- •Chapter 14. Gas turbine engine starting systems
- •14.1. General information
- •14.1.1. Starting system designation
- •14.1.2. Requirements to the starting system
- •14.2. Structure of gas turbine engine starting systems
- •14.3. Gas turbine engine starting diagram. Characteristic of start stages
- •Table 14.1 Typical rotational speeds of gte rotor
- •14.4. Calculation of gas turbine engine starting system
- •14.4.1. Determination of necessary maximum power of the starter
- •14.4.2. Starting diagram calculation
- •Fig. 14.5. Starter power dependence versus rotor rotational speed, for constant torque
- •Using equation (14.1), we will get
- •From equation (14.1) and in view of formula (14.6) we will get:
- •For the tpEs a rotor dynamical moment of inertia equals:
- •Fig. 14.8. Diagram of the redundant torque
- •14.5. Types of aeroengine starters
- •14.5.1. Electrical starters
- •14.5.2. Turbine starters
- •Fig. 14.17. Schematic of an air turbine starter
- •Fig.14.19. Schematic of the gas turbine starters:
- •Fig. 14.21. Cartridge-pneumatic starter scheme
- •14.5.3. Hydraulic starters
- •Questions for self-check
14.4. Calculation of gas turbine engine starting system
The purpose of the calculation is to determine the necessary maximum power of the starter, to build starting diagram and to determine starting duration.
14.4.1. Determination of necessary maximum power of the starter
This problem can be solved accurately provided the theory of power machines is applied.
Fig. 14.4. Gas temperature in turbine inlet versus rotor rotational speed at starting:
1 – maximum permissible temperature under conditions of rotor details strength; 2 – maximum permissible temperature under conditions of compressor gas-dynamic stability; 3 – optimal law of gas temperature change at starting; 4 – gas temperature at steady-state starting ratings
In previous calculations necessary maximum power NSDmax of the starting device was determined using statistic data of the made constructions of starter. On the basis of these data specific power values of the starter are determined:
- for TJEs and TFEs
;
- for TPEs, ТPFEs, ТShEs and APUs
,
where Рmax [kN], Nmax [MW] are an engine thrust and power at maximum rating.
Specific power values of starters for different types of GTEs can be follows:
- for TJEs and TFEs with thrust less than 10 кN
= 1,5...2,0 кW/кN;
- for TJEs and TFEs with thrust more than 10 кN
= 0,85...1,20 кW/кN;
- for one-shaft TPEs with power less than 1000 кW
= 30...50 кW/МW;
- for one-shaft TPEs with power more than 1000 кW
= 20...30 кW/МW;
- for free turbine GTEs with power less than 1000 кW
= 20...40 кW/МW;
- for free turbine GTEs with power more than 1000 кW
= 10...20 кW/МW;
- for APUs
= 80...100 кW/МW.
Required starter power maximum values for the given types of the GTEs are calculated by the formulas:
NSD max = Рmax;
NSD max = Nmax .
The GTE starter maximum power, which is closest to objective value can be determined using specific power value of engine-prototype starter.
14.4.2. Starting diagram calculation
Starting diagram calculation lies in МSD(n), МR(n) and МТ(n) functions determination.
An equation of power and torque applied to an engine rotor is used at determination of the starter torque
, (14.1)
where is the engine rotor angular speed of rotation.
The NSD(n) function depends on the type of the starter used. For gas turbine starters with a hydraulic clutch or differential reduction gear, as well as for electric starters with a special voltage regulator, it is possible to take МSDМ0=const (Fig. 14.5).
Fig. 14.5. Starter power dependence versus rotor rotational speed, for constant torque
From an equation (14.1) for starter turn off rotational speed n2 we will get the formula of М0 constant calculation
The MSD linear lowering is typical of air-turbine starters and gas turbine starters with the free turbine at rotational speed magnification (Fig. 14.6)
МSD(n) = М0 – bn,
where М0, b are the constants, which have to be determined for the solution of the problem.
Using equation (14.1), we will get
(14.2)
From the formula (14.2) follows that NSD = 0 at n = 0 and М0– bn = 0.
For function (14.2) maximum determination we will equate to zero its maiden derivative:
At NSD = NSD max.
Fig. 14.6. Starter power dependence versus rotor rotational speed, for torque MSD linear reduction
From an equation М0–2bnМ=0 we determine rotational speed nМ, which corresponds to the maximum of starter power:
(14.3)
Substituting values nМ in accepted linear dependence for МSD, we will get:
From equation (14.1) for МSD = М0/2 and n = nМ we will get
(14.4)
From equation (14.4) the initial torque М0 of the starter is determined as:
(14.5)
Constant “b” for a linear function МSD (n) can be got, when equation (14.5) is substituted in the formula (14.3):
For air turbine starters b=0,005…0,015 and for electric starters b=0,04…0,07.
The value nM is determined with the help of the statistic data through the rotational speed n2:
where k is a statistical factor.
For gas turbine starters, which have a free turbine k=1,5...1,6; for air-turbine starters k=1,8...2,0.
The MR engine rotor antitorque moment determination is solved according to the requirement of powers balance on the rotor at idling. The compressor creates main antitorque moment at starting. A part of power (not more than 5...7 %) is expended on the drive of engine units and overcoming of the friction forces in rotor support bearings. Thus, we can write down
MR(n) = (1,05...1,07) МCR,
where МCR is an antitorque moment of the compressor rotor, for which quadratic relation can be obtained
МCR = C n2, (14.6)
where C is a constant.
The power, which is spent on rotation of the compressor rotor at idling, is determined by known thermodynamics ratio
(14.7)
where LAD C is an adiabatic work of the compressor at an idle; Ga is an air mass flow rate at the same rating; c is an efficiency of the compressor at idling.