Atp FLT Plan 5
Atp FLT Plan 5
FLIGHT PLANNING
1. Planning Revision 01
2. Cruise Performance 13
3. Flight Plans 19
4. Graphs 37
5. Weight & Balance 43
6. Critical point 47
7. Point of No Return 49
PLANNING REVISION
In the process of compiling a flight plan for an aircraft, the weight schedule must be
consulted to ensure that certain weight limitations are not exceeded. In later chapters,
balance limitations (location of the C of G) will also be considered. The weight schedule
given below is the ideal and complete one, although certain operators may elect to combine
items in order to abbreviate the process.
Least of 3 method
Step 1
Calculate fuel at Brakes Release….
Step 2
MTOW 89 350kg
MLW+trip fuel 85 062kg (72 600+12 462)
MZFW+fob 80 642kg (63 500+17 142)
MZFW 63 500kg
- Basic weight 47 000kg
PAYLOAD 16 500kg
NOW….
If it was the TOW that was found to be the lowest you would :
Landing Weight
-Taxi Fuel
-Reserve Fuel
-Basic Weight
PAYLOAD
WEIGHT LIMITATIONS
Using the above figures found in the manual, what is the maximum amount of start up and
taxi fuel that can be carried?
The physical dimensions of the Runway, Stopway and Clearway have a very definite effect
on an aircraft's Maximum Take-Off Weight.
THE STOPWAY
The Stopway is an extension to the end of the runway, which may be used to stop the aircraft
in the event of a rejected take-off. The Stopway must be at least as wide as the runway, able
to support the aircraft without incurring structural damage, but is not intended for normal use.
THE CLEARWAY
The Clearway is an area beyond the end of the runway, which complies with the following
criteria:
03 21
100ft
600ft
End of runway Runway length 1950ft Clearway
The length of runway available for the ground run of an aircraft taking off.
Runway 03 : 1950 ft
Runway 21 : 1950 ft
Runway 03 : 2550 ft
Runway 21 : 2250 ft
The total distance required to reach a height of 35 ft at a speed not less than V2, after failure
of the critical power unit at V1 (also known as accelerate go distance required).
Or
115 % of the total demonstrated distance required to reach V2 at 35 ft over the runway with
all engines operative.
Runway 03 : 2150 ft
Runway 21 : 2250 ft
The Accelerate Stop Distance for either the engine out or all engine case, is the sum of the
following:
1. Acceleration distance from brake release to speed V1
2. Distance from V1 to application of full braking
3. Distance with full braking applied to stop. (one braking aid not considered)
A recognition time, i.e. between the actual engine failure and recognition by the pilot
is built into the engine out Accelerate Stop Distance .
Minimum time intervals between V1 and each subsequent braking action are given.
The Accelerate Stop Distance required is the greater of either the engine out or all
engine Accelerate Stop Distances.
REFERENCE ZERO
This is the reference to which the co-ordinates of the various points in the take-off flight path
are referred. It is defined as the end of the Take-off Distance Required and is 35 feet below
the flight path at this point.
The length of the runway, which is declared to be available and suitable for a landing. The
landing distance available commences at the threshold and in most cases corresponds to the
physical length of the runway. HOWEVER, if the threshold is displaced, the landing distance
available is reduced and will normally be the distance between the threshold and the far end
of the runway.
Runway 03 : 1850 ft
Runway 21 : 1950 ft
BALANCED FIELD
The balance field occurs when the accelerate stop distance required equals the engine out
distance to 35ft.
The V1 speed is the speed which the pilot used as a reference in deciding whether to
continue or to abort the take off .
V1 is selected so that:
1. If the take-off is continued after an engine failure recognized at or above V1
speed it will be possible to attain a height of 35ft within the scheduled take off
distance, or
2. If the take-off is abandoned at or below the V1 speed it will be possible to
bring the aircraft to a stop within the scheduled accelerate stop distance.
The scheduled take off field lengths are based on stopping if an engine failure is recognized
before reaching V1 and on continuing the take off if the engine failure is recognized after V1.
An appropriate time interval is allowed between recognition of the failure and completion of
all actions required for rejection. It is also required that one of the available braking systems
must not be used during certification or if all braking devices are used that an additional
factor be applied.
If the runway surface is contaminated by, for example, water or snow, the aircraft will require
more runway length to reach take-off speed. If this extra runway length is not available, the
aircraft's take-off weight will have to be reduced.
RUNWAY SLOPE
An uphill slope requires a longer take-off run, and therefore, possibly a reduction of the take-
off weight. A runway with a downhill slope would have the opposite effect.
A point worth bearing in mind is that an uphill slope would mean less distance required to
bring the aircraft to a stop in the event of rejected take-off and vice versa for a downhill slope.
A definitive answer on the effect of slope on an aircraft's take-off weight would, of course, be
extracted from the appropriate performance graphs.
A tailwind component at take-off increases the amount of runway required for take-off, and
therefore, possibly a reduction of the take-off weight. A headwind component at take-off
would have the opposite effect.
The combination of weight and air density (altitude and temperature) affects the performance
of the aircraft, and even if the aircraft can get off the ground with an engine failure at V1, its
rate of climb would be too low to satisfy the required climb gradients during the Take-Off
Flight Path.
This will be that portion of the flightpath, which begins at a height of 35ft above the runway
i.e. the end of the Take-Off Distance Required. It should be assumed that this height is
reached at the end of TODR, with one engine inoperative. The Take-Off Flightpath ends
when the aircraft is 1500ft AGL or clear of the last obstacle.
This represents the Gross Take-Off Flightpath, reduced by the amount considered necessary
to allow for various contingencies, i.e. the need to manoeuvre, unavoidable variations in
piloting technique, temporary below average performance and take-off on wet or slushy
runways, etc.
The Net Take-Off Flightpath should clear en-route obstacles by at least 35 ft with one engine
inoperative.
V2
Gross
Gear Up
400ft
Net
1500ft
FIRST SEGMENT
SECOND SEGMENT
THIRD SEGMENT
FOURTH SEGMENT
NOTE:
The gradients quoted are for a four engined jet aeroplane with one engine inoperative.
The performance classification number for a runway is an expression of its bearing strength.
The aircraft classification number is derived graphically using its single isolated wheel
loading (SIWL) and tyre pressure. ACN can also prove to have a limiting effect on the
maximum take-off weight of an aircraft.
In the process of bringing an aircraft to a stop, its brakes convert kinetic energy into heat
energy. The amount of heat energy that the brakes can absorb certainly has limits. The
greater the take-off weight of an aircraft, the higher its take-off speed will be and the more
energy the brakes will have to absorb in the event of a rejected take-off. Although the brake
energy limit (known as Vmbe) may not directly limit the take-off weight, many aircraft have a
minimum turn around time between landing and subsequent take-off, which will ensure
adequate braking in the event of a rejected take-off. This minimum turn around time is
directly proportional to the weight at which the aircraft landed and the weight for the next
take-off.
Much like the aircraft's brakes, the tyres also have certain limitations to ensure their structural
integrity. The limit is the maximum true ground speed that the tyres can absorb. The higher
the take-off weight of the aircraft, the higher the take-off speeds will be, and this may prove
to be a limiting factor requiring a reduction in the maximum take-off weight.
HUMIDITY
Humidity and air density are inversely proportional. The greater the humidity, the less the air
density. Piston engine aircraft performance is adversely affected by humidity to the extent
where maximum take-off weight may be limited. The effect of humidity on jet engine
performance, however, is negligible.
FLAPS
The effect of flaps on maximum take-off weight varies from aircraft to aircraft and from flap
setting to flap setting. Factors to be considered are not only the effect of flaps on the take-off
run, but also on the initial climb performance after take-off. A definite answer on the effect of
flaps on an aircraft's maximum take-off weight would be extracted from the appropriate
performance graphs.
In conclusion, all of the above mentioned factors may limit an aircraft's maximum take-off
weight and it is the most limiting case that will determine the aircraft's actual take-off weight.
Maximum floor load is an indication of the physical bearing strength of the aircraft's floor,
normally in the cargo or baggage area. It is an expression of the maximum weight that can
be borne per surface area. Because maximum floor load is derived by weight per area, the
height of any object to be loaded is of no consequence.
In most load calculations, the maximum floor load of the aircraft is given. The pilot must
calculate the area of the object to be loaded and its weight, to check whether it may be
loaded.
To calculate the area of a circular object, for example a barrel, use the formula:
AREA = pr²
EXAMPLE:
The maximum floor load of an aircraft's cargo hold is 700 Kg/m². What is the
maximum weight that can be loaded onto a pallet that measures 2 m by 3 m?
= (2 m x 3 m) x
= 4200 Kg
Vr : Rotation speed
Vs : Stall speed.
b) Determine the maximum payload in an average W/C of -50 kts for the flight.
a. 89 000kg
b. 88 000kg
c. 86 000kg
2. Using the same data as in (A), beyond which value of headwind would the payload
have to be reduced?
a. 84kts
b. 82kts
c. 83kts
5. FAGC elevation 5327 ft, QNH 1007.4 hPa. Temperature + 24°C. What is the density
altitude?
a. 2400ft
b. 7903ft
c. 5503ft
8. With reference to question 7 above, what is the take-off distance available on runway
33?
a. 8600ft
b. 9200ft
c. 9800ft
9. Plan a flight from A-B. Fuel is prohibitively expensive at B, so plan not to uplift before
returning to A. Plan to carry minimum fuel on departure at A, because fuel isn’t cheap
there either
CRUISE PERFORMANCE
The aim of this chapter is to illustrate the various methods of expressing and calculating an
aircraft's performance. In doing so, students should refresh their memories concerning the
use of the 1/x function on their calculators. The use of this function can greatly reduce the
workload during performance problems.
NOTE: You are reminded to be aware of the difference between Specific Gravity (SG) which
relates to 1 imperial gallon or 1 litre of water and Specific Weight (SW) which relates to the
US gallon only.
BASIC PERFORMANCE
RANGE PERFORMANCE
The amount of distance that can be flown for a given amount of fuel.
The combination of two factors, distance and fuel, gives rise to numerous expression
of range performance.
E.g. :
EXAMPLE:
i) ANM/LBS
ii) LBS/GNM
SOLUTION
From the series of performance expressions, select two which will satisfy the
requirements in terms of units:
IN CLASS EXAMPLES
1. Given: TAS 240 kts WC +30 kts TW GS 270 kts Fuel Flow 750 Lbs/Hour
GS 270 Kts
Then aircraft performance is ? = 0.36 GNM / LB
Fuel Flow 750 Lbs / Hour
OR
Fuel Flow 750 Lbs / Hour
= 2.7778 LB / GNM
GS 270 Kts
3 An aircraft at FL 350, TAS 232 kts, Fuel Flow 545 LBS/Hour has a performance of
0.355 GNM/LB.
The Wind Component affecting the aircraft is :-
4 An aircraft flying at FL 310 at TAS 494 kts obtains a performance of 46.06 ANM/1000
kgs in Zero Wind conditions. At FL 350 the TAS is 484 kts and the performance is 48.36
ANM/1000 kgs. It will be less economical to cruise at FL 350 if the Head Wind
component is greater than:-
1. Track 058° (T), W/V 240/20, TAS 240 kts, Fuel flow 1500 LBS/Hr
a) GNM/LB
b) LBS/ANM
Calculate:
3. TAS 210 kts, Performance 6.5 LBS/GNM, Fuel flow 166.5 US GAL/HR, SG 0.8.
Calculate:
a) G/S
b) The wind component
4. Cruising at FL 160, TAS 220 kts, F/F 1500 LBS/HR, Track 238° (T), W/V 040/20.
At FL 180, the TAS will be 230 kts and the fuel flow only 1400 LBS/HR, but the W/V
360/05. Will it be worthwhile to climb to FL 180?
6. On a flight from A - B, distance 800 nm, the aircraft has 900 USG of fuel (SG 0.79)
excluding reserves. What is the maximum TAS at which the aircraft can fly the route
if there is a constant wind component of -10 kts for the route?
TAS F/F
8. TAS 500 kts, F/F 4743 USG/hr, SG 0.67, performance 0.037 GNM/kg. What is the
wind component?
10. FL 290 TAS 501kts, performance 94.8 ANM/1 000 kg, Zero wind.
FLIGHT PLAN
The CAA requirement for this section is to perform some, or all of, the following calculations,
using the B747 manual:
A climb.
A cruise sector (normally two).
A descent.
A diversion to alternate.
A hold.
In essence, this is almost the same as completing an entire flight plan except -
One of the most important points to bear in mind when answering these questions, is the
sequence of fuel used throughout a flight:
RAMP WEIGHT
- TAXI FUEL (600 kg)
TOW
- TRIP FUEL
- 4 % (Standard contingency or reserve)
- APPROACH FUEL (Standard 1 100 kg)
Landing Weight at destination or overshoot
- ALTERNATE FUEL
- 4 % of ALTERNATE FUEL (Standard contingency or reserve)
Landing Weight at Alternate or Enter Hold
- HOLDING FUEL
- MINIMUM IN TANKS (Standard 1 600 kg)
ZFW
Refer graph:
Using the graph, find the Optimum altitude if the TOM is 340 000kg, and the aircraft will
cruise at Long Range Cruise (LRC) 30 800ft.
Find the optimum altitude for a flight from Luxemburg to Munich, distance is 236nm, the TOC
weight is estimated to be 245 600kg, and the temperature deviation is expected to be ISA
+15c. Find the optimum altitude under these conditions for this flight… 27 500ft
- Time to climb.
- Fuel to climb.
- TAS in the climb.
All from SEA LEVEL to the chosen FL. At the bottom of each page is a fuel correction table
for departure airport elevation.
EXAMPLE:
- 22 MINS to climb.
- 8 950 kg of fuel to climb (from sea level)
- 142 NAM to climb
- 448 Kts TAS in the climb
From the bottom of the page adjust the climb fuel for the departure airport elevation.
Further data that can be calculated for a climb sector: If the CAA offers the true track
and wind for the climb.
Refer to page 1-2-2 for drift angles and wind components. The left hand table is for climb,
descent and diversion and the right hand table is for the cruise. The vertical axis of the table
is for the angular difference between the wind and the track. The horizontal axis is for the
wind speed.
The angular difference between the wind and the track is 60°. Look this up on the left-hand
table. The 60 is listed with 300 because a wind 60° off track is the same as a wind 300° off
track, except the one will drift you left and the other will drift you right. Now look up 60°
against 40 Kts wind speed.
This completes the data that can be calculated for a climb. The most popular CAA question
for the climb is only the fuel calculation, but with a correction for departure airport elevation.
Remember that even though it may be offered, the wind will have no effect on either the fuel
or the time to climb.
EXAMPLE:
TOW 336 500 kg. Climb to FL 310. Departure airport elevation 5 500ft
ISA + 15°C. Track 165° (T). Wind 070/60.
Because of the TOW, this example requires interpolation to derive the answers.
The first set of tables is for a M0.84 cruise and the second set of tables is for a Long Range
Cruise (LRC). The vertical axis of the table is for the gross weight of the aircraft and the
horizontal axis is for the flight level at which the aircraft is cruising.
This means that to use the aircraft weight at the beginning of a cruise sector would be to
incur an unfair penalty in terms of fuel flow. Likewise, to use the aircraft weight at the end of
a cruise sector would be too generous in terms of fuel flow. Instead, the weight halfway
through the cruise sector should be used as being most representative of the aircraft weight
throughout the cruise sector. This weight is called the mid-zone weight (MZW).
An MZW should always be derived twice in order to refine its accuracy. The first MZW is
called the approximate MZW and the second MZW is called the actual MZW.
EXAMPLE:
LRC ISA + 10°C FL 310. Aircraft weight at the commencement of the cruise sector 290
000 kg. Sector distance 620 NM. True track 020°. Wind 160/70.
Refer to page . 3-2-5(a). Against FL 310 and 290 000 kg, read off.- TAS 501kts.
- FF 11 408 kg.
Now determine the wind component and drift angle from table 1-2-2. (Right-hand table for
the cruise.) The angle between the track is 140° (vertical axis) and the wind speed is 70 Kts
(horizontal axis).
- Drift is 5°.
- Wind component + 52 Kts (tailwind).
Now using this actual MZW, do the computations for the cruise sector one last time to
derive the CAA answer.
Against FL 310 and 283 721 kg.
The first column gives the flight level, the second column gives the cruise speed and the
fourth column gives the weight at which a climb to that flight level is optimum.
With reference to the previous example, the aircraft, at LRC, could climb from FL 310 to FL
350 when the weight is 281 000 kg or less.
A very simple method is used for calculating this en-route climb: assume 100 KG FUEL
BURN PER 1 000ft CLIMB. Subtract the climb fuel from the weight at the commencement
of the sector to derive a new weight at the commencement of the sector i.e. assume the
aircraft went vertically up at 100 kg/1 000ft but with no distance or time used up on that
cruise sector at the new flight level.
EXAMPLE:
M0.84. FL 330 climbing to FL 370. Cruise sector 496 NM. Temperature at FL 370 ISA
+15C. Wind 260/60. True track 140°. Weight at commencement of the cruise sector
260 000 kg.
TAS 498 KTS and G/S 525 KTS remain unchanged, therefore, time remains 57 mins.
F/F : 10 048 KG/HR - 9 704 KG/HR = 344 KG/HR
344 KG/HR 0.486 = 167 KG/HR
9 704 KG/HR + 167 KG/HR = 9 871 KG/HR
9 871 KG/HR 57 MINS = 9 326 FUEL BURN
9 326 KG 2 = 4 663 KG FUEL TO HALFWAY
Although not a common occurrence it may happen that the aircraft has to descend to a new
flight level before continuing in the cruise (perhaps due to changing track requiring a change
from odds to evens or vice versa or perhaps due to conflicting traffic joining the same
airway).
Should the CAA pose such a question in the exam, the solution is simple - pretend it never
happened, just continue the cruise at the new flight level with the descent having no effect
whatsoever on time, speed or fuel for that sector.
- Time to descend;
- Fuel to descend;
- Distance (NAM) to descend.
The effect of destination airport elevation on time, fuel and distance to descend may be
ignored.
If the CAA offers you the true track and average wind in the descent then:
In order to calculate a flight to alternate, the first step must be to select a suitable flight level.
For this purpose, use the bottom graph on page 2-2.
The following data must be given to you in order to use this graph:
EXAMPLE:
Distance to alternate 325 NM. Forecast temperature for the upper levels ISA + 15°C.
TOW 315 000 kg. Trip fuel 106 000 kg. ODDS sector.
Now, enter the graph with the distance, temperature and weight:
- Answer 37 600ft.
- Therefore, choose FL 370.
If this had been an evens sector, choose FL 350 (the next one lower), not FL
390, as it would be above optimum.
Now, in order to calculate the time and fuel to alternate, use the graph on page 3-5-5.
EXAMPLE:
First calculate the landing weight at alternate - a catch 22 question, because you are trying
to calculate the fuel to alternate. .
As can be seen, the standard figure of 13 000 kg is a sensible one, because now with the
benefit of having completed the question:
Using the standard 13 000 kg, we derived a landing weight of 196 000 kg which is
certainly close enough.
As can be seen from the table, as the aircraft weight reduces in the hold, so the fuel flow
decreases, in other words, a holding MZW must be calculated in order to derive the fuel flow
in the hold. Once again, a standard figure is used. This standard figure assumes that a
standard 30 minutes hold would correspond to a fuel burn of 4 400 kg, therefore, halfway
through the hold, the aircraft would have burned off 2 200 kg.
EXAMPLE: TOW 315 000 kg. Trip fuel 106 000 kg. Fuel to alternate 8 700 kg. Hold
for 30 mins at FL 150.
The CAA could also have given the same question except requiring the holding MZW to be
calculated in reverse.
EXAMPLE:
The B747 arrives overhead destination with 23 500 kg fuel in tanks. ZFW 222 000 kg.
Fuel to alternate 8 000 kg. Contingency 320 kg. Fuel to hold at alternate 4 000 kg. How
long can the aircraft legally hold overhead destination at FL 250, before it has to divert to
alternate?
First determine how much of the 23 500 kg the aircraft has to keep in tanks to satisfy the
Law.
Now determine how much fuel is available for the hold overhead destination.
If 8 480 kg is available for the hold, then ½ of this plus the weight at the end of the hold will
give the holding MZW.
The function of a simplified flight plan is the same as that of a full flight plan, albeit
abbreviated.
The climb plus all the cruise sectors plus the descent, are all found on one graph.
The diversion to alternate is found on the same graph as the full flight plan.
The holding fuel need not be calculated because it is an assumed standard for
simplified flight planning i.e. 30 MINS and 4 400 kg.
If the holding fuel need not be calculated and the alternate time and fuel are calculated in the
same way as per the full flight plan, there is only one question that can be asked:
Determine the trip time and fuel for a particular flight.
Graphs 3-5-1 and 3-5-1(a) are for a M0.84 cruise at a constant flight level.
Graph 3-5-2 is for a 350 Kts IAS short distance cruise.
Graphs 3-5-3 and 3-5-3(a) are for LRC at a constant flight level.
Graph 3-5-4 is for a cruise with a step climb to optimum altitude.
EXAMPLE:
Trip distance 3500 nm. Mean W/C for the trip -50 Kts. Brake release weight 310 000 kg.
Mean temperature deviation for the trip ISA + 10°C. Determine the trip fuel and time for a
step climb to optimum altitude, graph 3-5-4.
EXAMPLE:
Trip distance 3500 nm. Mean W/C for the trip -50 Kts. Brake release weight 310 000 kg.
Mean temperature deviation for the trip ISA + 10°C. M0.84. FL 310. Determine the trip fuel
and time using graph 3-5-1(a).
Part of the graph requires the landing weight (at destination),a catch 22 situation because the
landing weight is dependant on the trip fuel which we are trying to determine. This is the
solution:
Now:
TAS 500 KTS - W/C 50 KTS = G/S 450 KTS
DISTANCE 3 500 NM G/S 450 KTS = TIME 7 HRS 47 MINS
7 HRS 47 MINS F/F 12 000 KG/HR = 93 333 KG TRIP FUEL
TOW 315 000 KG - 93 333 KG = 221 667 KG LANDING WEIGHT
Use this weight on the graph to determine the trip fuel and time.
- Trip fuel = 90 000kg
- Trip time = 8hrs
The same procedure would apply for a LRC and a 350 KTS IAS cruise.
METHOD
On the flight from A - B - C, with alternate at D, the following fuel must be carried.
A - B - C Burn-off
A-B-C 4%
Approach fuel (1100 kg)
C - D Burn off
C-D 4%
30 minutes holding fuel
Taxi fuel (600 kg)
Minimum in tanks (1600 kg)
On this flight the fuel requirement is so great that the payload would be significantly limited,
perhaps to the extent of the flight being unprofitable. The alternative would be to carry less
fuel and to make and en-route stop for refuelling.
On the flight from A - B - E, with alternate F, the following fuel must be carried :
A - B - E Burn-off
A-B-E 4%
Approach fuel (1100 kg)
E - F Burn-off
E-F 4%
30 minutes holding fuel
Taxi fuel (600 kg) Minimum in tanks (1600 Kg)
Calculate flight A - B - C in the normal fashion, except : eliminate the 4 % fuel from A-B.
Eliminating the 4 % fuel for leg A - B means that more payload can be carried.
If the flight now reaches point B, the re-despatch point, and the fuel remaining in the tanks
indicates that only the B/O has been used (as in fact should be the case), the flight may
legally continue to point C with not only B/O, but also 4 % in the tanks.
If, however, the flight reaches point B, and the fuel remaining in the tanks indicates that the
aircraft has used more than just the B/O (perhaps due to inaccurate forecast winds), it will
have to set course for point E and again, not only have B/O, but also 4 % in the tanks.
Should it occur that the fuel for flight A - B - C - D, even with a portion of the 4 % contingency
eliminated, is greater than the fuel for the flight A - B - E - F, this amount of fuel must
obviously be carried out would be carried on flight plan A - B - E - F as extra fuel.
FLIGHT PLANNING
1. TOW 312 000 kg. Departure airport elevation 5 558ft. ISA + 12°C. Calculate the fuel
required to climb to FL 330.
2. TOW 307 600 kg. Departure airport elevation 3 700ft. ISA + 8°C. Calculate the fuel
required to climb to FL 310.
3. TOW 296 000 kg. Departure airport elevation 2 777ft. ISA + 4C. Climb track 340T.
Wind 270/70. What is the ground distance to TOC FL 330?
4. Aircraft weight 287 500 kg. ISA + 14C. Sector distance 521 nm. Track 328T. Wind
270/70. Calculate the fuel required for this sector at FL 310 and M0.84.
5. Sector distance 612 nm. LRC. FL 310 climbing to FL 350. Track 272T. Wind
300/40. Aircraft weight at the beginning of the sector 271 100 kg. ISA + 10°C.
Calculate the fuel required for this sector.
6. FL 310. ISA + 12°C. Track 250T. Wind 230/60. M0.84. Sector distance 447 nm.
Aircraft weight at the beginning of this sector 313 370 kg. What is the fuel flow on this
sector?
7. FL 330. ISA + 12°C. Track 115°T. Wind 250/55. Sector distance 405 nm. Weight
at the beginning of this sector 310 070 kg. What is the fuel required for this sector?
8. FL 310. ISA + 13°C. Track 275°T. Wind 210/40. LRC. Sector distance 284 nm.
Weight at the beginning of the sector 336 050 kg. What is the fuel flow for this sector.
9. Descend from FL 350. Track 260°T. Wind 205/35. What is the total ground distance
to descend at speeds MO.84/320/250?
10. Distance to alternate 270 nm. Track 280°T. VAR 11°W. TOW 345 000 kg.
Trip fuel 91 470 kg to destination. What is the correct FL to alternate at ISA + 15°C?
11. Distance to alternate 180 nm. Track 140°T. VAR 5°E. TOW 335 000 kg.
Trip fuel 76 130 kg to destination. What is the correct FL to alternate at ISA + 15°C?
13. Distance to alternate 410 nm. W/C + 28 Kts. TOW 351 000 kg. Trip fuel 85 250 kg.
Calculate the fuel and time to alternate.
14. TOW 345 000 kg. Trip fuel 91 470 kg. Fuel to alternate 8 300 kg. Calculate the fuel
required to hold for 30 mins. at FL 150.
15. ZFW 226 470 kg. Calculate the fuel required to hold at alternate at FL 200 for 30
mins.
16. An aircraft arrives overhead destination at FL 200 with 19 700 kg fuel in tanks. The
scheduled fuel to alternate is 7 200 kg, the contingency fuel is 288 kg and the fuel to
hold at alternate is 4 000 kg. How long can the aircraft safely hold at this level if the
ZFW is
218 000 kg?
17. An aircraft arrives overhead destination at FL 140 with 21 700 kg fuel in tanks. The
scheduled fuel to alternate is 6 000 kg, the contingency is 240 kg and the fuel to hold
at alternate is 4 400 kg. How long can the aircraft safely hold at this level if the ZFW
is
221 400 kg?
SIMPLIFIED PLANNING
1. Trip distance 3 200 nm. Average W/C for trip -25 Kts. TOW 315 000 kg average
upper level temperatures ISA + 10 with reference to Simplified Flight Planning Graph
3-5-4 “Step Climb to Optimum Altitude”, what is the trip fuel and time?
2. Trip distance 3 700 nm. Average W/C + 30 Kts. Constant FL 330. TOW 316 000
kg. Mean temperature deviation ISA + 15°C LRC. With reference to Simplified Flight
Planning Graph 3-5-3(a), calculate the fuel required.
3. Trip distance 4 000 nm. Average W/C - 45 Kts. Constant FL 310. TOW 325 000 kg.
M0.85. With reference to Simplified Flight Planning Graph 3-5-1(a), calculate the
trip fuel.
4. Distance from destination to alternate 375 nm. Mean W/C + 25 Kts. TOW 305 000
kg. Trip fuel 92 000 kg. Calculate the fuel to alternate with reference to graph 3-5-5.
GRAPHS
If an actual take-off weight is given, it will automatically do away with the necessity to write
down the above three conditions.
Enter the take-off speeds table (Page 1-7) with this weight and extract V1, VR, V2.
CASE 1 : If the speeds lie in the shaded area this means that the V1 speed may be
affected by Vmcg.
a) Enter the speeds table with the field length limited take-off weight.
b) If the speeds are out of the shaded area use the speeds determined in
step 2 - the take-off is legal.
c) If the speeds still fall in the shaded area, the take-off is not legal.
CASE 2 : If the problem states that either the anti-skid is inoperative or two brakes
are de-activated:
c) Enter the speeds table with the lowest of these three weights to extract
VR and V2.
d) Enter the speeds table with the field length limited take-off weight
BEFORE REDUCTION to extract V1.
1) Wind.
2) Slope.
3) Step vi (a) reduction.
f) The correct V1 will be the lower of this V1 and the V1 for the actual
TOW (corrected for slope and wind) as per para. A (ii). Always cross-
check to ensure that the chosen V1 is above Vmcg.
IN CLASS EXAMPLES
2. Determine V1, Vr & V2 for a take off under the following conditions:
TOM 377 842KG FLAP 20 PH 4600FT COAT +25C
RWY 11 800FT NIL WIND NIL SLOPE PACKS ON
2 BRAKES U/S
The integrated range tables (B747 manual, pages 3-3-1 to 3-3-15) are used to calculate a
simplified figure for the anticipated fuel burn-off for a particular trip distance.
SPECIAL NOTES
i) There are integrated range tables for LONG RANGE CRUISE at various flight
levels, and integrated range tables for MACH 0.84 cruise at various flight
levels.
ii) The fuel figures derived from these tables excludes climb and descent fuel,
thus in their pure form would be used in the event of a dog-leg or unplanned
routing.
iii) The tables are valid for ISA conditions. If conditions deviate from ISA, there
are adjustments for fuel required and TAS below the tables.
iv) The tables are valid for still air conditions. If there is a prevailing wind, the fuel
required will have to be adjusted.
IN CLASS EXAMPLES
iii) Against 2771 in the table, read 230 000 Kg (left) and 4000 kg (top).
iv) The weight at the end of the trip is thus 234 000 kg.
vi) No fuel adjustment is required due to ISA conditions and still air prevailing.
QUESTIONS
TAKE OFF GRAPHS
1. TOW 345 000 kg, flaps 20, PA 3000ft, temperature + 27°C, headwind 15 Kts. 1 %
uphill slope. Determine the take-off speeds.
2. TOW 270 000 kg, flaps 10, PA 2800ft, temperature + 27°C, field length 9000ft, wind
calm, nil slope. Determine whether the take-off is legal and if so, what are the take-
off speeds?
4. TOW 304 000 kg, runway 05 elevation 3762 ft, runway 23 elevation 3562 ft. Runway
05 headwind 14 Kts, runway length 10 000 ft, flaps 10°, PA 4000 ft, temperature +
30° C, anti-skid inoperative. Determine the take-off speeds.
5. Determine the take-off speeds at MTOW, Runway length 9000 ft, slope 1 % up, wind
calm, flaps 20°, 2 brakes de-activated, PA 5000 ft, temperature + 35° C.
1. Mach 0.84 cruise, FL330, trip distance 3624 nm, weight at the commencement of the
trip 341 000 Kg. What is the fuel required?
2. Mach 0.84 cruise FL330, trip distance 3624 nm, weight at the commencement of the
trip 341 000 Kg, ISA + 15°C. What is the fuel required?
3. Mach 0.84 cruise, FL330, trip distance 3624 nm, weight at the commencement of the
trip 341 000 kg, average wind component for the trip -50 Kts. What is the fuel
required?
4. Mach 0.84 cruise, FL330, Trip distance 3624 nm, weight at the commencement of the
trip 341 000 kg, average wind component for the trip -50 Kts, ISA + 15°C. What is the
fuel required?
5. Trip distance 4170 nm. Weight at beginning of the trip 316 000 kg, WC - 40 Kts,
temperature ISA + 14° C. M0.84 cruise FL 280. Determine the trip fuel in kg.
6. Trip distance 3099 nm. Weight at beginning of the trip 281 500 kg, WC + 35 Kts,
temperature ISA + 8° C, M0.84, FL 290. Determine the trip fuel in kg.
7. Trip distance 3200 nm. Weight at the beginning of the trip 297 000 kg W/C - 22 Kts.
Temperature ISA + 13C. LRC. FL 310. Determine the trip fuel in kg.
8. Trip distance 1200 nm. Weight at the beginning of the trip 331 500 kg. LRC. FL
310. ISA + 12. W/C + 55 Kts. Determine the trip fuel in kg.
When considering the subject of weight and balance, it is important to understand that there
are two very distinct matters under consideration:
CENTRE OF GRAVITY (C of G)
The centre of gravity is defined as that point on the aircraft through which the
total weight may be considered to act.
Centre of Gravity
REFERENCE POINT/DATUM
In order to express the position of the centre of gravity accurately, it is necessary to have a
reference point. This reference point is called the datum line. The choice of datum line
position varies from aircraft to aircraft and is of arbitrary importance only.
Once a datum line has been chosen, the location of the C of G can be accurately expressed;
e.g. 300ft aft of datum. 300 ft aft of datum
DATUM
Clearly, if weight is added to the aircraft, for example, in the nose section, the C of G must
move forward to keep the aircraft in balance.
Arm
Certainly, with large aircraft, the moments calculated are cumbersome and difficult to work
with.
To solve this, a suitable reduction factor (RF) can be chosen and divided into the moment to
make it more workable. For example a RF of 10 000 could be used. When a moment is
divided by a RF, it becomes known as an index.
The chord line is the line joining the leading and trailing edges of an aerofoil. On aerofoils
with taper and/or sweepback, a mean or average aerodynamic chord can be calculated.
LEMAC is then the leading edge of this mean aerodynamic chord.
1. Shortly before take-off, an extra passenger is given permission to board the aircraft.
Before boarding, the weight of the aircraft was 11 200 Lbs and the C of G at
191inches aft. The passenger weighs 170 Lbs and is allocated a seat at FS 259.
What is the new C of G?
2. An aircraft has a MAC of 162 inches LEMAC is at FS 324. The C of G is 412 inches
aft of datum. What is the C of G position expressed as % MAC?
3. From the following data, calculate the position of the C of G in inches aft of datum and
as a percentage MAC.
OEW : 66 600 kg
C of G : 480inches
ZONE A FS 290 LOAD 28 STANDARD PASSENGERS
ZONE B FS 480 LOAD 42 STANDARD PASSENGERS
ZONE C FS 680 LOAD 46 STANDARD PASSENGERS
HOLD 1 FS 200 LOAD 1500 kg
HOLD 4 FS 750 LOAD 500 kg
WING TANK FS 490 LOAD 41 020 kg
CENTRE TANK FS 480 LOAD 9080 kg
4. Aircraft weight 10 400 lbs. C of G 100". What is the furthermost aft FS that freight
weighing 500 lbs can be loaded without exceeding the rearmost C of G limit of 120"?
6. Before take-off, the aircraft weighs 11 000 lbs and the C of G is 191" aft of the datum.
Where does the C of G lie after take-off when the undercarriage is retracted? The
main wheels weigh 380 lbs. When extended they are at FS 85 and when retracted
they are at FS 91. The nosewheel has a negligible effect.
All of the previously mentioned principles for the PET also hold true for the CP. For CP
calculations, a reduced (one engine inoperative) TAS will be given.
i) Use this reduced TAS to determine a reduced GSO and a reduced GSH.
Use this GSO and GSH in the CP formula to determine the distance to the
CP.
ii) Use the full TAS to determine a full GSO. Divide the distance to the CP by
the full GSO to determine the time to the CP.
THE CP FORMULA
CP DIST =
Multi Leg CP
2.Find the CP
1. A - B track 084° (T) distance 607 nm, W/V 210/15, TAS 240 Kts, reduced TAS 180
kts.
Solve:
2. A - B track 145° (T), distance 860 nm, W/V A - CP 060/20, CP - B 120/30, TAS 240
kts, reduced TAS 180 kts.
Solve:
3. A - B track 316° (T), distance 1040 nm, W/V 090/30, TAS 240 Kts, reduced TAS 180
kts, fuel flow 1500 Lbs/Hr. Fuel flow with one engine inoperative 1250 Lbs/Hr. The
aircraft experiences an engine failure at the CP and elects to return to departure due
to better maintenance facilities. What was the fuel used on return at A?.
4. A - B distance 1072 nm, track 210° (T), TAS 490 Kts, reduced TAS 460 kts, W/V A -
CP 020/47, W/V CP - B 065/65. What is the distance and time to the CP?
5. Distance A - B 3140 nm, track 137° (T), W.V. 040/52, full TAS 480 kts, full F/F 9750
kg/hr. Reduced TAS 460 kts, reduced F/F 8240 kg/hr. If the aircraft experiences an
engine failure at the CP and elects to continue to destination, what will the fuel burn
off be on arrival at B?
If the aircraft reaches the CP, and then returns, what will the fuel on board be on
arrival at A?
With still air conditions prevailing, the PNR will be at the half-way mark in terms of safe
endurance time.
A B
To determine the distance to the PNR, multiply the time out with the speed out;
Where there is a prevailing wind, the PNR will move into wind in terms of time. To fly
a given distance will take a longer time flying into a headwind and a shorter time
flying with a tailwind. The sum of the two times will equal the safe endurance.
A B
To determine the distance to the PNR, multiply the time out with the speed out;
PNR TIME =
The second formula for the PNR and the second formula for the PET are closely linked
PET (DIST) =
therefore
AND ALSO:
PNR TIME =
therefore
1. A - B 941 nm
Track 084° (T)
TAS 240 kts
W/V 160/25
Safe endurance 6 hrs 16 mins
3. A-B
Distance 762 nm
Track 040° (T)
W/V 090/20
B-C
Distance 502 nm
Track 090° (T)
W/V 210/10
C-D
Distance 801 nm
Track 135° (T)
W/V 120/25
FAJS - KMV
Distance 240 nm
Track 248° (T)
W/V 180/20
KMV - FACT
Distance 390 nm
Track 240° (T)
W/V 270/30
KMV - FABL
Distance 80 nm
Track 125° (T)
W/V 180/20
5. On a flight from A - B, the safe endurance equals the flight time plus 25 %. Track
075° (T), W/V 220/45, TAS 470 kts distance 4875 nm. What is the time and distance
from the PET to the PNR?
SAMPLE EXAM
a) 8 800 kg;
b) 7 940 kg;
c) 8 300 kg. (4)
2. Cruise at FL 350. Temperature ISA +15ºC. Long Range Cruise. Track 086º T.
Wind Velocity 310/40. Leg distance 378 nms. The aircraft weight at the
commencement of the leg is 308 600 kg. What is the fuel required?
a) 8 485 kg;
b) 7 940 kg;
c) 9 060 kg. (4)
3. Cruise at FL 290. Temperature ISA +12ºC. MACH 0.84. Track 186º T. Wind
velocity 270/40. leg distance 512 nms. the weight at the commencement of the leg
is 316 200 kg. What is the fuel flow on this leg?
a) 12 060 kg/hr;
b) 12 530 kg/hr;
c) 12 980 kg/hr. (4)
4. Take off weight 361 250 kg. Trip fuel A-B 98 700 kg. In the event of a go-around,
what will the flight level to alternate be, if the alternate distance is 386 nms and the
magnetic track to alternate 268º M, ISA +15ºC?
a) FL 350;
b) FL 310;
c) FL 390. (3)
5. Integrated range. FL 350. MACH 0.84. Trip distance 3600 nms. The weight at
the commencement of the trip 316 500 kg. The wind component of the trip is + 25
KTS. Temperature ISA +12ºC. What is the trip fuel?
a) 61 778 kg;
b) 63 842 kg;
c) 64 920 kg.
6. Determine the VI speed at the maximum take-off weight. Runway length 11 000ft.
Nil slope. Wind component – 10 KTS. Temperature +20ºC. Pressure altitude 5
500ft. Two brakes are de-activated. Flap 20.
a) 144 KTS;
b) 150 KTS;
c) 136 KTS. (4)
a) 10 100 kg;
b) 11 400 kg;
c) 10 900 kg. (3)
8. Determine the maximum landing weight with anti-skid operative. Field length 8 500ft.
Two brakes inoperative. Dry runway. Pressure altitude 5 500ft. Headwind 5 KTS.
Flap 30
The TAS throughout the flight is 512 KTS. Determine the distance to the PET.
a) 783 nms;
b) 821 nms;
c) 880 nms. (4)
10. The wind velocity from A to the CP is 260/26. The wind velocity from the CP to B is
210/40. TAS 260 KTS. Reduced TAS 210 KTS. The track from A to B is 170º T.
The distance from A to B is 962 nms. Determine the distance to the CP.
a) 600 nms;
b) 491 nms;
c) 518. (3)
The wind component at FL 310 which gives the same performance of GNM/1 000 kg
as for FL 370 with a 60 KTS headwind is:
a) 19 KTS;
b) 27 KTS;
c) 38 KTS. (4)
TAS A – E is 260 KTS. Safe endurance excluding reserves is 8 HRS 45 MIN. If the
aircraft departed from A at 0900Z, the ETA for the PNR is:
a) 1405 Z;
b) 1417 Z;
c) 1429 Z. (4)
13. Basic operating empty weight 105 500 lbs. Standard passenger weight 170 lbs. C
of G 880”. Mac 180.9”. Lemac 860.5”. The loading details are as follows:
a) 22.56%
b) 24.79%
c) 26.82% (4)
14. Aircraft mass 298 500 kg. FL 330. Mach 0.84 cruise. Temperature ISA +5ºC.
Headwind 65 KTS. Sector distance 855 nms. According to the integrated range
tables, the sector fuel required is:
a) 19 000 kg;
b) 20 500 kg;
c) 21 600 kg. (3)
15. Airport pressure altitude 3 000ft Temperature 34ºC. Slope 1% uphill. 15 KTS
headwind. Runway length 9 000ft. Flap 20. PAX on. What is the maximum take-
off weight?
16. Airport pressure altitude 5 000ft. Flap 30. Wet runway. Two brakes inoperative.
Anti-skid operative. Runway length 8 800ft. Headwind 10 KTS. According to the
Landing Performance Graph (5-3) the maximum landing weight?
a) 90 000 kg;
b) 94 500 kg;
c) 99 000 kg. (3)
18. Take-off with anti-skid inoperative. TOW 327 000 kg. Pressure altitude 5 500ft.
Temperature +25ºC. Runway length 12 000ft. Slope 1% downhill. Runway
headwind component 15 KTS. Packs off. Flap 10.
a) 123
b) 130
c) 136 (4)
19. Departure elevation 3 500ft. Estimated take-off mass 347 200 kg. With reference to
the B747 climb tables, the fuel required to climb for FL 330 with a temperature of ISA
+12 is:
a) 9 200 kg;
b) 9 670 kg;
c) 8 650 kg.
TOW 343 000 kg. ZFW 233 700. Trip fuel 90 140 kg. Contingency fuel 3 605 kg.
Holding fuel 30 mins. Approach fuel 1 100 kg. Minimum in tanks 1 600 kg.
Distance Kilo to Lima 350 nms. Wind component + 21 KTS.
According to the B747 Alternate Planning Graph, 3-5-5, the fuel required from Kilo to
Lima is:
a) 7 900 kg;
b) 8 600 kg;
c) 9 300 kg. (3)
21. A B747 arrives overhead its alternate airport after diverting, at a mass of 247 450 kg.
According to table 4-3, the fuel required for a 30 minute hold at FL 150 with flap up is:
a) 4 405 kg;
b) 4 445 kg;
c) 4 485 kg. (3)
a) 12 230 kg;
b) 12 680 kg;
c) 13 130 kg. (4)
If the aircraft arrives overhead Hotel with 19 500kg of fuel in tanks, it could hold at FL
150 before diverting to India with reserves intact for:
a) 24 mins.;
b) 29 mins.;
c) 34 mins. (4)
24. On a flight from Cape Town on a track of 347ºT, an aircraft performs as follows:
The distance from Cape Town beyond which the aircraft will be unable to return to
Cape Town is:
a) 1534 nm;
b) 1439 nm;
c) 1485 nm. (4)
25. The following figures relate to an aircraft’s performance at various flight levels:
a) FL 250;
b) FL 270;
c) FL 280. (3)
27. Floor load limit 173 LBS / sq. ft. pallet mass 79 LBS. tie downs mass 35 LBS.
Pallet dimensions 70ft X 70”. What is the maximum cargo that can be carried on this
pallet.
a) 5772 lbs.;
b) 5807 lbs.;
c) 5886 lbs. (3)
28. Aircraft mass 4800 LBS. C of G 82”. AFT C of G limit 85”. The maximum mass
that could be carried at station 155 without exceeding the AFT C of G limit is:
a) 227.3 LBS;
b) 214.9 LBS;
c) 205.9 LBS. (4)
a) 2000ft;
b) 2350ft;
c) 2650ft. (2)
30. Aerodrome elevation 2480ft. QNH 1018.7. Runway 01 slope 1.2% up. Surface
wind 060/15. Temperature + 33ºC. Flap 20. At a break release weight of 353 250
kg, the minimum runway length required for take-off is;
a) 11 200 FT;
b) 12 300 FT;
c) 14 000 FT. (3)
31. Aircraft weight 352 500 kg, FL 290. M0.84. Cruise temperature ISA + 15ºC.
Tailwind 55 KTS. Sector distance 1500 nm. According to the integrated range
tables, the sector fuel is:
a) 35 200 kg;
b) 36 500 kg;
c) 38 000 kg. (4)
33. From XRAY to WHISKEY 3906 NMS. Mean W/C –25 KTS . Mean temperature
deviation + 12ºC. Take-off mass 368 800 kg. The trip time and fuel according to
simplified flight planning “Step Climb to Optimum Altitude’ (3-5-4) is:
a) 146 KTS;
b) 149 KTS;
c) 153 KTS. (3)
35. Departure aerodrome elevation 4 250 ft. Estimated take-off mass 336 500 kg. With
reference to B747 Climb Tables, the fuel required to climb to FL 350, ISA +8ºC is:
a) 8 530 kg;
b) 8 950 kg;
c) 9 440 kg. (4)
36. A flight plan is to be prepared from JNB to Athens with Brindisi as the alternative
airport. According to the B747 Alternative Planning Graph (3-5-5), the fuel required
from Athens to Brindisi is:
Take-off mass 341 000 kg. ZFW 223 500 kg. Trip fuel 98 110 kg. Contingency
fuel 4% 3925 kg. Holding fuel 30 mins. Approach fuel 1100 kg. Minimum in tanks
1600 kg. Distance Athens to Brindisi 315 NMS. W/C –35 KTS.
a) 10 600 kg;
b) 9 950 kg;
c) 9 300 kg. (4)
37. A B747 has arrived over its alternate after a diversion. Mass 238 300 kg. According
to the B747 manual page 4-3, the fuel required for 30 minutes holding at FL 150 with
flaps up is:
a) 4 338 kg;
b) 4 392 kg;
c) 4 439 kg.
a) 12 330 kg;
b) 12 780 kg;
c) 13 230 kg. (4)
39. The following figures relate to a B747 flight from JULIET to KILO with LIMA as the
alternate airport.
ZFW 233 700 kg.
Fuel to alternate 12 500 kg.
4 % contingency (ALT) 500 kg.
30 mins holding at alternate 4315 kg.
Approach 1100 kg
Minimum in tanks 1600 kg.
If the aircraft arrives overhead KILO 26 000 kg of fuel remaining, it could hold
overhead Kilo at FL 150 before diverting to LIMA with reserves intact for:
a) 26 mins;
b) 32 mins;
c) 38 mins. (4)
40. A B747 is flying at FL 330. Long range cruise. ISA +10. Aircraft mass 277 500 kg,
time 1315 Z. The time at which the aircraft mass has reduced to that at which FL
370 is the optimum altitude is:
a) 1514 Z;
b) 1519 Z;
c) 1524 Z. (4)
ANSWERS
V x SG = W
44 Imp Gal x 7.5 = 330 lbs
AREA = pr²
= p x 0.28 m x 0.28 m
= 0.2463 m²
Calculate the maximum weight that the floor can sustain on an area this size.
W = A x FL
= 0.2463 m² x
= 172.4 Kg and the weight of the drum is only 169.7 Kg, therefore it can be
carried.
LSS =
= 592 kts
LSS = 38.945
592 = 38.945
15.2 =
15.2² = ºC + 273
231 = ºC + 273
ºC = 231 - 273
ºC = - 42ºC
5. Convert elevation to PA
= 5502.5 ft
Convert PA to DA
At 5502.5 ft, the ISA temperature should be + 4ºC. The temperature is + 4ºC. It is
therefore 20ºC too hot.
7. You may not plan on landing before A displaced threshold or use the stopway at the
other end, therefore:
The two contingencies are not burn off and some of it may be left behind. Which
one? The first one - 1 067 kg.
Therefore: Grand total fuel 52 425 kg - 1 067 kg = 51 358 kg
Put this equation to the acid test. Imagine a CAA inspector at A and also at B.
Inspector A knows your route, contingency and approach, therefore, he wants to see
28 374 kg in tanks. You have 51 358 kg - he’s happy.
Before return to A, CAA inspector B, who knows your route, contingency and
approach wants to see 23 691 kg in tanks - you have exactly that.
1.
a)
b)
2.
a)
3.
a)
b) The wind component is the difference between the TAS and the G/S
= 210 - 170.6
= -39.4 Kts (Headwind)
a) FL160
b) FL180
ii) FL180
iii) FL190
Despite the strong W/C, FL190 is the best level to cruise at.
(b) With a total of 7400 LBS on board and a fuel flow of 1300 LBS/HR, with 1
HR reserve required, the available trip fuel is 6100 LBS.
6100 LBS ¸
= 4.69 HRS
4.69 HRS x
= 1004 NM RANGE
In order to complete the flight, the aircraft must use a maximum of 5920 LBS over the
800 nm.
Clearly the maximum TAS lies between 220 Kts and 240 Kts. Use interpolation to
determine the exact TAS.
Endurance 70 000 Kg ´
= 2800 nm
= 56 kts H/W
= 0.0462 GNM/KG
At FL 350
= 87 kts H/W
10. If there is no wind at FL 290, then 94.8 ANM/1000 kg is also 94.8 GNM/1000 kg.
This represents the bottom line performance at FL 350 - What headwind would
make it so?
The average TAS is no problem because it is a constant 492 KTS throughout the
flight. The average FF is a problem though, because the two fuel trip fuel flows were
far for varying amounts of time. To solve this problem, calculate total fuel burn
total time =
average FF
A-B
506 NM 480 KTS = 1.054 HRS
1.054 HRS 12 200 KG/HR = 12 861 KG
B-C
481 NM 474 KTS = 1.015 HRS
1.015 HRS 12 800 KG/HR = 12 989 KG
A-C
1.054 HRS + 1.015 HRS = 2.069 HRS
12861 KG + 12 989 KG = 25 820 KG
25 850 KG
= 12 494 KG / HR
2,069 HRS
= 39.38 ANM/1000 KG
FLIGHT PLANNING
7 600 kg + 80 kg = 7 680 kg
5 558' - 4 000'
850 kg - 550 kg = 234 kg
6 000' - 4 000'
5 558' - 4 000'
900 kg - 600 kg = 234 kg
6 000' - 4 000'
444 Kts
ISA + 4 C - ISA + 0 C
17,6 MINS - 16,6 MINS = 0,4 MINS
ISA + 10 C - ISA + 0 C
ISA + 4 C - ISA + 0 C
444 Kts - 435,6 Kts = 3,36 Kts
ISA + 10 C - ISA + 0 C
58 KTS - 50 KTS
47 KTS - 38 KTS = 7,2 KTS
60 KTS - 50 KTS
AT ISA + 10°C
TAS = 503 Kts
AT ISA + 15°C
TAS 509 Kts
NOW: TAS 507.8 Kts - W/C 39.8 Kts = 468 Kts G/S
At this weight the TAS, W/C, G/S and TIME do not change.
ISA + 10°C
ISA + 15C
ISA + 14°C
At this weight the TAS, W/C, G/S and TIME do not change.
ISA + 10°C
ISA + 15°C
ISA + 14°C
16. Calculate the amount of fuel that must remain in the tanks.
SIMPLIFIED PLANNING
1. Fuel 75 000 kg
Time 8 hrs
2. This graph requires a landing weight - use standard TAS, 500 Kts and standard
F/F 12 000 kg/hr.
FUEL = 79 000 KG
3. This graph requires a landing weight - use standard TAS, 500 Kts and standard
F/F 12 000 kg/hr.
FUEL = 8 700 KG
Chapter 4
V1 = 149.5 Kts
VR = 159 Kts
V2 = 169.5 Kts
Slope : + 1 Kt
Wind : + 1 Kt
V1 = 151.5 Kts
VR = 159 Kts
V2 = 169.5 Kts
V1 = 131 Kts
VR = 135 Kts
V2 = 155 Kts
The speeds fall in the shaded area which means that they may be affected by Vmcg.
Calculate the field length limited take-off weight : 312 000 Kg.
Apply 312 000 Kg to the speeds table. 312 000 Kg lies out of the shaded area, in other
words, the take-off is legal and the speeds for the take-off are those indicated above.
Where aircraft weight and ambient conditions give a V1 speed below Vmcg, this V1 speed is
increased to be above Vmcg and then shaded. Therefore, the shaded speeds on the table
are not below Vmcg. The shading indicates that these speeds have been subjected to an
increment to place them above Vmcg.
The lowest of these three will be the actual take-off weight. Enter the speeds table with 356
000 Kg.
V1 = 153 Kts
VR = 163 Kts
V2 = 173 Kts
Slope : + 1 Kt
Wind : + 1 Kt
V1 = 155 Kts
VR = 163 Kts
V2 = 173 Kts
Enter the 2 brakes de-activated table. Extract a weight reduction and a V1 reduction.
Enter the speeds table with 354200 Kg and extract only VR and V2.
VR = 163 Kts
V2 = 172 Kts
Enter the speeds table with the field length limited take-off weight before reduction to
extract V1. Enter the speeds table with 356000 Kg.
V1 = 153 Kts.
+ 1 wind
+ 1 slope
V1 - 150 Kts
VR - 163 Kts
V2 - 172 Kts
Subtract 9100 Kg
Subtract 21 kts
V1 = 150 kts
+ 1 Wind
- 4 slope
- 21 anti-skid inoperative
128
V1 = 126 Kts (Vmcg is 122 kts)
But the V1 for the actual TOW of 304000 kg (corrected for slope and wind) is 120 Kts,
which is lower than 126 Kts, therefore the correct V1 is 120kts but Vmcg = 122, take off
illegal.
Subtract 2300 Kg
Subtract 6 kts
VR = 137 kts
V2 = 147 kts
V1 = 129 kts
+ 1 slope
- 6 brakes
V1 = 124 kts (Vmca is 117.5 kts)
take off illegal.
INTEGRATED RANGE
1. 341,000 Kg = 7783 nm
7782 nm - 3624 nm = 4158 nm
4158 nm = 258 280 Kg (interpolated)
341 000 Kg - 258 280 Kg = 82 720 Kg
This amount of fuel must be increased, due to the non-standard temperature, at the rate of
0.9 % per 10°C above ISA. (0.09 % per 1°C Above ISA).
From the top of the table read TAS 488 Kts - 50 Kts W/C = 438 Kts G/S.
3624 nm ¸ 438 Kts = 8 hrs 16 mins. This time multiplied by the TAS will give the air
distance flown.
341,000 Kg = 7782 nm
7782 nm - 4038 nm = 3744 nm
3744 nm = 249 900 Kg
341 000 Kg = 249 900 Kg = 91 100 Kg
First do a very rough calculation to determine an average TAS for the flight.
331 500 Kg = 500 Kts + 12 Kts ISA Dev + 55 Kts W/C = 567 Kts G/S.
1200 GNM 567 Kts G/S = 2.12 Hrs
2.12 Hrs 512 Kts TAS = 1 084 ANM
Halfway between 500 Kts and 494 Kts is 497 Kts Rough TAS.
CHAPTER 5
W x A = M
2.
412" = 324" = 88"
483 - 447 =
= 25 % MAC
5. Although the C of G of the aircraft is not given, an arbitrary one may be chosen,
because it is only the change of C of G that is required
W ´ A = M
12200 ´ 100 = 1220000
- 170 259 = 44030
+ 170 315 = 53550
12200 100.7 = 1229520
6. W ´ A = M
11000 191 = 2101000
- 380 85 = 32300
+ 380 91 = 34580
11000 191.2 = 2103280
a) CP distance =
= 289 nm from A
b)
2.
Determine the GSR and GSO. Note the different winds for each.
CP DIST =
The aircraft flew from A to the CP at 260 Kts with a fuel flow of 1500 Lbs/Hr.
= 2655 Lbs
The aircraft then flew from the CP back to A at 158 Kts with a fuel flow of 1250 Lbs/Hr
= 3639 Lbs
4. CP =
414
= 1072 nm
512 + 414
= 479 nm from A
Time to the CP
479 nm ¸ full GSO for leg A - CP
479 ¸ 536 Kts
= 54 mins
CP =
= 1549 nm from A to CP
TIME A - CP
= 1549 nm ¸ 484
= 3 Hrs 12 x 9750 Kg/Hr
= 31212 Kg
TIME CP - B
6.
Assume the CP is at B
380 nm - 75 nm = 305 nm
GSR
CP = 305 nm
GSO + GSR
405 KTS
= 305 KTS
455 KTS + 405 KTS
= 144 nm
PNR TIME =
= 748 nm
The units for the formula are Kg/Gnm, thus both expressions of performance will have
to be inverted.
PNR DISTANCE =
=
= 1397.5 Nm
Does the PNR lie at point B? If so, the sum of times A - B and B - A will equal the
safe endurance.
A-B B-A
= =
A - B + B - A = 6 Hrs 22 Mins
This is less than the safe endurance; therefore the PNR must lie beyond point B.
Does the PNR lie at point C? If so, the sum of the times A - B - C and C - B - A will
equal the safe endurance.
A-B C-B
3 Hrs 21 mins =
= 2 Hrs 08 Mins
B-C B-A
= 3 Hrs 01 Mins
= 2 Hrs 03 Mins
A - B -C + C - B - A
= 10 Hrs 33 Mins
This is more than the safe endurance; therefore the PNR must lie between points B
and C.
This 1 Hr 38 Mins must take the aircraft from B - PNR and the PNR - B
A-B B - PNR
3 Hr 21 Mins 0 Hr 48 Mins = 4 Hrs 09 Mins
A-B B - PNR
0 Hrs 48 Mins x 245 Kts
762 + 196 nm = 958 nm
4. Make a schematic diagram and solve the GSR and GSO for each leg.
Does the PNR lie at KMV? If so, the sum of the times FAJS - KMV - FABL will equal
the safe endurance. (Note that the aircraft does not return to FAJS).
= 1 Hr 02 Mins = 21 Mins
= 1 Hr 23 Mins
This is less than the safe endurance time; therefore the PNR must lie on leg KMV -
FACT.
= 2 Hrs 46 Mins
PNR TIME =
= 1 Hr 32 Mins
1 Hr 32 x 214
SE = 9:38 hrs + 25 %
= 12 hrs 03mins
Therefore, the time to go beyond the PET to the PNR and back is 2 hrs 25 mins.
PNR =
432
= 2 hrs 25
506 + 432
= 563 nm
= 9792 Kg
PNR DIST =
= 1643 NM
S.E. LBS
PNR (DIST) = LBS LBS
GNM OUT + GNM PET
149 189 LBS
=
44,42 LBS / GNM OUT + 40,29 LBS / GNM RETURN
= 1 761 NM to point X
1 C 21 C
2 A 22 B
3 B 23 A
4 A 24 B
5 B 25 A
6 A 26 A
7 B 27 A
8 A 28 C
9 B 29 B
10 C 30 B
11 A 31 A
12 A 32 B
13 B 33 C
14 C 34 A
15 B 35 B
16 B 36 C
17 B 37 A
18 C 38 A
19 A 39 C
20 C 40 C