Steam as a coolant is a possible option to cool blades in high temperature gas turbines; however there is practically no experimental data. This work deals with an attempt to generate such data and with the design of an experimental setup used for the purpose. Initially, in order to guide the direction of experiments, a preliminary theoretical and empirical prediction of the expected experimental data is performed and is presented here. This initial analysis also compares the coolant properties of steam and air

Engeda, A.

Lloyd, J.R.

Wilmsen, B.

Wilmsen, Bernd

Engeda, Abraham

Lloyd, John R.

UNT Digital Library

DOEMCl2906 1-96lCO672 Steam as Turbine Blade Coolant: Experimental Data Generation Author: Bernd Wilmsen Abraham Engeda John R. Lloyd L L L A J C  d L  Contractor: 0 9 i>3b s- $ v-* I [ + - 9 t - i 2  " F 2 4  #an- South Carolina Energy Research and Development Center Clemson University Clemson, SC 29634 Contract Number: DE-FC21-92MC29061 Subcontract No. 94-01-SR026 Subcontract No. 95-0 1 -SR040 Conference Title: Advanced Turbine Systems Annual Program Review Conference Location: Morgantown, West Virginia Conference Dates: October 17-19, 1995 Conference SDonsor: U.S. Department of Energy, Office of Power Systems Technology, Morgantown Energy Technology Center Contractinp Officer Representative (COR): Norman Holcombe DISTRIBUTION OF THIS DOCUMENT IS U N U M W  li_s B 1 Disclaimer This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or use- fulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof. This report has been reproduced directly from the best available COPY. Available to DOE and DOE contractors from the Office of Scientific and Technical Information, 175 Oak Ridge Turnpike, Oak Ridge, TN 37831; prices available at (615) 576-8401. Available to the public from the National Technical Information Service, U.S. Department of Commerce, 5285 Port Royal Road, Springfield, VA 22161; phone orders accepted at (703) 487-4650. 2 P19 Steam as Turbine Blade Coolant: Experimental Data Generation Bernd Wilmsen (e-mail: wilmsenb@egr.msu.edu; pho.: 517-432 1102) Abraham Engeda (e-mail: engeda@me.msu.edu; pho.: 51 7-432 1834) John R. Lloyd (e-mail: lloyd@me.msu.edu; pho.: 517-355 9717) A23 1 Engineering Building Mechanical Engineering Department Michigan State University East Lansing, MI 48823 Abstract Steam as a coolant is a possible option to cool blades in high temperature gas turbines. However, to quantify steam as a coolant, there exists practically no experimental data. This work deals with an attempt to generate such data and with the design of an experimental setup used for the purpose. Initially, in order to guide the direction of experiments, a preliminary theoretical and empirical prediction of the expected experimental data is performed and is presented here. This initial analysis also compares the coolant properties of steam and air. Nomenclature 2 1, m, n, o Di h k L Nu Pr Re Tf P P Tb V Avg. specific heat at const. press. Condition dependent constants Inside tube diameter Avg. convective heat trans. coeff. Avg. conductivity of fluid in tube Length of tube Nusselt Number Prandtl Number Reynolds Number Avg. bulk temperature of fluid Avg. film temperature Avg. velocity of fluid Avg. density of fluid Avg. absolute fluid viscosity Research sponsored by the U.S. DOE’S METC, under Contract # 94-01-SRO26 & 95-01-SRO40 with Michigan State University Introduction Maximizing power output from gas turbines requires engine operation at the highest possible temperature. However, the material limitations of the first turbine stages limit operating temperature: either strength deteriorates markedly at elevated temperatures or the material approaches its melting temperature. To allow for higher operating temperatures in gas turbines, under current know-how, blade cooling is the obvious solution. Several methods, with differing merits, have been developed over the years to keep turbine blade temperatures below critical levels. In all cases, the main objective in turbine blade cooling has been to achieve maximum heat transfer coefficients while minimizing the coolant flow rate. Even though steam as a thermodynamic working fluid is a common occurrence in the superheaters of steam power plants, general heat transfer data related to steam is not available. In particular there is a great lack of information on: The effect of steam flow passage geometry on ‘ the heat transfer and pressure drop, both for laminar and turbulent flows. Experimental data related to wall heat transfer and friction characteristics for fully developed turbulent steam flow. 3 Any work based on steam flow that studied, pumping work, and heat transfer coefficients, both with constant heat flux and constant surface temperature conditions. The experimental set up A compact stand alone steam unit with a controllable and measurable steam source has been developed as shown in figure 1 and 2. As opposed to a real cooling situation where the 'coolant-steam' is heated by the turbine flow air, the heat transfer in this work is in the reverse direction where the air is heated by the steam. The steam unit consists of a Chromalox IOKW steam generator followed by a superheater. The steam leaves the superheater and enters the test section. The steam entering the test section will have enough superheat to remain superheated as it leaves the test section for each test condition. Finally the steam is condensed and rejected. The controllable superheater adds heat the steam. The associated instrumentation will measure the electrical input and steam mass flow in addition to all thermal properties of the steam, both in the radial and axial direction. The conduit inside wall temperature will also be measured. The air loop is driven by a 15 KW FUGI Blower. The air loop is an open loop with flow control and flow measurements at the suction side. The pressure side is connected to the test section where the air exchanges heat with the Steam. A blade being cooled acts basically as a heat exchanger. The design and analysis of any heat exchanger requires a knowledge of the heat transfer coefficient between the wall of the conduit and the fluid flowing inside it. The sizes of the heat exchanger depend largely on the heat transfer coefficient between the inner surface of the tubes and the fluid. Once the heat transfer coefficient for a given geometry and specified flow condition is known, the rate of heat transfer at the prevailing temperature difference can be calculated. Also to determine the area required to transfer heat at a specified rate for a given temperature difference potential, the fluid temperature, which varies along the conduit and at any cross section, must be defined with care and precision. Thermodynamic Design of the Steam Unit The thermodynamic design of the steam and air flow cycles was carried out on an EXCEL spread sheet, which allowed instant component sizing and overall optimization. The design sheet used is summarized in Table I. Major measured quantities temperatures - TU, free stream air temperature - Tw, air side wall temperature - Tst, i-0, temperature of steam in and out pressures - ps~rf., st. pressure distrib. of test surface - pst, i-0, steam pressure, in and out free stream air velocity, uu turbulence intensity before test section steam and air flow rates Major derived quantities ha, heat transfer coeff. of air, local and avg. hst, heat tran. coeff. of steam, local and avg. turbulence intensity of the air Rea, the Reynolds number of air Rest, the Reynolds number of steam temperature ratio Ma, the air Mach number q, heat flux from steam Ahst, enthalpy fall of steam 4 Expected Results First a simple tube geometry and next a simplified blade, both shown in figure 3 will be experimentally investigated. Based on the works of Dittus-Boelter, Sieder-Tate, Kays-London, Petukhov-Popov, and Sleicher-Rouse extensive data and correlation for turbulent gas and liquid flow through tubes and ducts have been presented through the years. The correlation for the heat transfer, resulting from these works, takes the general form: The number of parameters have been shown to be reduced by introducing the following dimensionless numbers: 0 0 0 Reynolds number (Re): PvDi P Re=- Prandtl number (Pr): cPP Pr = -Nusselt number (Nu): k h Di k NU=- Equation 1 can then be expressed as Nu = C[Re]’[Pr]m[:J[Fr (3) (4) Colburn /1/ showed that the influence of the pipe length on the Nusselt number is negligible if the Reynolds number is larger than 5x103. The Reynolds number in the present test section are expected to be higher than 1x104 in all test cases. The temperature difference between the pipe surface and pipe center may lead to variable fluid properties. This influence will be accounted for by the relationship between bulk dynamic viscosity and wall dynamic viscosity. Properties of steam The Reynolds and Prandtl numbers are calculated with averaged properties. In figure 4, the Prandtl number for various pressures is shown. The properties for steam are calculated using the 1967 IFC relationships for industrial use. Figure 5 shows, that for a given mass flow, steam can transport nearly twice the energy that air can. The density of steam is lower than the density of air, but despite that, steam can transport more energy per unit volume than air as can be seen in figure 6. Calculation of Heat transfer The Nusselt number has been calculated with equation (5) using the following constant values: 0.027 0.8 1/3 0.14 These constant values were suggested by Colburn /1/ and Sieder and Tate 121 for flow conditions similar to the present planned test. The Nusselt number and the heat transfer coefficient have been calculated based on: Pipe inner Diameter: Test section length: 12.7 cm Inlet pressure: 5 bar Mass flow: 0.0035 kg/s Inner wall temperature: [ 1/21 inch 900 K for heating 300 K for cooling For cooled steam, the Nusselt number is larger than for heated steam because of the smaller boundary layer. This is a result of the lower dynamic viscosity at lower temperatures. The same effect is visible for air. In figure.7, it is 5 shown that the Nusselt number for steam is larger than for air at the same mass flow and the same thermodynamic conditions. The heat transfer in figure 8 shows the same trend. Reynolds Number In figure 9, it can be seen that the Reynolds number for steam flow is larger than for air flow. This means, the loss coefficient is lower in steam flow than in air flow. The influence of the mass flow on the heat transfer coefficient can be seen in figure 10. The heat transfer coefficient increases nearly linearly with the mass flow. The slope of the curve for steam is much higher than air. Conclusions A preliminary simple theoretical evaluation has been performed, to test the coolant potential of steam and to seek justification for the planned experiments. The results confirm that the experimental data are essential and will be applicable and useful for actual blade cooling design. References [l] Colbum, A.P.. Engg. Bull. Purdue University, Vol. 26, No. 1 (Engineering Experiment Station, Res. Series No. 84); January 1942 [2] Sieder, E.N., and Tate G.E., Ind. Engg. Chem. 28,1429; 1936 6 I lpart One: Steam Cycle Exit steam generator: hg [kJ/kg]: 2747.54 Enthalpy difference[kJ/kg]: 2579.94 Exit temDerature IK1: 425.00 est section: I I I ioe diameter Iml: 0.01 270 I Cross section Im21: I 0.00012668 Steam density [kg/mA3]: 1.407 Steam abs. viscosity [Pa SI: 2.86E-05 Avg. Velocity [m/s]: 19.572 Avg. Reynolds number: 12237.07 Part Two: Air Cycle I Table I : Thermodynamic design of the Steam Unit 7 f c 16 114' Figure 1: The Stand Alone Steam Unit connection Steam Gentr. 1 I n l  r'igure 2.: 'lhe Stand Alone steam Unit 8 3 Steam- y//, ’, ‘ t u  1 I I Air I I I I I I I I * I  I I 1 I - ---- J A  A-A I I  I /  A-A Figure 3 : Schematic representation of two blades to be investigated 9 Oa9 t n a# $ 1.5 -. E 1 -. 0.5 -- 0 Q 0 0.8 ! I t 1 I I I I I I I I I I I I I 273 373 473 573 673 773 873 Temperature [K] Saturation line 5 bar 10 bar 15 bar 20 bar 25 bar ----- -- - - - - - -  ------ ------- ~ ~ Figure 4 : Prandtl # vs. Temperature for steam 2 P------ 400 600 800 1000 Temperature [K] Steam ----- A i r  0 l o  600 800 1000 400 Temperature [K] Steam - - - - - - - -  Air  Figure 5 : Cp vs. Temperature ~~ Figure 6 : Cp p vs. Temperature 10 100 Air cooled ----- 80 6 0  4 0  *O 0 t.. 400 600 800 1000 Temperature [Kl Figure 7 : Nusselt ## vs. Temperature 25000 i I 20000 15000 5 u) a C >. Q) 10000 LT 5000 0 400  600 800 1000 Temperature [K] Steam ----- A i r  'igure 9 : Reynolds vs. Temperature ------- -I--- " I  I I I 400 600 800 1000 Temperature [K] Steam cooled cooled - - - - - A i r  Figure 8 : Heat transfer coefficient vs. Temperature 500 - 400 -. y" 0 4  E 300-. \ p 200- Y 100 -. 0 r 0 I I I 0 0.005 0.01 Massflow [kg/s] A i r  - - - - - Steam T=750 K T=750 K Figure 10 : Heat tra. coeff. vs Mass flow 1 1  

Steam as turbine blade coolant: Experimental data generation

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