Wages of Flight

Copyright ©2010 by Paul Niquette. All rights reserved.
Solvers of Green Flight will be well acquainted with aerodynamic drag, specifically that there are two kinds, "parasitic drag" and "induced drag."  For our purposes here, it will be useful to regard the latter as resulting from the "Need for speed," as explored in other puzzles, including Look-at-Me Car and Steamboat Hill.  The latter form -- parasite drag -- is more properly named "lift induced drag."  It is a consequence unique to things that fly, and we have dubbed it Wages of Flight.

We seek a simple relationship between fuel consumption rate F (gph) and airspeed V (mph), beginning with these symbols...

D = aerodynamic drag (lbs)
a" = conversion parameter for parasite drag, dP = a" V 2 ~~~ "Need for Speed"
b" = conversion parameter for induced drag dI = b" / V 2 ~~~~Wages of Flight
One might readily appropriate a conventional equation for Induced drag while applying the so-called Drag equation for parasite drag and thus write the sum...
D = dP + dI =  a" V 2 + b" / V
...reminding ourselves that parasite drag increases as the square of airspeed while induced drag decreases with the square of airspeed.  As many as a dozen technical factors and coefficients can be found embedded in that expression. 

Conversion parameter a" has the units lbs/(mph)2 and varies somewhat with altitude and outside air temperature.  Conversion parameter b" has the units lbs-(mph) and varies with the square of lift, and lift is equal to aircraft weight.  Since aircraft weight can only decrease during flight, using gross take-off weight in our calculation will assure a conservative approximation of drag.  All other aircraft parameters, such as aircraft size and shape, do not change in flight, so we shall consider both a" and b" to be constant in level flight.

As seen in the solution to Green Flight requisite horsepower H is proportional to both airspeed V and thrust, the latter being equal to drag D, so we write...

H = D V = (a" V 2 + b" / V 2 ) V = a" V 3 + b" / V
...in which we may substitute conversion parameters a' and b' and write...
H = a' V 3 + b' / V
...wherein  a' has the units hp/(mph)3 and b' has the units hp-mph. 

In level flight with a constant power setting, both a' and b' are considered to be constant for engine parameters such as propeller speed and pitch.  One final pair of conversion factors a and b can be used to give us a simple equation for fuel consumption per unit time (gph) as follows:

F = a V 3 + b / V
...wherein a has the units gph/(mph)3  and b has the units gph-mph.  With an assumed specific fuel consumption (lb/(hp·hr) for the aircraft's engines, both a and b may be considered as constants. 

Our object now is to ascertain the numerical values of a and b for Amelia Earhart's Lockheed Electra 10E.  For that, two sets of corresponding values of F and V will give us two parametric equations in two unknowns. Here they are...

  1. Turning first to Fred Noonan's flight plan in The Clock Won't Wait, we obtain an estimated F = 50.0 gph for V = 157.0 mph. 
  2. Next we turn to readily available references and find that the Electra had a top speed of 202.0 mph according to its specifications.  Each of the 10E's Pratt & Whitney R-1340 Wasp S3H1 engines developed a maximum of 600 hp with a rated specific fuel consumption of 0.48 lb/(hp·hr) or 0.079 gal/(hp-hr) and thus would consume 47.7 gph per engine for a total of 95.3 gph at 202.0 mph. 
Accordingly, we merely solve these two equations...:
  1. 50.0 = a (157.03) + b / (157.0) 
  2. 95.3 = a (202.03) + b / (202.0)
...simultaneously to yield...
      a = 10.8 (10-6) gph/(mph)3 and...
      b = 1.29 (103) gph-mph, such that...

    F = 10.8 (10-6) V 3 + 1.29 (103) / V

The relationship above is plotted on the graph below, which also highlights Fred Noonan's flight plan values: 50 gph at an airspeed of 157 mph as well as the top speed values for the Electra at the right and top of the graph.

The estimated headwind of 15 mph is not indicated in this graph.  The resulting ground speed of 142 mph means that, consuming 50.0 gph, the Electra would be getting 2.8 mpg.  To make good the 2,556 miles from Lae to Howland would require a total of 18 hours of fuel or 900 gallons, leaving about 200 gallons in reserve.  It is reasonable to assume that, upon arrival in the vicinity of Howland, the Electra would be throttled back to save fuel.  At an airspeed of 100 mph, say, the engines would be consuming 23 gph according to the graph, and the 200 gallons in reserve would last for more than 8.5 hours. 

Reality #1:  Amelia Earhart and Fred Noonan faced higher headwinds.
Over the island of Nukumanu, some 850 miles from Lae, the Amelia Earhart reported a headwind of 26.5 mph.  If we assume...
{a} that wind speed to have prevailed for the whole 2,556 miles and 
{b} that no change in airspeed was made to overcome it...
...the flight's ground speed would have been reduced to 130.5 mph, and it would require 19.5 hours to reach Howland.  With an airspeed of 157 mph facing a 26.5 mph headwind, the Electra would be getting 2.6 mpg.  To make good the 2,556 miles would require a total of 983 gallons.  But that still leaves nearly 117 gallons. With the Electra slowed to 100 mph., 117 gallons would last more than 5 hours.
Reality #2:  Amelia Earhart and Fred Noonan faced a deadline.
Solvers of the Here Comes the Sun puzzle will be acutely aware that the rising sun would set a deadline for taking the last celestial fix.  Furthermore, at some point in the flight, Fred Noonan must have become concerned about whether the radio direction finding would be functional for homing to  Howland Island, as seen in the solution to Live Reckoning.  His original plan for the last celestial fix was apparently intended to occur no more than 200 miles away from Howland, a point that would be reached at about 16:30 GCT on the original flight plan facing the estimated 15 mph headwind. 

To make good the original 142.0 mph ground speed facing the 26.5 mph headwind, would require an airspeed increase to 168.5 mph.  Let this be our solution for Wages of Flight.. 

According to the equation derived above, 168.5 mph calls for a fuel consumption of 59.3 gph.  At 16:30 GCT, the Electra would arrive at the last celestial fix as planned, having consumed a total of 980 gallons, leaving only 121 gallons in reserve!  Note the exclamation point at the end of the previous sentence and the next one.  Amelia Earhart and Fred Noonan would have as much as 250 miles still to go!  We need to determine the best airspeed to use after the last celestial fix.  Here is a graph for doing that.

Slowing to 120 mph, still facing 26.5 mph headwind, results in a ponderously slow ground speed of 93.5 mph, and it would take more than two and a half hours to reach Howland, cutting the reserve in half.  Solvers of Shoot the Moon know that between 1800 and 1900 GCT, Amelia Earhart descended to 1,000 feet.  Every pilot knows that winds aloft diminish close to the surface. 

Accordingly, at 1,000 feet, a reasonable assumption for the headwind would be 15 mph as originally estimated in Fred Noonan's flight plan.  The resulting groundspeed flying at the economical 120 mph would then be 105 mph for the last 250 miles to the 157-337 LOP, saving about 20 minutes.  Given all the conditions known to solvers...
 

An estimate of between 167 and 170 mph might be reasonable for the overall airspeed used.

Ironically, insofar as fuel consumption is concerned, it would have been more advisable for Amelia Earhart to set her cruise speed slower than the median 168.5 mph (165 mph, say) and thus more economical.  Fred Noonan would then be required to take the last celestial fix farther from Howland resulting in larger navigation errors, as shown in the solution to the Live Reckoning puzzle and summarized in the solution to Which way, Amelia?


 
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