This disclosure relates to an aircraft jet engine mounted fuel centrifugal boost pump, for example, in particular to the centrifugal boost pump volute.
The centrifugal boost pump is commonly packaged together with the main fuel pump, which is usually of a positive displacement gear pump type, both being driven by a common shaft. The fuel leaving the boost stage goes through a filter and a fuel oil heat exchanger before entering the main pump. Pressure losses are introduced by these components and the associated plumbing, while heat is also added to the fuel. The fuel feeding the centrifugal boost pump comes from the main frame fuel tanks through the main frame plumbing. The tanks are usually vented to the ambient atmospheric pressure, or, in some cases, are pressurized a couple of psi above that. The tanks are provided with immersed pumping devices, which are in some cases axial flow pumps driven by electric motors or turbines, or in other cases ejector pumps, collectively referred to as main frame boost pumps.
During flight, the pressure in the tank decreases with altitude following the natural depression in the ambient atmospheric pressure. Under normal operating conditions, industry standards require the main frame boost pumps to provide uninterrupted flow to the engine mounted boost pumps at a minimum of 5 psi above the true vapor pressure of the fuel and with no V/L (vapor liquid ratio) or no vapor present as a secondary phase. Under abnormal operation, which amounts to inoperable main frame boost pumps, the pressure at the inlet of the boost stage pumps can be only 2, or 3 psi above the fuel true vapor pressure, while vapor can be present up to a V/L ratio of 0.45, or more. Definition of terms, recommended testing practices, and fuel physical characteristics are outlined in industry specifications and standards like Coordinating Research Council Report 635, AIR 1326, SAE ARP 492, SAE ARP 4024, ASTM D 2779, and ASTM D 3827, for example.
During normal or abnormal operation, the centrifugal boost pump is required to maintain enough pressure at the main pump inlet under all the operating conditions encountered in a full flight mission such as the main pump can maintain the demanded output flow and pressure to the fuel control and metering unit for continuous and uninterrupted engine operation. There are also limitations in the maximum pressure rise the engine mounted centrifugal boost pump is allowed to deliver such not to exceed the mechanical pressure rating of the fuel oil heat exchanger, or limitations pertaining to minimum impeller blade spacing such as a large contaminant like a bolt lost from maintenance interventions would pass through and be trapped safely in the downstream filter. All these requirements along with satisfying a full flow operating range from large flows during takeoff to a trickle of flow during flight idle descent, and fuel temperature swings from −40 F to 300 F, makes the aerodynamic design of the engine mounted fuel pumps a serious challenge.
The volute collects the flow which is leaving the impeller in an almost tangential direction and with high velocities close to that of the impeller tip tangential velocity and directs it to the pump discharge port. From the pump inlet to the impeller exit port, the only element which adds power to the fluid is the impeller. The power is supplied at the shaft by the pump driver. A successful pump is expected to deliver the flow at the pump discharge port with relatively low velocities, at the required pressure rise above pump inlet pressure and with the best efficiency possible.
In general, impellers by themselves present high efficiencies between 75% and 95% depending on the pump size in terms of flow and running speed. The flow stream leaving the impeller exit port, aside from containing potential energy in the form of static pressure, also contains a fair amount of kinetic energy due to the high velocity of the fluid stream. Hence, in order to achieve a high overall efficiency for the entire pump, the volute must provide a high degree of pressure recovery, or transfer as much kinetic energy as possible into potential energy, or static pressure. To achieve this goal, the volute cross section is progressively increased in the direction of flow, which forces the fluid stream to slow down and, in the process, energy is recovered in the form of pressure.
The volute is composed of three distinct sections. The first section, which wraps around the impeller exit port, is called the volute proper. The second section, which usually is a straight tapered segment with a roundish cross section, is called a diffuser. The last section, which turns the flow from a normal plane relative to the impeller axis to an axial direction, is called exit bend. The need for the exit bend is dictated by the specific requirements of a given application.
A disclosed boost pump volute includes normal to flow cross sectional surfaces distributed over the length of the passage. The volute includes a volute proper, an exit bend and a diffuser fluidly interconnecting the volute proper to the exit bend. The cross sectional surfaces are defined as dimensions set out in one set of data, which includes Tables N-1 and N-2 for the volute proper and Table N-3 for the volute exit bend, where N is the same value.
The disclosure can be further understood by reference to the following detailed description when considered in connection with the accompanying drawings wherein:
A schematic of an example of engine mounted fuel delivery system, for example, for an aircraft, is illustrated in
The shaft 23 is splined to a drive gear 34, which is couple to and rotationally drives a driven gear 36. A drive gear floating bearing 38 and a drive gear fixed bearing 40 support the drive gear 34. A driven gear floating bearing 42 and a driven gear fixed bearing 44 support the driven gear 36.
During operation, fuel flow enters through the inlet from the far right side opening 45 of the boost pump housing cover 26 flowing axially from left to right. The fuel flow then enters first the inducer section 53 of the rotating impeller 24 where the pressure is raised and the eventual air and vapor phase present in the mixture are compressed back in to solution such by the time the fuel flow reaches the impeller section 51 most of the mixture is in the liquid phase. The fuel flow then enters the impeller section 51 where the majority of the pressure rise takes place, while the fluid absolute velocity is greatly increased. The fuel flow leaves the impeller 24 at its outside diameter exit port, or perimeter 62, under significantly larger pressure and with large velocity in an almost tangential direction. At this location, the flow stream contains potential energy based on the actual static pressure and a good amount of kinetic energy due to the high flow velocity.
It is the purpose of the volute to gradually capture this flow stream, progressively slow its velocity down and guide it towards the boost pump discharge port. By slowing down the flow stream velocity in a smooth way and without generating of any eddies, the majority of the kinetic energy of the flow stream is transformed into potential energy, or pressure. At the exit port of the boost pump, flow is delivered to the downstream system at much higher pressure than that from the boost pump inlet and with a relatively low velocity commonly used in the fuel system plumbing to deliver the fuel flow throughout the system.
The volute 54 is defined by inner and outer arcuate walls 72, 74 that are radially spaced from one another. The radius “r base” from the axis Z defines the inner arcuate wall 72 and is provided as a ratio to an impeller outer diameter D2 throughout this disclosure (see
First and second axial spaced walls 76, 78 adjoin the inner and outer arcuate walls 72, 74 to provide a generally quadrangular cross-section. One or more of the corners of this quadrangular cross-section may include a radius, which in one example is 0.032 in (0.81 mm). In a first portion of the volute proper 56, represented by section A-A in
In a second portion of the volute proper 56, represented by section B-B in
The volute exit bend 60 is illustrated by the section C-C in
In a second portion of the volute proper 156, represented by section B-B in
The volute exit bend 160 is illustrated by the section C-C in
In a second portion of the volute proper 256, represented by section B-B in
The volute exit bend 260 is illustrated by the section C-C in
Tables N-1, N-2 and N-3 defining the volute and exit bend geometry provide the values for the critical dimensions in accordance with
Although an example embodiment has been disclosed, a worker of ordinary skill in this art would recognize that certain modifications would come within the scope of the claims. For that reason, the following claims should be studied to determine their true scope and content.