Issue 020 - Aviation - Fuel burn and range
Is a 24-hour nonstop flight fuel-efficient?
Reuters reported that a specially adapted Airbus A350-1000ULR flew 23,075 km from Melbourne to Toulouse in 24 hours and 24 minutes. Qantas says the future Project Sunrise passenger configuration is designed for just 238 seats. Estimate total fuel burn and fuel per passenger.
The problem
Estimate the total jet fuel burned during a 23,075 km, 24-hour 24-minute nonstop Airbus A350-1000ULR flight.
Then estimate fuel consumed per passenger if all 238 seats were occupied, and fuel per passenger per 100 km.
Compared with a hypothetical one-stop route covering roughly the same total distance, does nonstop probably save fuel by avoiding a second takeoff and indirect routing, or consume more because the aircraft must carry many hours of extra fuel as dead weight?
Because Fermi problems target an order of magnitude, I normally use no more than two significant digits and write most calculations in scientific notation; the Fermi reference explains both conventions.
Before checking sources
Matt's first pass
My intuition is that the energy cost of maintaining airspeed and staying aloft during the flight will be much greater than the energy cost of takeoff, so I wanted to test that first.
I assumed an Airbus airplane weighs somewhere between a large elephant, about 10^4 kg, and an adult blue whale, about 10^5 kg. I guessed the midpoint, 5 x 10^4 kg. Then I added the weight of about 240 passengers at 90 kg each, an additional 2.2 x 10^4 kg, so I used a mass without fuel of about 7.2 x 10^4 kg.
The average speed for 23,000 km in 24 hours and 24 minutes is about:
distance ~= 2.3 x 10^7 m
time ~= 8.8 x 10^4 s
speed ~= distance / time
~= (2.3 x 10^7 m) / (8.8 x 10^4 s)
~= 2.5 x 10^2 m/s
To figure out takeoff energy, I set it as approximately equal to the kinetic energy of an Airbus moving at 250 m/s:
takeoff KE ~= 1/2 x mass x speed^2
~= 1/2 x (7.2 x 10^4 kg) x (2.5 x 10^2 m/s)^2
I wrote that down as about 6.3 x 10^4 J, though that arithmetic is one of the things to check later.
For the energy cost of staying aloft, I assumed wind resistance would be negligible compared with the energy cost of overcoming gravity. Looking at slices of 1 second, the plane should drop by about 10 m per second, so we need to overcome that gravitational energy each second.
energy per second ~= m x g x h
~= (7.2 x 10^4 kg) x (10 m/s2) x (10 m)
~= 7.2 x 10^6 J/s
whole-trip energy ~= (7.2 x 10^6 J/s) x (8.8 x 10^4 s)
~= 6.3 x 10^11 J
From this, I thought the cost of maintaining altitude was about seven orders of magnitude greater than the energy cost of takeoff. Intuitively, more stops and carrying less fuel weight should mean much lower energy expenditure.
If overcoming gravity during flight is the main energy expenditure, and jets are about 50% efficient, I divided by about 9 x 10^7 J/L and solved for approximate fuel volume per kg of flying mass. I got about 0.10 L per kg.
fuel for 7 x 10^4 kg airplane ~= 7,000 L
fuel for carrying that fuel ~= 700 L
fuel for carrying that fuel ~= 70 L
fuel for carrying that fuel ~= 7 L
whole trip fuel ~= 7,777 L
If instead there was a stop at the halfway point, I estimated about 3,500 L of fuel for each half-trip, plus fuel to carry that fuel, for a full-trip total near 7,367 L. In that model, stopping midway would save about 410 L of fuel.
Calibration Score
Matt's Calibration Score: 15 / 100
Higher is better: earn points for accurate pegs, sound models, correct math, and a result close to the sourced answer. The image shows percent full of it: 100 minus the Calibration Score.
Pegs: 0/30. Aircraft mass, fuel burn, and energy-model pegs were badly low.
Model: 0/30. The flight model leaned on vertical support work rather than drag, lift-to-drag, and fuel burn.
Math: 5/10. Some arithmetic survived, but the setup drove the answer far away from the sourced scale.
Result: 10/30. The qualitative conclusion about nonstop fuel penalty was useful, but the fuel quantity was off by orders of magnitude.
Grounding facts
The surprising passenger result is that a giant airplane can look fairly efficient per passenger-kilometer when it is full, even while burning a huge absolute amount of fuel. A central estimate of 180,000 liters is enormous, but spread across 238 people and 23,075 km, it becomes about 3 L/passenger/100 km.
Ultra-long-haul flying has a compounding penalty: fuel has weight, and fuel carried for the end of the flight must itself be carried through the beginning of the flight. That is why route planners care so much about range, payload, winds, reserves, and intermediate stops.
After checking sources
Check and recalibrate
The first big correction is mass. Airbus lists the standard A350-1000 maximum zero-fuel weight as 223 tonnes and maximum fuel capacity as 168,300 liters. The Project Sunrise version is reported to add about 20,000 liters of fuel capacity, so a rough fuel-capacity peg is about 1.9 x 10^5 liters.
A simple capacity-and-time estimate is therefore:
flight time ~= 24.4 hours
average fuel burn ~= 6 to 8 tonnes/hour
fuel mass ~= (24.4 h) x (6 to 8 tonnes/hour)
~= 1.5 x 10^2 to 2.0 x 10^2 tonnes
Jet fuel density is about 0.8 kg/L, so:
fuel volume ~= (1.5 x 10^5 to 2.0 x 10^5 kg) / (0.8 kg/L)
~= 1.9 x 10^5 to 2.5 x 10^5 L
The upper end is too high for a practical A350-1000ULR fuel load, so the best Fermi answer is roughly 1.5 x 10^5 to 1.9 x 10^5 liters, with 1.8 x 10^5 liters as a useful central estimate.
A drag-work estimate lands in the same neighborhood. NASA explains that in cruise, lift is about equal to weight and thrust is about equal to drag. For a modern long-haul aircraft, use an L/D ratio around 20. If average aircraft mass during the flight is roughly 250 tonnes, then:
average mass ~= 2.5 x 10^5 kg
weight ~= mass x g
~= (2.5 x 10^5 kg) x (10 m/s2)
~= 2.5 x 10^6 N
drag ~= weight / (L/D)
~= (2.5 x 10^6 N) / 20
~= 1.25 x 10^5 N
distance ~= 2.3 x 10^7 m
useful work ~= drag x distance
~= (1.25 x 10^5 N) x (2.3 x 10^7 m)
~= 2.9 x 10^12 J
Jet fuel contains about 35 MJ/L, and not all of that becomes useful propulsive work. If useful efficiency is around 30% to 40%, then useful work per liter is about 10 to 14 MJ/L:
fuel ~= (2.9 x 10^12 J) / (1.0 x 10^7 to 1.4 x 10^7 J/L)
~= 2.1 x 10^5 to 2.9 x 10^5 L
That simple model is high because the average mass, efficiency, and L/D assumptions are rough, but it correctly shows why the answer is hundreds of thousands of liters, not thousands. Drag, not an imagined one-second gravitational drop, is the central cruise cost.
Now compute the hypothetical passenger metric using 238 occupied seats:
fuel per passenger ~= (1.8 x 10^5 L) / 238
~= 7.6 x 10^2 L/passenger
distance units ~= 23,075 km / 100
~= 2.3 x 10^2 hundred-km
fuel per passenger per 100 km ~= (7.6 x 10^2 L) / (2.3 x 10^2)
~= 3.3 L/passenger/100 km
A reasonable answer is therefore about 3 liters per passenger per 100 km, perhaps 3 to 4 L/passenger/100 km depending on actual fuel load and passenger/cargo assumptions.
For the one-stop comparison, Matt's intuition about fuel weight is probably right. An extra takeoff and climb do cost fuel, but a 24-hour nonstop aircraft carries enormous fuel mass early in the flight. Splitting the trip into two legs lets the aircraft fly both halves at lower average weight. If the route distance is similar and the stop does not add large detours or operational waste, the one-stop version probably burns less fuel.
The commercial appeal of the nonstop is not likely pure fuel efficiency. It is time savings, convenience, premium pricing, fewer missed connections, and the value some passengers place on avoiding a stop. Qantas itself says Project Sunrise can reduce point-to-point travel time by up to four hours compared with one-stop flights.
Post-check reflection
Matt's reflection
My airplane mass estimate was about one-third of what it probably should have been, maybe a bit lower. That was one of the less significant errors.
I also did not have the right mental model for what sort of energy expenditure I needed to calculate: drag was the big issue rather than overcoming gravity directly. I was not familiar with using the L/D ratio to estimate cruise work, so I was way low on energy usage. I also did not do a great job of figuring out the cost to take off and underestimated both. In the end, I was a few orders of magnitude low on the fuel required for the trip.
My intuitions were still correct about whether a direct flight was more efficient than a partial trip: it is probably more efficient to stop and refuel. But I expect the draw to the direct flight is the time savings. We are happy to spend more and consume more fuel if it saves us half a day.
Recommended memory peg
Remember jet fuel is about 0.8 kg/L and about 35 MJ/L, large widebody cruise fuel burn is roughly 5 to 8 tonnes/hour, and modern airliners have a cruise L/D around 20. For aircraft fuel Fermi problems, use fuel per passenger per 100 km = total fuel / passengers / (distance/100).
Reader results
Bars show how submitted estimates sort into the answer choices from the gut-check prompt.