Patent Description:
Aviation accounts for approximately <NUM>-<NUM>% of total carbon dioxide emissions. Aviation is expected to grow by <NUM>-<NUM>% per annum in next decade. In addition to carbon dioxide, aviation also contributes to climate change through creation of contrails and exhaust of NOX and water vapor in higher atmospheric levels. The net-zero challenge is twofold: both carbon and non-carbon emissions must be reduced to zero.

Current air traffic patterns clearly indicate which type of aircraft and which stage lengths contribute most to CO2 and related non-CO2 emissions. From ICCT estimates of CO2 emissions from commercial aviation in <NUM>, <NUM>, and <NUM>, it can be estimated that approximately <NUM>% of all civil aviation CO2 emissions stem from flights shorter than <NUM>, <NUM>% from flights up to <NUM> and <NUM>% from flights up to <NUM>.

Many publications in recent years have underlined the perceived limitations for battery-electric aircraft.

<NPL> conclude that, for aircraft, the limited power-to-weight ratio of electrical components impedes the development of all-electric propulsion. The authors argue that instead of using all-electric propulsion, it is more beneficial to use an electrical system as a secondary system that would be running in parallel and would assist the existing primary propulsion system in certain flight phases to increase the overall efficiency.

<NPL> conclude that all electric designs are not feasible at any scale (from thin haul to long haul) because the required battery mass is larger than the airframe parameters can support. This paper argues that even with optimistic estimates of battery capacities available in <NUM>, batteries alone are unlikely to power aircraft at current design missions for thin haul, regional medium haul and long haul aircraft.

<NPL>, Number <NUM>, conclude that electric propulsion is not a promising path to significant reduction of aviation's CO2 in the first half of the 21st century. Supporting this conclusion, the authors state that ninety-two percent of aviation's CO2 is produced by single- and twin-aisle aircraft requiring <NUM>,<NUM> to <NUM>,<NUM> kW of shaft power and <NUM>,<NUM> to <NUM>,<NUM>,<NUM> kWh of energy at takeoff and that no known battery technology is capable of powering such aircraft at the ranges now flown.

<NPL>, predict that electric aircraft with <NUM>-<NUM>% battery weight will only be feasible for regional or short haul flights when battery specific energies increase to much greater values than are currently available.

<NPL> consider that a purely battery powered aircraft is suitable for only short-range applications and therefore out of scope for FlyZero. In supporting this conclusion, the authors consider that typical empty operating mass is <NUM>% and fuel mass fractions are <NUM>% and that a battery powered aircraft with this energy fraction could manage only a very short range of less than <NUM> nautical miles (nm). The authors also concluded that the range for battery powered aircraft would only increase to <NUM> at the cost of decreasing the payload mass fraction to zero (thereby ruling out the use of the aircraft to carry any passengers).

<NPL>, conclude that purely battery-powered aircraft will play a very small role in lowering the climate impact of aviation. The authors support this conclusion by arguing that the expected design space for battery electric aircraft is one in which the empty operating mass and battery mass are around <NUM>% and <NUM>%, respectively, of the maximum take-off mass, yielding an effective range of only <NUM>.

At least two themes emerge from the existing literature. First, the range of existing electric aircraft and existing electric aircraft designs is too low to noticeably impact the emissions of the overall air transport sector. The well-known Breguet range equation shows that range is driven by the energy fraction (ratio of energy mass divided by maximum take-off mass). However, many authors claim that this energy fraction cannot exceed <NUM>-<NUM>% for rechargeable batteries, since current well-designed short range fossil fuel aircraft have similar fuel mass fractions. Second, a suitable rechargeable battery for such existing electric aircraft designs will not exist in the near future. Battery energy density is simply too low according to existing electric aircraft design principles.

Therefore, the common opinion in aerospace engineering literature is that battery electric aircraft will play a very small role in realizing net-zero because that the range obtainable using existing design principles for electric aircraft is too low for electric aircraft travel to significantly reduce global aviation emissions.

The integration of rechargeable batteries in electric aircraft is not well studied. Rechargeable batteries can be recharged in situ in the aircraft but they must be replaced after they have reached a maximum number of charging cycles. Designs must therefore allow access for periodic replacement of the rechargeable batteries. However, provision of access may come at the cost of compromising other design aspects.

It is well-known that aircraft are required by aviation authorities to contain fuel reserves, for example for diversion to an alternative airport and meeting the required loiter and contingency reserves. Though rarely used, such fuel reserves add extra mass to the aircraft which must be carried on every flight.

<NPL>, review all-electric conceptual, experimental, and commercial aircraft that have been researched in the past decades, with a particular focus on light aircraft, along with progress in battery technology. In addition, they develop all-electric aircraft designs starting from existing, conventionally-powered aircraft (Airbus A320neo). The theoretical performance of these all-electric aircraft is compared to advanced conventionally-powered aircraft optimized for the same, short design ranges.

The present disclosure seeks to address the disadvantages encountered in the prior art by providing an improved aircraft design.

According to an aspect of an invention, there is provided an aircraft according to the appended claims.

Specific embodiments are now described, by way of example only, with reference to the drawings, in which:.

In overview, and without limitation, the present disclosure relates to defining a design space for electric aircraft which goes against the conventional thinking and design trends in this field to produce an electric aircraft with a longer range than previously thought possible using rechargeable batteries. This application also relates to a wing for such electric aircraft, load carrying hatches for aircraft wings, and non-rechargeable reserve energy sources for rechargeable battery electric aircraft.

Some of the design principles in the present disclosure seek to maximize the useful battery mass fraction, and therefore range, by minimizing the empty operating mass fraction for a given payload mass requirement. This is achieved by exploiting the design principles, design choices and design features as described herein.

Conventional thinking suggests that electric aircraft designs will be limited to very short range aircraft which may not be suitable for the majority of commercial flight distances. While the range of battery-powered aircraft is indeed shorter than fuel-based aircraft, the design principles presented in this document will show that it is in fact higher than literature and conventional thinking in electric aircraft design suggests, and therefore it can play an important role in realizing net zero.

The solution to increase the range of rechargeable battery aircraft is to increase what the inventors coin the electric range factor 'ERF' - the product of the lift-to-drag ratio and the battery mass 'BM' as a fraction of the maximum take-off mass 'MTOM' - while operating in the CS25 design space (i.e. so that the aircraft have an MTOM of at least <NUM>).

The inventors have recognised that an increase in MTOM coupled with shifting the design space to allow an increase in the battery mass fraction relative to existing electric aircraft designs is a particularly effective means for increasing the electric range factor. The inventors have also devised several means by which the empty operating mass fraction can be reduced. This allows a yet further increase in the battery mass fraction, which in turn increases range. In addition, or alternatively, reducing the empty operating mass fraction allows an increase in the payload mass fraction, thus reducing energy consumption per passenger km.

The inventors have also devised design features which support these general concepts. For example, by associating the battery mass primarily with the wing (for example by placing the rechargeable batteries in, on or under the wing), the wing root bending moment can be reduced. This allows the empty operating mass 'EOM' fraction (EOM/MTOM) to be reduced yet further because the relative mass of the aircraft structure can be reduced due to the reduction in in-flight stress where the wing meets the fuselage. This is just one example of a design improvement that allows a greater payload mass 'PLM' fractions (PLM/MTOM) and/or even greater battery mass fractions (BM/MTOM).

Embodiments employing these design principles, choices and/or features include aircrafts with a relatively large wing area (and volume) and a relatively small fuselage area (and volume), compared to typical CS-<NUM> or short range CS-<NUM> aircraft. This automatically implies a higher lift-to-drag ratio than typical CS-<NUM> or CS-<NUM> aircraft, further enhancing range for a given battery mass fraction.

Other design features or principles described in this disclosure can (further) increase the lift-to-drag ratio of the aircraft and/or allow a reduction in the empty operating mass fraction, this allowing even greater battery mass and or payload mass fraction and further increasing the range of the electric aircraft. For example, increasing the number of propulsors compared with conventional aircraft so that there are more than four propulsors on the wing helps to increase the airflow over the wings, thus increasing lift. In another example, the airframe mass can be reduced by adopting a low-wing construction in which the wing is connected to the underside of the fuselage. In yet another example, the in-flight wingspan and/or the size (e.g. planform area or volume) relationship between the wings and fuselage can be adjusted to increase the lift-to-drag ratio. For particularly large wingspan designs, the wing can include foldable tips to accommodate airport requirements.

Another aspect is directed to secondary energy sources for electric aircraft having rechargeable batteries as a primary energy source. The secondary energy sources are of greater energy density but can be used far less often, if at all, in normal operation of the aircraft due to their intended use as reserves. The aircraft can thus take advantage of secondary energy sources suited to these requirements to make the most efficient use of the mass fraction set aside for energy sources in the aircraft while allowing the aircraft to remain rechargeable by virtue of the primary energy source.

Yet another aspect is directed to load-bearing hatches in a wing structure for access to rechargeable batteries therein. Though rechargeable batteries can be recharged in situ in the wing structure, their useful lifetimes may be only a fraction of the useful lifetime of the wing structure and hence replacement of the batteries is required from time to time. Replacement requires access into the wing structure through an opening. Such openings potentially weaken the wing structure or reduce its ability to carry loads applied to it, for example during flight. Rather than increasing the wing structure mass by reinforcing areas around the opening to transfer applied loads around it, the hatches are configured to carry the load instead. Thus, the wing structure mass does not need to increase to accommodate the openings for access to the rechargeable batteries.

The following abbreviations are used in this disclosure for conciseness:.

The following symbols and parameters are also used:.

The following definitions are useful for understanding the disclosure:
Breguet range: cruise flight range, as calculated based on the adapted Breguet range equation (see formula section).

Useful range: maximum serviceable air range; i.e. maximum distance that a given payload can be transported by the aircraft, from take-off until touchdown, in normal weather conditions without wind, while adhering to the necessary requirements in terms of reserves. This range can be calculated by taking the Breguet range and making several adjustments for a. take off, climb, etc., (see calculation assumptions).

Total range: useful range plus the effective range that the aircraft must be able to cover in the air for reserves. The "reserves" comprise three main components: contingency, diversion and loiter.

Lift-to-drag ratio: ratio between the lift force, defined as the component of the aerodynamic force generated on the airframe (excluding propulsors) that is perpendicular to the incoming flow direction, and the drag force, defined as the component that parallel to the incoming flow direction.

For an existing aircraft (i.e. in the real world), this parameter can be measured, whereas in the conceptual design process, it is estimated numerically. For the values and limits established in this disclosure:.

Additionally, zero-lift drag due to fuselage upsweep (following Ch. <NUM> of the Daniel Raymer textbook referenced herein) and heat exchangers of the thermal management system (assuming <NUM> N drag per kW of heat rejected) are included. Drag due to external stores, windmilling engines, and trans/supersonic parasite drag are not considered applicable and are therefore neglected.

Battery mass (BM): mass of the rechargeable battery pack used for propulsive and non-propulsive purposes, including the energy cells, battery management system, and elements which contribute to the structural integrity (e.g. a frame or other mechanical elements), thermal management (e.g. cooling plates or channels), exchangeability, or safety & reliability of the cells. In other words, the rechargeable battery pack consists of the components that are removed and replaced when the cells reach their end-of-life on the aircraft, plus any components that remain in the aircraft during the process of replacing the cells, but which functionally (i.e. structurally, thermally, etc.) contribute to the integrity and operability of the cells on board the aircraft.

Battery energy density: total end-of-life useful energy capacity of the cells in the rechargeable battery pack, divided by the battery mass as defined above.

For example, for cells which, when new, provide <NUM> Wh of energy per kg of cell at a discharge rate of 1C, with a <NUM>% mass overhead for packaging, a maximum depth-of-discharge of <NUM>%, and a chosen end-of-life capacity of <NUM>%, the battery energy density would be (<NUM> · <NUM> · <NUM>) Wh / (<NUM> + <NUM>) kg = <NUM> Wh/kg.

Electric range factor: non-dimensional parameter defined as the product of the lift-to-drag ratio and the battery mass fraction, where the latter is the ratio between the battery mass and the maximum take-off mass of the aircraft.

Range extender: a set of powertrain components which is used to increase the total range beyond what is achievable with the rechargeable batteries alone. For example, in the case of a fuel-based gas-turbine solution (a turbogenerator), the "range extender" would comprise the gas turbine and its accessories (oil system, intake, exhaust, etc.), the fuel, the fuel system, the electric generator, and cables and other additional elements of the electrical system required to deliver power to the rechargeable batteries or propulsors. In the case of a non-rechargeable battery, such as a metal-air battery or aluminium-air battery, the range extender would comprise the battery including the energy cells, battery management system, and elements which contribute to the structural integrity (e.g. a frame or other mechanical elements), thermal management (e.g. cooling plates or channels), exchangeability, or safety & reliability of the cells, as well as additional cables or power distribution elements required to transfer power from the non-rechargeable battery to the rechargeable battery or propulsors. Note that the range extender mass, regardless of type of range extender, is considered a part of the EOM.

Primary energy source: the rechargeable batteries for powering the propulsors.

Secondary energy source: energy source used by the range extender, which is of a different type than rechargeable batteries. For example, non-rechargeable batteries, or Jet A1 fuel. In the case of a non-rechargeable-battery solution, the secondary energy source is the non-rechargeable battery itself. In the case of a fuel-based gas-turbine solution, the range extender includes fuel as the second energy source as well as the other components as described herein.

Range extender effective energy density: effective energy capacity of the range extender, divided by the mass of the range extender.

Propulsor: device used to generate thrust; e.g. a propeller or fan.

Batteries "associated with wing": batteries which are installed in such a way that they contribute to a reduction in wing root bending moment during steady level flight. For example, batteries installed in the wing box (or in the volume of the wing), or batteries attached to the wing spars, the wing skin, or in pods installed on or under the wing.

"Rechargeable" battery: a battery (i.e. an energy storage device containing one or more electrochemical cells) whose energy can be charged again after being discharged by applying external electrical power; optionally, meaning that the battery is rechargeable in situ while installed in the aircraft.

Wing structural mass (WM): mass of the basic wing structure, including ribs, spar, skin panels, etc., but excluding secondary elements such as high-lift devices, spoilers, speed brakes, or actuator mechanisms. For an existing aircraft this can be measured, while in the conceptual design process it must be estimated. For the values and limits established in this document, the (basic) wing structural mass is defined following <NPL>.

Wingspan: distance from one wing tip to the other wing tip when the wings are positioned for normal flight. Wing: a wing has two (typically symmetric) halves; i.e. conventional (monoplane) aircraft have one main wing.

Battery mass/wing mass ratio (BM/WM): mass of the batteries which are associated with the wing adopting the definitions of 'battery mass' and 'associated with the wing' provided herein, regardless of whether they constitute the primary or secondary energy source, divided by the 'wing structural mass', as defined herein.

Load-carrying hatch: hatch that acts as an integral part of the wing structure when closed, transmitting aerodynamic, inertial, gravitational, or other loads from one point in the wing structure to another, and maintaining the desired shape and structural integrity of the wing in flight.

The following formulas and supporting description provide basis for calculations, estimations, principles and concepts described in the present disclosure.

The range of a battery electric aircraft is defined by equation <NUM>, known as the adapted Breguet equation: <MAT>.

Increasing either or both BM/MTOM and L/D is desirable for increased range. The other terms of equation <NUM> are defined herein in the symbols and parameters section and are essentially fixed at a maximum currently achievable value as will be described in the following description. As described herein in the definitions section, the product of the terms BM/MTOM and L/D in equation 1a is defined herein as the electric range factor 'ERF' given by equation 1b.

Equation <NUM> defines the energy efficiency of the aircraft in cruise flight: <MAT> (Note: <NUM> pax = <NUM> Newton).

Increasing PLM/MTOM reduces energy per pax km and therefore increased energy efficiency per passenger.

Another formula is the so-called unity equation: <MAT>.

This simply states that total aircraft mass (or MTOM) is the sum of maximum payload, batteries and the empty operating mass (EOM). Note that PLM is the maximum payload mass. This unity equation can also be written as a sum of three ratios: <MAT>.

Some of the design principles described herein aim to maximise BM/MTOM and/or PLM/MTOM, by minimising EOM/MTOM.

The adapted Breguet range and energy efficiency formulas (equations <NUM> and <NUM>) incorporate several parameters that are the focus of the design principles of the present disclosure. However, for calculations presented herein, some values must be assumed for these variables. These assumptions are representative of a "large" commercial transport aircraft. The reason for focusing on this aircraft category is explained in the following description, especially under the headings 'think big' and 'think <NUM>'.

ηelec = <NUM>%. ηelec is the total efficiency from battery discharge to energy delivered to the propeller shaft. It is the multiplication of four efficiencies (together with assumed values for calculation purposes): battery discharge efficiency (<NUM>%), cable efficiency (<NUM>%), inverter efficiency (<NUM>,<NUM>%) and electric motor efficiency (<NUM>%). The quoted percentage values are high but attainable levels for these components.

ηp = <NUM>%. ηp is the Propulsive Efficiency; a measure for the efficiency of the propeller in converting the power received from the propeller shaft into thrust and speed in cruise flight. The assumed propeller efficiency of <NUM>% is already realized in current fossil fuel turboprop aircraft. Distributed propulsion and optimized propeller design could further improve this.

ebat = <NUM> - <NUM> Wh/kg. There are several factors determining this parameter:.

Since useful battery energy density in <NUM> years from now is unknown, the principles and calculations in the present disclosure may apply a range of <NUM>-<NUM> Wh/kg. The lower end of this range represents current technology, whereas the upper end of this range is the aspired technology, e.g. as expressed by the NASA SABERS project. Several publications use much higher energy densities and still conclude that meaningful large scale battery electric aviation is not feasible. Therefore, showing the possibilities for battery electric aircraft with an energy density of <NUM>-<NUM> Wh/kg, proves the validity of the design principles of the present disclosure. However, in embodiments, the rechargeable batteries have an energy-to-mass ratio of at least <NUM> Wh/kg, preferably at least <NUM> Wh/kg, more preferably at least <NUM> Wh/kg. In any case, in embodiments, the rechargeable batteries have an energy capacity sufficient to provide the aircraft with range of at least <NUM>; at least <NUM>; or at least <NUM>.

L/D = <NUM>. Most regional and narrow body aircraft have an L/D of <NUM>-<NUM>, whereas current larger long-range aircraft approach an L/D of <NUM>-<NUM>. However, as discussed in the following description, L/D values of <NUM>-<NUM> can be assumed for a well-designed electric aircraft. For calculations, an L/D of up to <NUM> has been assumed.

The Breguet range (or Breguet cruise range) is calculated with these above-mentioned assumptions. This range is the theoretical maximum range in cruise flight. It assumes that all battery energy available, is used for propulsion and it does not take into account any efficiency losses due to taxi, take off, climb, etc..

The useful range is calculated by taking the Breguet range and making the following corrections:.

The useful range thus expresses the range that can actually be flown from 'gate to gate' in still air. Note: the range calculated for the various parametric designs (e.g. in table <NUM>) is the useful range, calculated as explained above.

Aircraft are required to carry sufficient fuel/energy for both the trip at hand and to cover diversions or other emergency situations. The required fuel (or energy) consists of following elements:.

The proposed design covers the taxi and trip energy through rechargeable batteries. The final reserve (loiter), alternate reserve and contingency reserve are covered through a range extender. The total range can be calculated as the sum of the useful range and the range stemming from the above three energy reserves.

The inventors have recognised that the conventional thinking in electric aircraft design envisages a very limited useful range for aircraft with rechargeable batteries. New design principles are proposed in the present disclosure which are contrary to existing trends, intuition and design ideologies for electric aircraft.

The present disclosure includes nine design principles that define a new design space for commercial battery electric aircraft. These nine principles can be used in any combination.

The Breguet range equation is independent of the size of aircraft. This applies both to the smallest radio-controlled aircraft and the Airbus A380. However, there are several scale effects that influence the parameters in the Breguet equation:.

There are two sets of airworthiness certification requirements for passenger aircraft. In Europe these are labelled CS-<NUM> and CS-<NUM>. In the USA a similar set of regulations exists. CS-<NUM> applies to aircraft with <NUM> passengers or less, and a maximum weight of <NUM>. CS-<NUM> applies to larger aircraft. The requirements of CS-<NUM> in many respects are more stringent than those of CS-<NUM>.

In order to realize a meaningful range, EOM/MTOM must be as low as feasible and L/D needs to be as high as feasible. The inventors have recognised that, considering the above mentioned considerations about scale affecting empty operating mass, empty weight fraction and L/D, the CS-<NUM> design space is much better suited for battery electric aircraft.

Therefore, in embodiments, the MTOM is greater than <NUM>,<NUM>. The MTOM may also be greater according to embodiments and improved effects on the range can be seen the higher the MTOM. For example, the MTOM is greater than <NUM>,<NUM>, optionally greater than <NUM>,<NUM>, optionally greater than <NUM>,<NUM>, optionally greater than <NUM>,<NUM>, optionally greater than <NUM>,<NUM>. The maximum MTOM may be <NUM>,<NUM>, <NUM>,<NUM> or <NUM>,<NUM>. Thus, the range of MTOM of rechargeable battery electric aircraft according to the present disclosure may be defined by any combination of these upper and lower limits, or any open range defined by the lower limits.

Prior studies on the potential of electric aircraft use modern short-range fossil fuel aircraft as reference aircraft for comparison. Short-range fossil fuel aircraft require relatively little fuel, and therefore have a low energy mass fraction (EM/MTOM), of the order of <NUM>% - <NUM>%. These aircraft typically have an empty operating mass fraction EOM/MTOM around <NUM>%. Such studies subsequently assume that, since batteries are heavy (i.e. battery energy density is low compared with jet fuel energy density), an electric aircraft would at best have a comparable EOM/MTOM. However, this assumption is incorrect, and has led numerous authors to focus on a wrong part of the design space.

At the dawn of the jet age in the <NUM>, several aircraft were developed with much lower empty operating mass fractions and much higher energy fractions than aircraft today. The Boeing <NUM> and Douglas DC8-<NUM> had EOM/MTOM fractions around <NUM>%. This was driven by the need to cover intercontinental distances, which, combined with the poor thermodynamic efficiency of first-generation jet engines and modest aerodynamics, led to a high fuel consumption. For example, Aerodynamic Design of Transport Aircraft, E. Obert, IOS Press, <NUM>, shows the EOM/MTOM and EM/MTOM fractions of several aircraft developed in the <NUM>-<NUM> timeframe. The author (Obert) concludes that <FIG> of his book "shows that for a certain aircraft category, the empty weight fraction is more or less constant and almost independent of aircraft size but is dependent on range. For a long-range aircraft, the empty weight fraction would be <NUM>% and the fuel fraction about <NUM>%, leaving <NUM>% for the payload. Short haul aircraft have a fuel fraction of about <NUM>-<NUM>%, empty weight fractions of <NUM>-<NUM>% and payload fraction of <NUM>-<NUM>%. " Obert uses weight but the reader will understand that "Mass" (kg) and "weight" (N) may be used interchangeably when describing a mass or weight fractions or correlations, since they differ only by a constant factor g, a term which cancels in such fractions or correlations.

In <NPL>, a similar relationship is observed. There, the author (Torenbeek) concludes that "this suggests that the EOM fraction is more closely related to the fuel fraction than to any other characteristic". Torenbeek then proposes a formula for Class <NUM> empty weight estimation for narrowbody aircraft (all units in kg): <MAT>.

Combining this equation with the unity equation (equation 3a) and specifying a PLM (e.g. <NUM> for a <NUM> pax aircraft), one can express both EOM and EOM/MTOM as a function of EM/MTOM. In addition, using equation <NUM>, the energy consumption per passenger kilometer as a function of EM/MTOM can be calculated. Equation <NUM> is provided or illustrative purposes only and the relationship between EOM, PLM and MTOM in embodiments may or may not follow this relationship.

<FIG>, respectively, show a plot of EOM/MTOM, EOM and energy consumption as a function of EM/MTOM (which can also be read as BM/MTOM for battery electric aircraft) calculated using Equation <NUM>. <FIG> and <FIG>, are all indicative and for illustrative purposes only and are not intended to limit the present disclosure. However, for clarity a number of assumptions are listed as follows. The EOM estimate is based on formula from<NPL>. The EOM (in kg) = <NUM>,<NUM> x PLM + <NUM>,<NUM> x MTOM + <NUM>. PLM is assumed to be <NUM> and is indicative of a <NUM> pax plane.

<FIG> show a clear relationship between three parameters and the energy fraction EM/MTOM:.

These correlations are counterintuitive and often poorly understood. Many authors implicitly assume that a low EOM/MTOM implies a low EOM and therefore a more efficient aircraft. However, compared to today's aircraft, the long-range jets and props of the <NUM> did not have a lower EOM/MTOM because they had a lower EOM, but because they had a higher MTOM as a consequence of the high energy mass.

A similar effect occurs for electric aircraft: in which case the EM/MTOM fraction is not high due to the long range, nor due to a poor thermodynamic efficiency, but because the energy source itself is not energy dense compared with fossil fuels and therefore very heavy at the energies needed to achieve longer range flights.

In other words, if comparing an electric aircraft and a fossil-fuel based aircraft, both designed for e.g. <NUM> range, the electric aircraft inherently has a higher EM/MTOM, and therefore inherently has a lower EOM/MTOM.

To illustrate this effect, the schematic shown in <FIG> conceptually depicts how EOM/MTOM, PLM/MTOM and EM/MTOM vary with the range (and how EOM/MTOM, PLM/MTOM scale with EM/MTOM). <FIG> shows a schematic plot with a vertical axis <NUM> representing mass as a percentage of MTOM and a horizontal axis <NUM> simultaneously representing aircraft range in km and EM/MTOM. The horizontal axis shows two scales for the range, a first scale <NUM> for fossil fuel aircraft and a second scale <NUM> for rechargeable battery electric aircraft. The plot shows three areas. a first area <NUM> representing PLM/MTOM, a second area <NUM> representing BM/MTOM and a third area <NUM> representing EOM/MTOM. The range values indicated in <FIG> are notional, indicative of typical values that could be obtained using a Breguet cruise range equation.

As can be seen in <FIG>, a first design space <NUM> exists at the lower end of the range (or EM/MTOM) scale on the horizontal axis and a second design space <NUM> exists at the higher end of the scale. It should be noted that the design spaces are only schematically represented and the scale of the markers representing the limits of the design space does not limit the present disclosure. In relation to fossil fuel powered aircraft, the first design space <NUM> represents turboprops and the second design space <NUM> represents long-range fossil fuel jets adopting the 'think big' and/or 'think <NUM>' design principles described herein.

As can be seen in the left-hand side of <FIG>, the first design space <NUM> is characterised by higher empty operating mass fractions, higher payload mass fractions, and lower energy mass fractions. As shown on the right-hand side of <FIG>, the second design space <NUM> is characterised by lower empty operating mass fractions, lower payload mass fractions, and higher energy mass fractions.

Table <NUM> compares the typical range, MTOM, EOM/MTOM, PLM/MTOM and EM/MTOM of several aircraft to reflect the trends shown in <FIG> with actual data. The ATR72-<NUM>, Q400, DC-<NUM>-<NUM> and B707-320B are known fossil fuel aircraft and the F9X represents a design for an electric aircraft having rechargeable batteries according to an embodiment.

Therefore it may be understood that a fossil fuel-based aircraft can be designed for either the first design space <NUM> of <FIG> (first range <NUM> of the order of <NUM>-<NUM>,<NUM>, high payload mass fraction) or the second design space <NUM> (first range <NUM> of the order of <NUM>,<NUM>-<NUM>, low payload mass fraction), depending on the targeted market segment. However, since the range of rechargeable battery electric aircraft is significantly lower than for a fuel-based aircraft, a meaningful mission capability can only be achieved if the range is as high as possible. The inventors have recognised that an electric aircraft designed according to the second design space <NUM> may achieve commercially meaningful mission capability. While the second design space <NUM> leads to lower payload-mass fractions than a fossil-fuel-based aircraft designed for the same range, <FIG> shows that the energy consumption per passenger-km is still competitive due to the substantially higher powertrain efficiency.

The inventors have recognised that a correct understanding of these scaling effects results in an apparently simple yet ubiquitously overlooked conclusion: a well-designed electric aircraft lies in a very different part of the design space than a conventional aircraft of a similar range capability. Retrofitting an existing aircraft with batteries, designing a new electric aircraft with the same mass fractions, or even designing a new electric aircraft for the same set of mission requirements as a short-range fuel-based aircraft results in a sub-optimal design.

This unique way of viewing the design problem for rechargeable battery electric aircraft results in three choices for designs proposed in the present disclosure. First, the mission requirements (payload, range, take-off distance, etc.) are not a given, but are treated as design variables in the exploratory phase. Second, for that exploratory phase, the mass fractions corresponding to an aircraft with a similar EM/MTOM are used, instead of an aircraft with similar range. And third, EOM/MTOM is selected as an important parameter to minimize when making design choices at vehicle level, since that maximizes PLM/MTOM and EM/MTOM. The design principles and choices described under the headings 'Associate batteries with the wing', 'Low power -to-weight ratio', 'Optimal wing loading', 'A low-wing configuration' and 'Load carrying hatches' in the present disclosure focus on this EOM/MTOM reduction. As shown in <FIG>, these design principles 'tilt the energy wedge downward'. <FIG> shows a replica of <FIG> for comparison and beneath it the same plot-type shown for rechargeable battery electric aircraft employing one or more the aforementioned principles which allow lowering the of EOM/MTOM.

If EOM/MTOM is reduced and BM/MTOM (as now we are describing battery electric aircraft in particular) maintains the values in the plot shown in <FIG>, PLM/MTOM is allowed to increase in proportion to the decrease in EOM/MTOM. Alternatively, BM/MTOM and PLM/MTOM can both be increased according to the desired purpose of the aircraft (balancing the PLM and range requirements, for example).

In summary, in terms of mass fractions, a well-designed electric aircraft should have more in common with a long-range fossil fuel aircraft from the <NUM> than with a modern short-range propeller plane. That is, for rechargeable battery electric aircraft according to the present disclosure, the battery mass may be at least <NUM>%, at least <NUM>%, at least <NUM>%, at least <NUM>%, at least <NUM>%, or even at least <NUM>% of MTOM. The empty operating mass may be less than or equal to <NUM>%, less than or equal to <NUM>%, less than or equal to <NUM>%, less than or equal to <NUM>% or even less than or equal to <NUM>% of MTOM. The payload mass may be at least <NUM>%, at least <NUM>%, at least <NUM>%, at least <NUM>% or even at least <NUM>% of MTOM. Embodiments include any of the rechargeable battery electric aircraft defined herein having combinations of the abovementioned limits of BM/MTOM, EOM/MTOM and PLM/MTOM (adding up to <NUM>% as per the unity equation).

Even if the skilled person was to realise that the empty operating mass is to be lowered or limited for increased range, there are no existing rechargeable electric aircraft that realise this because the battery mass fraction and lift to drag ratios are not sufficient to meet the electric range factors defined in the present disclosure.

Another characteristic of <NUM> long range aircraft (or of aircraft designed according to the second design space <NUM> of <FIG>) is that the fuselage is small compared with the wing size. In contrast, with electric aircraft designed using turboprop fossil fuel aircraft as a reference, the fuselage is larger compared with wing size. This is described further under the heading 'High L/D is a free gift'.

The relationship between EOM, PLM and MTOM shown in <FIG> and <FIG> hold true for conventional fossil fuel 'tube and wing' aircraft, that carry passengers and cargo in the fuselage and fuel/energy in the wing.

The position of fuel or batteries in the aircraft has a significant impact on the empty operating mass. Batteries do not lose their mass during flight, and while this is often considered a disadvantage, in many cases this can also be utilized to reduce the structural weight. The wing structure mass is driven predominantly by the wing bending moment at the wing root (wing/fuselage intersection). The fuselage structural mass is driven by fuselage size and weight carried in the fuselage.

The inventors have recognised that if the batteries are carried in the fuselage instead of in the wing, the following effects occur:.

Therefore, a design principle of the present disclosure is to associate the batteries with the wing in accordance with the corresponding definition provided herein. For example, the batteries can be loaded in the wing volume (in the wing box), or be housed on or under the wing. This contributes to a reduction in the wing-root bending moment because the mass of the batteries counteracts the contribution to the wing root bending moment from the lift in steady level flight. That is, the wing root bending moment in a first direction caused by lift is partially or wholly cancelled out by the wing root bending moment caused by the weight of the batteries associated with the wing or vice versa.

Distribution of the batteries along the wing in the spanwise direction contributes to maximize these benefits. This principle is well-known from <NUM>-1960ies studies for so-called span loaders: but this was applied to flying wings with all payload in the wing (see, for example, <FIG> of NASA/USRA Advanced Design Program Aeronautics Division. Final Report <NUM>-<NUM>. Design of a Spanloader Cargo Aircraft ). These aircraft concepts, although never built, showed that empty operating mass fractions of around <NUM>% are feasible. According to the present disclosure, it is not payload but rechargeable batteries that will be associated with the wing, in such a way as to reduce the wing root bending moment.

That is, even greater reduction in the wing root bending moment during normal flight can be achieved by adopting span loading principles for the rechargeable batteries. That is, the rechargeable batteries associated with the wing can be distributed across a spanwise direction in such a manner as to reduce the wing-root banding moment during normal flight. As will be understood by the skilled reader, except where described as particularly advantageous in the present disclosure, specific examples of this principle are a matter of design implementation based on the aircraft design. The inventors' contribution is to adopt these span loading principle specifically for the rechargeable batteries used to power the propulsors. Span loading principles may alternatively or in addition be adopted for the rechargeable batteries so as to reduce bending moments within the wing itself at locations other than at the wing-fuselage intersection.

<FIG> shows the magnitude of these effects by expressing MTOM as function BM/MTOM. <FIG> shows a plot having a horizontal axis <NUM> representing BM/MTOM as a percentage and a vertical axis <NUM> representing MTOM in kg. <FIG> shows a first plotted line <NUM> and a second plotted line <NUM> representing calculations for aircraft in which batteries are associated with the wing and fuselage, respectively. The calculations assume the weight of the wing and fuselage can be estimated using established semi-empirical methods (e.g. from<NPL>, which is sufficient for a first indication of the trends.

<FIG> shows that the effect of associating the batteries with the wing on battery electric aircraft weight is most pronounced at high battery mass fractions. For a given PLM (<NUM>,<NUM> in this case), at <NUM>% battery mass fraction, MTOM increases by approximately <NUM>% if batteries are placed in the fuselage instead of associated with the wing. This is due to the increase in structural mass needed to strengthen the aircraft to accommodate the higher wing root bending moment in steady level flight created by placing batteries in the fuselage. This directly translates into an increase in energy consumption and reduction in energy efficiency per passenger km.

The power-to-aircraft-weight ratio is the ratio between maximum continuous engine shaft power and maximum take-off weight (i.e., MTOM × g). The maximum continuous power is measured at sea level at standard atmospheric conditions.

Electric motors (or electric engines) differ in three main ways from turbine engines:.

Table <NUM> shows the maximum power differences between electric and turbine engines in index numbers for different density altitudes.

Power-to-aircraft-weight ratio is an important aircraft design parameter because it determines the powertrain weight fraction, and therefore also the EOM/MTOM, of the aircraft. The minimum allowable power-to-aircraft-weight ratio is determined by the flight performance requirements. The designer can choose the power-to-aircraft-weight ratio as long as the requirements are met (similar to the wing loading, discussed in the next section). For gas-turbine aircraft, the minimum allowable power-to-aircraft-weight ratio is typically limited by one of the three following performance requirements:.

For these reasons, for a battery electric aircraft, a power-to-aircraft-weight ratio of less than <NUM>% compared to turboprop aircraft is easily feasible. That is, aircraft according to the present disclosure may have a power-to-weight ratio of no more than <NUM>, no more than <NUM>, no more than <NUM>, or even no more than <NUM> kW/kg. In this case, the weight is MTOM and power is maximum continuous power while in flight.

The inventors have recognised that yet further improvements in rechargeable battery electric aircraft can be achieved by associating above a certain proportion of the rechargeable batteries with the wing. For example, aircraft according to the present disclosure may have at least <NUM>%; at least <NUM>%; at least <NUM>%; at least <NUM>%; at least <NUM>%; or at least <NUM>% of the total mass of the rechargeable batteries associated with the wing. This principle may be adopted with or without the span loading principles described herein.

Wing loading is the ratio of maximum take-off mass to the wing area. For commercial transport aircraft, the maximum allowable wing loading (i.e., the smallest possible wing size) is determined by a combination of two parameters in the approach/landing condition: the maximum lift coefficient (CLmax), and the approach speed, which is linked to the landing distance. Typical wing-loading values as provided in<NPL>, are approximately <NUM>-<NUM>/m2 for turboprops and up to approximately <NUM>-<NUM>/m2 for large jets.

It is commonly assumed that wing loading should be as high as possible, since it implies that the wing size is as small as possible. For a given wing aspect ratio ("slenderness"), a small wingspan is lighter. For a given wingspan, a small wing is more aerodynamically efficient. Because of this, large aircraft often use complex high-lift devices to enhance Clmax, and thereby enhance the maximum wing loading. Electric aircraft can further enhance this Clmax by using distributed propellers (propulsors) to "blow" additional air over the wing and increase the effective lift.

However, the inventors have recognised that for electric aircraft designed for commercial passenger transport, a very high wing loading is not beneficial. There are two reasons for this. First, a high wing loading requires more power from the engines to take off (in other words, it increases the required power-to-aircraft-weight ratio). While for gas-turbine aircraft the benefits of high wing loading outweigh the drawbacks of a high power-to- aircraft-weight ratio, for electric aircraft, which have heavy powertrains, the opposite occurs: it is more beneficial to have a small motor, even if this implies having a large wing. And second, a large wing provides more volume to house the batteries, further enabling the application of 'associate batteries with the wing' as described herein.

An understanding of this design principle results in the following design choice: compared to conventional jet aircraft operating from the same airfields with similar MTOM, a relatively lower wing loading is selected for the electric aircraft. Compared to turbo-prop aircraft, with much lower take-off and landing distance requirements, a much higher wing loading is selected. This results in wing-loading values of the order of ±<NUM>-<NUM> or <NUM>-<NUM>/m2 and, as a result, less complex high-lift devices are required.

It may be understood that the aircraft described herein adopt a fuselage and wing in a 'tube-and-wing' design. In this case, the wing can be joined to the fuselage in three ways;.

For passenger aircraft, a mid-wing configuration is very challenging, as the airframe structural weight increases if the spars of the wing are not continuous at the junction. A continuous spar is also challenging because it would have to cross the cabin halfway along the fuselage. This configuration therefore is not used for large (><NUM> pax) passenger aircraft.

For traditional fossil fuel aircraft, a high-wing or low-wing configuration have each their own pros and cons and therefore both are used. The low-wing design in general offers a weight advantage over a high wing design. This weight advantage is caused by the fact that the undercarriage length is relatively short and can be stowed in the wing. A high wing design either requires a large undercarriage (e.g. Fokker F27 and Fokker <NUM>) or an undercarriage joined to the fuselage (e.g. ATR <NUM>) and a strong (and heavy) construction between wing, fuselage and undercarriage to carry all loads, especially in taxiing and landing.

Still, the high wing design is often used for propeller aircraft. In this case, the high wing design allows a larger propeller diameter while maintaining the required ground clearance. Therefore, for turboprop aircraft to maximum <NUM> pax, the high wing configuration is the dominant design.

Existing studies and designs for electric or hybrid electric aircraft usually take existing turboprops as reference aircraft and therefore often propose a high-wing configuration. However, as will be explained, this approach is not conducive to producing rechargeable battery electric aircraft with longer ranges.

The inventors recognised the significance of the following four key differences between a traditional fossil fuel aircraft and a battery-electric aircraft:.

In arriving at a low-wing design, the inventors also recognised the significance of the following factors.

Rechargeable batteries degrade and must be replaced at certain intervals. One can expect typical replacement intervals of <NUM> to <NUM> months, depending on how the aircraft is used. The replacement procedure requires access to the batteries, which are placed, for example, in the wing box. Battery replacement can be considered a standard procedure but is not regularly required during line maintenance of the aircraft. Moreover, it can also be planned well in advance. Therefore, it is allowable for the replacement procedure to take substantial time (e.g. <NUM>-<NUM> hours), and it may be done in a dedicated environment with dedicated tooling (e.g. in a hangar).

This means that load-carrying hatches, which contribute to the wing structural strength but require a more complex installation/removal procedure, can be used to cover the openings used to access the rechargeable batteries when they need to be replaced or maintained. Despite the potentially longer installation/removal times, the load-carrying hatches distinguish themselves from other structural elements of the wing because they can be opened and closed multiple times as a part of a standard operating procedure. In this process of opening and closing, they do not have to be broken, dismantled or replaced by new hatches. It may therefore be understood that the load carrying hatches are arranged to undergo a cycle of removal and reattachment as part of a standard operating procedure.

Current fossil fuel aircraft also require access to the wing box for inspections or repairs; for example, to inspect the inside of the fuel tank. This is done by means of "access panels", which need to be opened regularly, in short time frames, and with simple tooling. Therefore, these panels cannot be constructed as a critical part of the wing structure, but instead all loads and stresses in the wing must be redirected around the opening. This requires a heavy aircraft structure because extra structural reinforcement needs to be applied around the access panels to carry applied loads around them.

According to the present disclosure, for battery replacement, a load-carrying hatch can be used to open and close the openings instead, where the removable panel is attached to the wing structure in a way that allows the panel itself to carry the loads. This allows a lighter overall construction because there is no need for a reinforced structure to be provided around the openings.

Therefore, aircraft according to the present disclosure can include a wing assembly including a wing structure comprising a load-bearing hatch, and rechargeable batteries disposed in (e.g. the internal volume of) the wing structure. The load-bearing hatch is arranged to open and close an opening in the wing structure, and the opening is arranged to allow access to the rechargeable batteries.

In embodiments, the load-bearing hatch is configured to bear at least a portion of a load applied to the wing structure, and/or transmit aerodynamic, inertial or gravitational loads exerted on the wing structure. At least part of the rechargeable batteries may be coupled to the load-bearing hatch so that the part of the batteries is supported by the load carrying hatch during flight and/or can be removed from the wing structure along with the load bearing hatch during maintenance.

It is to be understood that the present disclosure also relates to a wing assembly with a load bearing hatch whether or not the wing assembly carries rechargeable batteries and whether or not the wing is for an aircraft designed according to the other design principles defined in this disclosure. The meaning of load bearing hatch is defined under the definitions section of the present disclosure.

The Breguet range equation also features battery energy density as an input. The 'effective' energy density can be changed by using different energy sources or types of energy. Normally this would not make sense: the battery with highest energy density would always give the highest range, so any mix of battery types would only reduce range.

However, the effective range of an aircraft is the Breguet range minus the required range for flying to an alternate plus a so called 'final reserve range'. In total, these would increase the required range with ± <NUM>-<NUM> kilometer. This implies that a battery electric aircraft always carries energy for <NUM>, which it only uses in abnormal or emergency situations. Therefore, in the present disclosure, it is proposed to use this energy in a form, as light as possible, even if it is very costly and/or cannot be recharged, since it is hardly ever used.

Assuming a future battery energy density of <NUM> Wh/kg and energy consumption of approximately 130Wh/pax/km, the battery weight for the required reserves for a <NUM>-seater is approximately <NUM>. Assuming a SAF fuel range extender of <NUM> MW with specific power of <NUM> kW/kg and <NUM>% efficiency, the range extender weight would be <NUM> and required reserve fuel <NUM>. The 'effective energy density' of this SAF range extender plus fuel therefore is ± <NUM> Wh/kg. This effective energy density of a SAF range extender could equal the energy density of future Aluminum-Oxide (Al-air) non-rechargeable batteries or other metal-air batteries. These could be used as alternatives range extenders to further simplify the energy system and improve reliability.

Therefore, for rechargeable battery electric aircraft, two possibilities exist for carrying the energy for the required reserves: application of a regular fossil fuel range extender, used for alternate and final reserves and/or application of Aluminum-O2 (Aluminium-air), or other metal-air non-rechargeable batteries as alternative for range extender. In both cases, the effective energy density of the electric aircraft increases and a useful range of approximately <NUM>-<NUM> becomes feasible.

Therefore, according to the present disclosure, there is provided an aircraft comprising: a fuselage and at least one wing arranged in a tube-and-wing design; a plurality of propulsors; and a primary energy source configured to power the propulsors, the primary energy source comprising rechargeable batteries. The aircraft also comprises a secondary energy source configured to power the propulsors, the secondary energy source comprising a non-rechargeable battery having an energy density greater than that of the primary energy source.

The secondary energy source may have an effective energy density greater than <NUM> Wh/kg; greater than <NUM> Wh/kg; greater than <NUM> Wh/kg; greater than <NUM> Wh/kg; or greater than <NUM> Wh/kg. The secondary energy source is a fossil fuel, an SAF, an eSAF, or a non-rechargeable battery, for example a metal-air battery, or an aluminium-air battery.

The secondary energy source may be configured to operate exclusively as a reserve energy source, optionally for diversion to an alternative airport and meeting the required loiter and contingency reserves.

The secondary energy source may be used only for reserves, and not to enhance the useful range. However, the present disclosure is not limited thereto.

This aircraft may be designed according to one or more of the other design principles described in the present disclosure. However, the aircraft including the above-described secondary energy source is not limited thereto.

Another significantly influential parameter in the Breguet range equation is the lift-to-drag ratio; L/D. This parameter expresses the amount of drag that the aircraft experiences while generating the required lift. Since the lift equals its weight in cruise flight and engine thrust equals drag, the L/D ratio and MTOM determine the required thrust the engines should deliver in cruise flight.

Many factors determine the L/D ratio, however, for a regular 'tube and wing' aircraft two factors drive L/D:.

Many aerodynamic improvements have been considered in last <NUM> years to further enhance L/D. Examples are laminar flow profiles, tip propulsors, boundary layer ingestion, box wings, etc. However, attempts to apply such technologies to commercial transport aircraft usually results in modest or zero overall gains due to other implications for the aircraft's design.

Battery-electric aircraft have an aerodynamic advantage which is inherent their scaling effects (for example, those described herein with respect to engine motor size) and does not require additional complex technologies. Due to the low payload-mass fraction achievable with the other design principles described herein (for example 'think big' and 'think <NUM>'), battery electric aircraft with a conventional tube-and-wing configuration by definition have a relatively small fuselage and large wing.

<FIG> compares a <NUM>-seat battery electric aircraft with <NUM>-seat fossil fuel turboprop aircraft with equal wing loading (W/S) and equal wing slenderness (Aspect ratio; wingspan squared divided by wing area). The battery electric aircraft will have a much higher L/D relative to the fossil fuel aircraft, due to the relatively lower ratio of wetted area vs wing area. Thanks to this scaling effect, the increased wingspan causes the L/D to rise above <NUM>, to <NUM>-<NUM>. Aircraft according to the present disclosure may have a wingspan in flight (or maximum wingspan) of at least <NUM> meters, at least <NUM> meters, at least <NUM> meters, or even at least <NUM> meters. To accommodate airport requirements, the wing may include foldable tips.

To put these geometrical scaling effects into perspective, Table <NUM> compares the relative sizes of the wing and fuselage for the same aircraft presented in Table <NUM>. The table below compares the main characteristics of the wing and fuselage in one dimension (wing span/fuselage diameter or wing span/fuselage length), two dimensions (wing area/fuselage area), and three dimensions (wing volume/fuselage volume). For the area ratio, the fraction (<NUM>S)/(πDfuslfus) is employed, where the nominator is approximately equal to the wetted area of the wing (twice the planform area), and the denominator is approximately equal to the wetted area of the cylindrical fuselage (<NUM>πRfus · lfus).

Table <NUM> shows that higher aspect ratios are employed for the electric and shot-range propeller aircraft, than for the <NUM> jets. This leads to a lower induced drag coefficient, CDi. On the other hand, the ratio wing area/fuselage area is higher for the electric and long-range jet aircraft, than for the modern turboprops. This leads to a lower zero-lift drag coefficient, CD<NUM>.

Aircraft according to the present disclosure therefore have a wing-wetted-area to fuselage-wetted-area ratio of greater than <NUM>. Aircraft according to the present disclosure may have a wing aspect ratio of greater than <NUM>, greater than <NUM>, or greater than <NUM> and/or may have a wing area to fuselage area ratio of greater than <NUM>, or even greater than <NUM>. In more general terms the mathematical product of the wing aspect ratio and wing-area-to-fuselage-area ratio of aircraft according to the present disclosure may be greater than <NUM>, greater than <NUM>, or greater than <NUM>.

These aspects illustrate how an electric aircraft inherently has a lower drag coefficient (CD = CD<NUM> + CDi), and therefore a higher lift-to-drag ratio, than typical fuel-based aircraft. Note that, compared to the electric aircraft, the long-range jets have a smaller wing span relative to the fuselage diameter or length, but a comparable volume ratio. This is because the jet aircraft have a lower aspect ratio (span/chord) and taper ratio (tip chord/root chord) than the electric aircraft, leading to a large wing volume near the wing root. Aircraft of the present disclosure may therefore have a wing volume to fuselage volume ratio of least <NUM>, at least <NUM>, at least <NUM>, or at least <NUM>.

In Table <NUM>, the aircraft dimensions of short-range props and long-range jets is estimated based on publicly available data and sketches. The F9X electric model is an embodiment according to the present disclosure.

In Table <NUM>, underlined values highlighted in gray indicate values that differ by less than about <NUM>% from the electric aircraft.

Aircraft design often follows several steps. Starting from an initial specification, the aircraft designer develops an initial concept and verifies with a relatively simple set of calculations whether this concept is 'within the ballpark' of the top-level aircraft requirements (TLAR). The formulas and calculations that govern this conceptual verification are often labelled as 'Class <NUM>' estimates. These 'Class <NUM>' estimates are top-down (e.g. simple estimates of total aircraft mass, based on few parameters like payload mass and range, required power estimates, wing size estimates, etc.) and based on past experience.

As the design is further detailed towards a preliminary design, the designer can verify whether the design meets the specification through bottom-up 'Class <NUM>' estimates. These are weight estimates per aircraft component, based on formulas that have been derived from statistical correlations between certain parameters and the total weight of these components in existing designs. A similar approach is available for drag estimates and related performance estimates.

Only at the end of the detailed design process, a full weight and performance validation can be made. only when the wing is designed in full detail, the exact weight can be determined. However, there are some intermediate verification methods available for weight or drag estimation that combine both statistical models and physics-based models. These methods are often labelled 'Class <NUM>' estimates.

As per the principles set out in this disclosure, battery-electric aircraft designs exist in a new 'design space'. This by definition limits the usage of statistical approaches typically used in Class <NUM> design calculations. For critical elements like batteries, motors, cooling systems, etc. there is no prior experience. For other aircraft components and aircraft structures, existing Class <NUM> and higher estimates can be used, however, we must be mindful that these represent the 'fossil fuel'-past and sometimes this hinders the applicability of these estimates.

Therefore, in this disclosure, the evidence provided to prove the usefulness of the different design concepts is often based on 'Class <NUM>' estimates. In some instances, existing (fossil fuel based) Class <NUM> estimates have been adjusted and these adjustments have been estimated by extra calculations. The last section provides an initial set of calculations on 'Class <NUM>' level, to prove the applicability of the total set of design principles to maximize battery electric aircraft range.

Therefore, Class <NUM> methods have been used for the parametric studies in this disclosure, e.g. for all calculations regarding the relationship between EOM/MTOM and BM/MTOM, EOM and BM/MTOM, and energy efficiency (in Wh/paxkm) and BM/MTOM.

In the following calculations and examples, a refined 'Class <NUM>' analysis is used to calculate the weights, weight fractions, aerodynamic performance (L/D) and resulting range and energy efficiency of aircraft structures and systems that are comparable to fossil fuel aircraft and some simple estimates for other systems, based on established handbook methods and assumptions regarding new technologies (e.g. power-to-weight ratios for electric motors, weight estimates for heat pumps, etc.). See <NPL>; <NPL>; and <NPL>, for further details of these handbook methods.

According to recent consulting reports such as <NPL>, there are <NUM>+ new startups working on electric aircraft. The vast majority is in the eVTOL space: electric vertical take-off and landing vehicles for intra-urban transport of <NUM>-<NUM> passengers. There are also several General Aviation initiatives aiming on recreational flying and flight training (e.g. Bye Aerospace). There is only one EASA certified electric aircraft currently on the market: the Pipistrel Velis Electro <NUM>-seat trainer. Known initiatives of battery-electric aircraft for passenger travel in the CS-<NUM> design space are:.

Known initiatives of battery-electric aircraft for passenger travel in the CS-<NUM> design space include:.

There also have been several initiatives to electrify existing aircraft designs; that is, to retrofit an existing airframe with a new, battery-powered propulsion system. However, these initiatives where halted when the physical limitations of this approach became apparent. A simple illustration, based on the ATR <NUM> turboprop, reveals these limitations:.

Several parametric designs are now provided, by way of example only. The designs are of aircraft including fuselage and wing arranged in a tube-and-wing design; a plurality of propulsors; and a primary energy source configured to power the propulsors, the primary energy source comprising rechargeable batteries. The aircraft have a maximum take-off mass 'MTOM' of at least <NUM>,<NUM>; and an electric range factor 'ERF' of at least <NUM>. The aircraft may or may not include any of the features described under any or all of the design principles described above or two or more of the principles in any combination.

Three aircraft "sizes" are evaluated for a range of ERF values: <NUM> passengers, <NUM> passengers, and <NUM> passengers. The aircraft are designed for a runway length of approximately <NUM>, a cruise altitude of <NUM>, and a cruise speed of Mach <NUM>. A wing loading of MTOM/S = <NUM>/m2 is selected to meet the performance requirements, and the number and size of the propellers is adapted to maintain a constant disk loading among the various configurations. A wing aspect ratio of <NUM> is selected. For reserves, a <NUM> diversion is assumed, together with <NUM> mins loiter capabilities and an additional <NUM>% contingency reserve. These reserves are covered by a fuel-based range extender.

Since the battery energy density is largely determined by external factors unrelated to the aircraft design, for this comparison, a useful, end-of-life pack-level battery energy density of <NUM> Wh/kg is assumed. Aircraft range varies linear with battery energy density, and therefore the results can easily be extrapolated to other battery-technology levels.

The range, MTOM, energy consumption, empty operating mass fraction, battery mass fraction, lift-to-drag ratio, wing mass (excluding flaps and other secondary elements) and battery mass/wing mass fraction obtained for the various parametric designs are given in Table <NUM> and Figures <NUM>-<NUM>.

<FIG> shows how the range of the electric aircraft varies linearly with ERF, independently of the number of passengers, as expected from the Breguet equation. Moreover, <FIG> shows how the twelve designs fall in the design space of Claim <NUM> in terms of both ERF and MTOM, with the MTOM increasing with both passenger count and ERF (i.e., range). The MTOM values obtained for these designs range from typical turboprop values (20t - 30t) to narrowbody values (70t - 90t) and beyond (in the present disclosure 1t is <NUM>). Furthermore, <FIG> illustrates how the energy consumption per passenger kilometre improves with increasing passenger count ("think big"). The difference between <NUM> and <NUM> passengers is much smaller than between <NUM> and <NUM>, indicating that beyond <NUM> passengers, a plateau is approached in terms of energy efficiency per pax-km. Moreover, the energy consumption is lower for lower ERF values, since that corresponds to lower battery-mass fractions but higher payload-mass fractions.

<FIG> shows a schematic plot setting out a design space for passenger battery electric aircraft according to embodiments. The plot is defined in terms of the electric range factor on the horizontal axis <NUM> and number of passengers on the vertical axis <NUM>. The planform views of a first aircraft <NUM>, second aircraft <NUM>, third aircraft <NUM>, fourth aircraft <NUM>, and fifth aircraft <NUM>, according to embodiments appear across the design space. Design parameters for each of the first to fifth aircraft are provided in Table <NUM>.

The drawings show schematically how fuselage size increases only with payload (in this case number of passengers), while wing size increases with both payload and ERF (i.e., range). The contour of the middle configuration (<NUM> passengers, ERF = <NUM>) is indicated in gray transposed onto the other four configurations for comparison.

In <FIG>, where the comparison is performed at constant aspect ratio and wing loading, the wing span b is directly proportional to <MAT>. On the other hand, the size of the wing relative to the size of the fuselage, quantified using the area ratio Swing/Sfus, increases mainly with ERF, with higher values of SwinglSfus resulting in a higher lift-to-drag ratio. The ratio Swing/Sfus is defined as (<NUM>S)/(πlfusDfus), where the nominator is an approximation of the wing wetted area, while the denominator is an approximation of the fuselage wetted area. A higher value corresponds to a lower zero-lift-drag coefficient. This L/D increase partially contributes to the value of ERF, while the main reason for the change in ERF is the difference in battery-mass fraction. The figure also shows how different electric aircraft with comparable take-off masses (MTOM = <NUM> t ~ <NUM> t) can cover different missions: many passengers for a short range (<NUM> pax, ERF = <NUM>), moderate amount of passengers for a moderate range (<NUM> pax, ERF = <NUM>), or a small amount of passengers for a relatively long range (<NUM> pax, ERF = <NUM>). Furthermore, <FIG> and Table <NUM> shows how different numbers of propulsors are beneficial for different sizes of aircraft. The number of propulsors depicted in <FIG> is provided merely by way of example.

In summary, these design examples show that the design principles described in this disclosure are applicable to a wide range of payload, range, and other top-level aircraft requirements, while ensuring a technically feasible and energy-efficient aircraft.

As described herein and exemplified by the embodiments and examples, the proposed design principles primarily affect BM/MTOM and 'as a free gift' also increase L/D. Therefore, the parameter of merit for the proposed claim is the product of these two dimensionless parameters: <MAT>, referred to as the 'electric range factor' (ERF).

Assuming a <NUM>% power train efficiency and an <NUM>% propulsive efficiency, the Breguet range equation for battery electric aircraft can be rewritten as: <MAT>.

Note: R is in kilometers and ebat is in kJ/kg. <FIG> shows iso-range curves in a two-dimensional ERF vs ebat space. <FIG> plots Breguet cruise range and it may be understood that the example aircraft ranges are calculated based on more precise adaptions to the Breguet equation.

<FIG> gives a clear indication of what ranges are feasible in the design space (ERF is greater than <NUM>), depending on battery energy density and ERF. It is already known that, all other things being equal, the higher the energy density of the battery, the higher the range of an electric aircraft. However, a contribution of the present disclosure is to recognise that by designing the aircraft to increase the ERF, the range can be significantly increased. The higher the ERF, the lower the battery energy density needed to achieve a certain range. By employing the design principles, design features, or any of the embodiments described herein, the range and therefore viability of electric aircraft for commercial flights can improve significantly.

Claim 1:
An aircraft comprising:
a fuselage and at least one wing arranged in a tube-and-wing design;
a plurality of propulsors; and
a primary energy source configured to power the propulsors, the primary energy source comprising rechargeable batteries,
wherein the aircraft has:
a maximum take-off mass 'MTOM' of at least <NUM>,<NUM>; and
an electric range factor 'ERF' of at least <NUM>,
wherein: <MAT>
wherein L/D is the lift-to-drag ratio of the aircraft and BM is the mass of the rechargeable batteries, and characterised in that
the aircraft has:
a wing loading of <NUM>-<NUM>/m<NUM>, and/or
a wing-wetted-area-to-fuselage-wetted-area ratio of greater than <NUM>.