolds no. Effect of Material Fig8a: Variation of Nusselt Number Vs Reynolds Number Above graph indicates variation of Nusselt Number Vs Reynolds Number for cold water flow rate which is constant at 120 LPH, for Copper, and Steel screw tape with pitch value 20 mm Above graph clearly indicates that for Copper material Nusselt no is maximum for most of the Reynolds no. So that Copper inserts are more effective than the Steel inserts Fig8b: Variation of Pressure Drop Vs Reynolds Number. Above graph indicates variation of Pressure Drop Vs Reynolds Number for cold water flow rate which is constant at 120LPH, for Copper and Steel screw tape with pitch values 15 mm. Fig8c: Variation of Friction factor Vs Reynolds Number. Fig 7c:Variation of Friction factor Vs Reynolds Number. Above graph indicates variation of Friction factor Vs Reynolds Number for cold water flow rate which is constant at 60LPH for Copper screw tape with pitch values 20, 30, 40 mm respectively. Above graph clearly indicates that as pitch Value increases the Friction factor also decreases for different Reynolds no. Above graph indicates variation of Friction factor Vs Reynolds Number for cold water flow rate which is constant at 120LPH for Copper and Steel Screw tape with pitch values 20mm. Conclusions It can be found that enhancing heat transfer with passive method using different types of Screw tape construction in the inner tube of a double pipe heat exchanger can improve the heat transfer rate efficiently. However, the friction factor of the tube with the Screw tape insert also increases. The increase in heat transfer and friction can be explained by the swirling flow as a result of the secondary flows of the fluid. Following are the conclusions drawn from this research, the effect of varying hot fluid flow rate (or Reynolds Number) on the , Nusselt number & friction factor, and comparative study for above said parameters different flow regimes (i.e. 60LPH to 300LPH), the effect of varying fluid flow rate. Similarly the comparative study among material, pitch values for heat exchanger. i) It is found that pressure drop increases as Reynolds number increases for all screw tapes (i.e. by considering all variation of the pitch) & friction factor decreases with increase Reynolds number for all twisted tapes. ii) Nusselt number increases as Reynolds number increases for all tapes. iii) From result tables and calculation it is also found that Nusselt number for Copper Screw tape with pitch 20mm 40% increase as compared to plain tube heat exchanger and Steel with pitch 20 mm is 25-32% increase more as compared to plain tube heat exchanger. iv) Experimental analysis shows, for Copper 20 mm pitch value Nusselt number is more than remaining Five Screw tapes. v) Result shows that pitch value increases the Nusselt number decreases; so that minimum pitch value (20 mm) has maximum Nusselt number but pressure drop is maximum for minimum pith value (20 mm). 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