Gas Turbine Jet Engine Objectives This lab experiment was aimed at doing a start-up and power-down of Gas Turbine and data logging and become familiar with engine and its controls. Introduction A pure turbojet, CM-14 represents a jet engine. In this engine combustion causes expansion of gas capable of producing useful work and thus cause jet propulsion. It consists of a centrifugal flow compressor, axial flow power turbine, and annular combustor. The CM-14 engine is a model of gas generator core common in turbofan, turboshaft and turboprop gas turbine engines that are commonly used in marine and aircraft propulsion as well as in industrial and stationary power generation. The following figure shows a model gas turbine. Figure 1: Gas turbine. This gas turbine is made up of 4 sections and which are: o Inlet part o Compression part o Combustion part o Turbine and exhaust part The turbine part is responsible for creating needed power output to run propeller. It also serves to generate power for driving all other parts of the turbine and compressor. For it to produce power, this gas turbine has to expand gas at high pressure, velocity and temperature and transforms gas energy to mechanical energy available at the power shaft. The compressor is used to provide a certain amount of air. It works by creating air to the engine and where it is squeezed to generate high-pressure air needed in the turbine. Compressor works using mechanical power from turbine that converts gaseous energy in form of temperature and pressure. Gas turbine encounters frictional losses which makes it hard for the compressor to provide all air required by turbine. As such, the turbine does not provide all the power required by compressor. Therefore, it means energy has to be added to the air so as to supplement the deficit. The combustion part is where energy is produced. This happens when fuel is burned and fuel chemical energy transformed into gaseous energy at high temperature and air velocity. The gaseous energy is then transformed into mechanical energy and used to drive output shaft and compressor. Basically, the gas turbine consists of 4 cycles which are air intake, air compression, combustion and expansion and exhaust. The figure below shows cycles of a closed gas turbine on a T-S diagram. Figure 1: Closed gas-turbine T-S diagram From the gas turbine cycles stages 1 and 2 illustrates air compression in the compressor. Some work is done here and it is given by π€12 = −( β2 − β1 ) = −πΆπ (π1 − π2 ) After being compressed the air goes from stage 2 to 3 where undergoes heat addition at constant pressure. Heat is added and it can be calculated by using the equation π€23 = ( β3 − β2 ) = πΆπ (π3 − π2 ) From stage 3 to 4 air from combustion is compressed in the turbine. The work done by turbine can be calculated by π€πππ‘ = πΆπ ( π3 − β4 ) − πΆπ (π2 − π1 ) Heat input for this cycle is given by πππ = πΆπ (π3 − π2 ) 1 As such, efficiency can be computed by Ι³ = 1 − (π ) Ι£−1 Ι£ Gas turbine performance is depended on shaft horse power the engine produces at certain conditions. Most of jet engines have power ratings at 29.92 inches of mercury and 59oF. The specific fuel consumption at a certain condition defines the engine efficiency. The efficiency is determined by amount of air mass flow rate via the engine, operating temperatures, compressor pressure ratio, and individual component efficiencies. SAFETY PRECAUTION Safety was maintained by following instructions given by the manufacturer and also using common sense when handling high temperature and pressure. In addition, a distance of 10m was maintained on both sides when starting the experiment. Apparatus ο· Electronic console ο· Engine module ο· User PC with Armfield Before startup Prior to starting the experiment fuel was prepared and filled in a container as recommended by Armfield. Fuel ratio was 22.5% meaning 225ml of Aeroshell (Turbine 500) in 1000 ml of kerosene. PROCEDURE The Electronic console master switch was turned on. Armfield software was loaded onto the user PC and view diagram screen was selected. This displayed mimic diagram of the engine with readings from sensors superimposed. The screen showed readings for the engine parameters that is thrust, shaft speed, temperatures and pressure. The diagram on the screen of PC look like the one shown below. Before engine was started and recorded results zero buttons were clicked on all the sensor edit fields given with this function. This helped to compensate with residual errors in sensors. Observation Table 1: S.N0 Throttle Position T1 T2 T3 T4 T5 P0 P1 P2 P3 P4 P5 T n l [%] 1 27.00 29 52 654 611 622 101.30 -1.84 41.02 31.01 33.20 7.34 24 47988 0.38 2 32.00 28 55 615 511 520 101.30 -1.17 23.93 17.58 18.55 3.67 9 37441 0.17 3 34.00 27 54 604 503 504 101.30 -1.25 24.66 18.31 19.04 3.79 12 38203 0.17 4 24.00 27 82 540 504 501 101.30 -5.12 89.60 70.80 70.56 15.55 48 67910 0.34 5 30.00 27 97 506 481 483 101.30 -6.80 107.42 93.26 93.51 21.45 64 75469 0.39 6 37.00 27 111 501 470 473 101.30 -8.20 128.66 113.53 111.82 25.55 70 80859 0.43 7 42.00 27 124 500 470 472 101.30 -9.84 152.34 131.35 129.15 28.59 91 85371 0.47 Corresponding Data Table 2 Air Mas s Flow Rate Cp 1 Cp 2 Cp 3 Cp 4 Cp 5 S1 S2 S3 S4 S5 H1 H2 H3 H4 H5 0.32 1.0 0 1.0 1 1.1 3 1.1 2 1.1 2 0.0 0 3.9 8 6.6 4 6.6 3 6.6 6 306.6 9 329.6 9 967.7 9 920.3 0 932.5 2 0.26 1.0 0 1.0 1 1.1 2 1.0 9 1.1 0 0.0 0 4.0 8 6.6 0 6.4 4 6.4 7 305.9 3 333.1 0 924.6 2 809.5 6 819.5 3 0.26 1.0 0 1.0 1 1.1 2 1.0 9 1.0 9 0.0 0 4.0 6 6.5 8 6.4 2 6.4 4 305.4 3 332.1 3 912.0 3 801.1 0 801.6 0 0.53 1.0 0 1.0 1 1.1 0 1.0 9 1.0 9 0.0 0 4.3 8 6.3 6 6.4 0 6.4 3 305.4 3 359.9 5 841.5 9 802.0 9 798.6 1 0.62 1.0 0 1.0 1 1.0 9 1.0 9 1.0 9 0.0 0 4.5 2 6.2 5 6.3 3 6.3 9 305.1 8 375.3 3 803.3 7 776.8 0 779.2 7 0.68 1.0 0 1.0 1 1.0 9 1.0 8 1.0 9 0.0 0 4.6 4 6.2 2 6.3 0 6.3 7 304.9 3 390.0 2 798.8 9 764.9 4 767.9 0 0.74 1.0 0 1.0 1 1.0 9 1.0 8 1.0 9 0.0 0 4.7 2 6.1 9 6.2 9 6.3 7 304.6 8 402.3 5 797.7 7 764.9 4 766.9 1 [kg/ s] Nomenclature T1 Inlet Temperature [°C] Cp1 Specific Heat at inlet [KJ/Kg K] T2 Compressor Temperature [°C] Cp2 Specific Heat in compressor [KJ/Kg K] T3 Combustor Temperature [°C] Cp3 Specific Heat at combustor [KJ/Kg K] T4 Turbine Temperature [°C] Cp4 Specific Heat at Turbine [KJ/Kg K] T5 Exhaust Temperature [°C] Cp5 Specific Heat at Exhaust [KJ/Kg K] P0 Ambient Pressure [kPa] S1 Entropy at inlet [KJ/Kg K] P1 Inlet Pressure [kPa] S1 Entropy in compressor [KJ/Kg K] P2 Compressor Pressure [kPa] S1 Entropy at combustor [KJ/Kg K] P3 Combustor Pressure [kPa] S1 Entropy at Turbine [KJ/Kg K] P4 Exhaust Pressure [kPa] S1 Entropy at Exhaust [KJ/Kg K] P5 Inlet Pressure [kPa] H1 Enthalpy at inlet [KJ/Kg K] T Thrust [N] H2 Enthalpy in compressor [KJ/Kg K] n H3 Enthalpy at combustor [KJ/Kg K] Speed [RPM] l Fuel Flow [l/min] Air mass flow rate [Kg/ sec] H4 Enthalpy at Turbine [KJ/Kg K] H5 Enthalpy at Exhaust [KJ/Kg K] Discussion From data obtained it was seen that when percentage position of throttle increased pressure and temperature in the compressor, turbine and combustor increased. This happened because increasing throttle position percentage led to more fuel and air entering the gas turbine thus combustion increased and then there was higher temperature and pressure. Likewise, propeller speed increased with increase of throttle position. More air flow results in increased combustion and then more air-fuel mixture is converted to heat energy meaning more power is produced and thus higher speed. This was so because more energy is produced when air-fuel mixture is burnt and converted to mechanical power. As such, output shaft of the turbine and propeller rotate are very high speed. It can also be seen that increasing flow rate of air in the turbine leads to increased entropy. However, the enthalpy decreases gradually in the turbine, combustor, and exhaust as the air flow rate is increased. Conversely, compressor enthalpy increased when air flow rate increased. CONCLUSION From this lab experiment the gas turbine jet engine start-up, power down processes and data logging were performed. In addition, its enhanced familiarity with gas turbine parts and working principle and its control. Certain gas turbine parameters such as percentage throttle position and air mass flow rate on the engine performance were analyzed. From this experiment it was learnt that increasing the air-fuel mixture results to increased combustion rate and thus more heat energy which is converted to mechanical energy that is used to drive turbine shaft and propeller and enhance jet propulsion. References 1. Moran, M.J., Shapiro, H.N., Boelter, D. D., & Bailey, M. B. (2010). Fundamentals of engineering thermodynamics. John Wiley & sons. 2. Lab guideline manual. 3. Yunus A Cengel, Michael A. Boles. Thermodynamics an engineering approach. 5th edition.