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Archive / FAA Pilot’s Handbook of Aeronautical Knowledge / Pilot’s Handbook: Chapter 16 — Navigation

Chapter 16, Part 2

Navigation — Part 2

FAA-H-8083-25C (2023)

Figure 16-11. Magnetized portions of the airplane cause the

compass to deviate from its normal indications.

N33

30

W

24

21

S 15

12

E

6

3

N33

30

W

24

21

S 15

12

E

6

3

N33

30

W

24

21

S 15

12

E

6

3

Magnetic North

Magnetic North Magnetic North

Magnetized engine

Figure 16-12. Compass deviation card.

For (Magnetic)

Steer (Compass)

For (Magnetic

Steer (Compass)

E

86

W

274

60

57

240

243

N

0

S

180

30

28

210

212

120

117

300

303

150

148

330

332

Remember, if variation is west, add; if east, subtract. One

method for remembering whether to add or subtract variation

is the phrase “east is least (subtract) and west is best (add).”

Deviation

Determining the magnetic heading is an intermediate step

necessary to obtain the correct compass heading for the flight.

To determine compass heading, a correction for deviation

must be made. Because of magnetic influences within an

aircraft, such as electrical circuits, radio, lights, tools, engine,

and magnetized metal parts, the compass needle is frequently

deflected from its normal reading. This deflection is called

deviation. The deviation is different for each aircraft, and

it also may vary for different headings in the same aircraft.

For instance, if magnetism in the engine attracts the north

end of the compass, there would be no effect when the plane

is on a heading of MN. On easterly or westerly headings,

however, the compass indications would be in error, as shown

in Figure 16-11. Magnetic attraction can come from many

other parts of the aircraft; the assumption of attraction in the

engine is merely used for the purpose of illustration.

Some adjustment of the compass, referred to as compensation,

can be made to reduce this error, but the remaining correction

must be applied by the pilot.

Proper compensation of the compass is best performed by

a competent technician. Since the magnetic forces within

the aircraft change because of landing shocks, vibration,

mechanical work, or changes in equipment, the pilot should

occasionally have the deviation of the compass checked. The

procedure used to check the deviation is called “swinging the

compass” and is briefly outlined as follows.

The aircraft is placed on a magnetic compass rose, the engine

started, and electrical devices normally used (such as radio)

are turned on. Tailwheel-type aircraft should be jacked up into

flying position. The aircraft is aligned with MN indicated on

the compass rose and the reading shown on the compass is

recorded on a deviation card. The aircraft is then aligned at

30° intervals and each reading is recorded. If the aircraft is to

be flown at night, the lights are turned on and any significant

changes in the readings are noted. If so, additional entries

are made for use at night. The accuracy of the compass can

also be checked by comparing the compass reading with the

known runway headings.

A deviation card, similar to Figure 16-12, is mounted near

the compass showing the addition or subtraction required to

correct for deviation on various headings, usually at intervals

of 30°. For intermediate readings, the pilot should be able to

interpolate mentally with sufficient accuracy. For example,

if the pilot needed the correction for 195° and noted the

correction for 180° to be 0° and for 210° to be +2°, it could

be assumed that the correction for 195° would be +1°. The

magnetic heading, when corrected for deviation, is known

as compass heading.

Effect of Wind

The preceding discussion explained how to measure a TC

on the aeronautical chart and how to make corrections for

variation and deviation, but one important factor has not

been considered—wind. As discussed in the study of the

atmosphere, wind is a mass of air moving over the surface of

the Earth in a definite direction. When the wind is blowing

from the north at 25 knots, it simply means that air is moving

southward over the Earth’s surface at the rate of 25 NM in

1 hour.

Under these conditions, any inert object free from contact

with the Earth is carried 25 NM southward in 1 hour. This

effect becomes apparent when such things as clouds, dust,

and toy balloons are observed being blown along by the wind.

Obviously, an aircraft flying within the moving mass of air

is similarly affected. Even though the aircraft does not float

freely with the wind, it moves through the air at the same

time the air is moving over the ground, and thus is affected

by wind. Consequently, at the end of 1 hour of flight, the

aircraft is in a position that results from a combination of

the following two motions:

Figure 16-13. Motion of the air affects the speed with which aircraft

move over the Earth’s surface. Airspeed, the rate at which an

aircraft moves through the air, is not affected by air motion.

090°

Groundspeed 120 knots

WINDS ARE CALM

090°

Groundspeed 140 knots

WINDS 270° AT 20 KNOTS

090°

Groundspeed 100 knots

WINDS 090° AT 20 KNOTS

• Movement of the air mass in reference to the ground

• Forward movement of the aircraft through the air mass

Actually, these two motions are independent. It makes no

difference whether the mass of air through which the aircraft

is flying is moving or is stationary. A pilot flying in a 70-

knot gale would be totally unaware of any wind (except for

possible turbulence) unless the ground were observed. In

reference to the ground, however, the aircraft would appear

to fly faster with a tailwind or slower with a headwind, or to

drift right or left with a crosswind.

As shown in Figure 16-13, an aircraft flying eastward at

an airspeed of 120 knots in still air has a groundspeed (GS)

exactly the same—120 knots. If the mass of air is moving

eastward at 20 knots, the airspeed of the aircraft is not

affected, but the progress of the aircraft over the ground is

120 plus 20 or a GS of 140 knots. On the other hand, if the

mass of air is moving westward at 20 knots, the airspeed of

the aircraft remains the same, but GS becomes 120 minus

20 or 100 knots.

Assuming no correction is made for wind effect, if an aircraft

is heading eastward at 120 knots and the air mass moving

southward at 20 knots, the aircraft at the end of 1 hour is

almost 120 miles east of its point of departure because of its

progress through the air. It is 20 miles south because of the

motion of the air. Under these circumstances, the airspeed

remains 120 knots, but the GS is determined by combining

the movement of the aircraft with that of the air mass. GS can

be measured as the distance from the point of departure to

the position of the aircraft at the end of 1 hour. The GS can

be computed by the time required to fly between two points a

known distance apart. It also can be determined before flight

by constructing a wind triangle, which is explained later in

this chapter. [Figure 16-14]

The direction in which the aircraft is pointing as it flies is

called heading. Its actual path over the ground, which is a

combination of the motion of the aircraft and the motion of

the air, is called track. The angle between the heading and

the track is called drift angle. If the aircraft heading coincides

with the TC and the wind is blowing from the left, the track

does not coincide with the TC. The wind causes the aircraft

to drift to the right, so the track falls to the right of the desired

course or TC. [Figure 16-15]

The following method is used by many pilots to determine

compass heading: after the TC is measured, and wind

correction applied resulting in a TH, the sequence TH ±

variation (V) = magnetic heading (MH) ± deviation (D)

= compass heading (CH) is followed to arrive at compass

heading. [Figure 16-16]

By determining the amount of drift, the pilot can counteract

the effect of the wind and make the track of the aircraft

coincide with the desired course. If the mass of air is moving

across the course from the left, the aircraft drifts to the

right, and a correction must be made by heading the aircraft

sufficiently to the left to offset this drift. In other words, if

the wind is from the left, the correction is made by pointing

the aircraft to the left a certain number of degrees, therefore

correcting for wind drift. This is the wind correction angle

(WCA) and is expressed in terms of degrees right or left of

the TC. [Figure 16-17]

Figure 16-15. Effects of wind drift on maintaining desired course.

Heading

Wind

Track

Drift angle

Desired course

Figure 16-16. Relationship between true, magnetic, and compass

headings for a particular instance.

Heading

TN MN CN

TH-088°

MH-078°

CH-074°

VAR 10° E

DEV 4°

Figure 16-14. Aircraft flight path resulting from its airspeed and direction and the wind speed and direction.

Airspeed effect (1 hour)

20 knots

Distance covered over ground (1 hour)

To summarize:

• Course—intended path of an aircraft over the ground

or the direction of a line drawn on a chart representing

the intended aircraft path, expressed as the angle

measured from a specific reference datum clockwise

from 0° through 360° to the line.

• Heading—direction in which the nose of the aircraft

points during flight.

• Track—actual path made over the ground in flight. (If

proper correction has been made for the wind, track

and course are identical.)

• Drift angle—angle between heading and track.

• WCA—correction applied to the course to establish

a heading so that track coincides with course.

• Airspeed—rate of the aircraft’s progress through

the air.

• GS—rate of the aircraft’s inflight progress over

the ground.

Figure 16-17. Establishing a wind correction angle that counteracts wind drift and maintains the desired course.

Heading

Wind

Track

Wind

correction

angle

Desired course

090°

075°

Basic Calculations

Before a cross-country flight, a pilot should make common

calculations for time, speed, and distance, and the amount

of fuel required.

Converting Minutes to Equivalent Hours

Frequently, it is necessary to convert minutes into equivalent

hours when solving speed, time, and distance problems. To

convert minutes to hours, divide by 60 (60 minutes = 1 hour).

Thus, 30 minutes is 30/60 = 0.5 hour. To convert hours to

minutes, multiply by 60. Thus, 0.75 hour equals 0.75 × 60

= 45 minutes.

Time T = D/GS

To find the time (T) in flight, divide the distance (D) by the

GS. The time to fly 210 NM at a GS of 140 knots is 210 ÷

140 or 1.5 hours. (The 0.5 hour multiplied by 60 minutes

equals 30 minutes.) Answer: 1:30.

Distance D = GS X T

To find the distance flown in a given time, multiply GS by

time. The distance flown in 1 hour 45 minutes at a GS of 120

knots is 120 × 1.75 or 210 NM.

GS GS = D/T

To find the GS, divide the distance flown by the time

required. If an aircraft flies 270 NM in 3 hours, the GS is

270 ÷ 3 = 90 knots.

Converting Knots to Miles Per Hour

Another conversion is that of changing knots to miles per hour

(mph). The aviation industry is using knots more frequently

than mph, but is important to understand the conversion for

those that use mph when working with speed problems. The

NWS reports both surface winds and winds aloft in knots.

However, airspeed indicators in some aircraft are calibrated

in mph (although many are now calibrated in both mph and

knots). Pilots, therefore, should learn to convert wind speeds

that are reported in knots to mph.

A knot is 1 nautical mile per hour (NMPH). Because there are

6,076.1 feet in 1 NM and 5,280 feet in 1 SM, the conversion

factor is 1.15. To convert knots to mph, multiply speed in

knots by 1.15. For example: a wind speed of 20 knots is

equivalent to 23 mph.

Most flight computers or electronic calculators have a

means of making this conversion. Another quick method of

conversion is to use the scales of NM and SM at the bottom

of aeronautical charts.

Fuel Consumption

To ensure that sufficient fuel is available for your intended

flight, you must be able to accurately compute aircraft fuel

consumption during preflight planning. Typically, fuel

consumption in gasoline-fueled aircraft is measured in

gallons per hour. Since turbine engines consume much more

fuel than reciprocating engines, turbine-powered aircraft

require much more fuel, and thus much larger fuel tanks.

When determining these large fuel quantities, using a volume

measurement such as gallons presents a problem because

the volume of fuel varies greatly in relation to temperature.

In contrast, density (weight) is less affected by temperature

and therefore, provides a more uniform and repeatable

measurement. For this reason, jet fuel is generally quantified

by its density and volume.

This standard industry convention yields a pounds-of-fuel-

per-hour value which, when divided into the nautical miles

(NM) per hour of travel (TAS ± winds) value, results in a

specific range value. The typical label for specific range is

NM per pound of fuel, or often NM per 1,000 pounds of fuel.

Preflight planning should be supported by proper monitoring

of past fuel consumption as well as use of specified fuel

management and mixture adjustment procedures in flight.

For simple aircraft with reciprocating engines, the Aircraft

Flight Manual/Pilot’s Operating Handbook (AFM/POH)

supplied by the aircraft manufacturer provides gallons-per-

hour values to assist with preflight planning.

When planning a flight, you must determine how much

fuel is needed to reach your destination by calculating the

distance the aircraft can travel (with winds considered) at

a known rate of fuel consumption (gal/hr or lbs/hr) for the

expected groundspeed (GS) and ensure this amount, plus an

adequate reserve, is available on board. GS determines the

time the flight will take. The amount of fuel needed for a

given flight can be calculated by multiplying the estimated

flight time by the rate of consumption. For example, a flight

of 400 NM at 100 knots GS takes 4 hours to complete. If an

aircraft consumes 5 gallons of fuel per hour, the total fuel

consumption is 20 gallons (4 hours times 5 gallons). In this

example, there is no wind; therefore, true airspeed (TAS)

is also 100 knots, the same as GS. Since the rate of fuel

consumption remains relatively constant at a given TAS,

you must use GS to calculate fuel consumption when wind

is present. Specific range (NM/lb or NM/gal) is also useful

in calculating fuel consumption when wind is a factor.

You should always plan to be on the surface before any of

the following occur:

• Your flight time exceeds the amount of flight time

you calculated for the consumption of your preflight

fuel amount

• Your fuel gauge indicates low fuel level

The rate of fuel consumption depends on many factors:

condition of the engine, propeller/rotor pitch, propeller/

rotor revolutions per minute (rpm), richness of the mixture,

and the percentage of horsepower used for flight at cruising

speed. The pilot should know the approximate consumption

rate from cruise performance charts or from experience.

In addition to the amount of fuel required for the flight,

there should be sufficient fuel for reserve. When estimating

consumption you must plan for cruise flight as well as startup

and taxi, and higher fuel burn during climb. Remember that

ground speed during climb is less than during cruise flight

at the same airspeed. Additional fuel for adequate reserve

should also be added as a safety measure.

Flight Computers

Up to this point, only mathematical formulas have been used

to determine such items as time, distance, speed, and fuel

consumption. In reality, most pilots use a mechanical flight

computer called an E6B or electronic flight calculator. These

devices can compute numerous problems associated with

flight planning and navigation. The mechanical or electronic

computer has an instruction book that probably includes

sample problems so the pilot can become familiar with its

functions and operation. [Figure 16-18]

Plotter

Another aid in flight planning is a plotter, which is a protractor

and ruler. The pilot can use this when determining TC and

measuring distance. Most plotters have a ruler that measures

in both NM and SM and has a scale for a sectional chart on one

side and a world aeronautical chart on the other. [Figure 16-18]

Pilotage

Pilotage is navigation by reference to landmarks or

checkpoints. It is a method of navigation that can be used

on any course that has adequate checkpoints, but it is more

commonly used in conjunction with dead reckoning and

VFR radio navigation.

The checkpoints selected should be prominent features

common to the area of the flight. Choose checkpoints that can

be readily identified by other features, such as roads, rivers,

railroad tracks, lakes, and power lines. If possible, select

features that make useful boundaries or brackets on each

side of the course, such as highways, rivers, railroads, and

mountains. A pilot can keep from drifting too far off course

by referring to and not crossing the selected brackets. Never

place complete reliance on any single checkpoint. Choose

ample checkpoints. If one is missed, look for the next one while

maintaining the heading. When determining position from

checkpoints, remember that the scale of a sectional chart is 1

inch = 8 SM or 6.86 NM. For example, if a checkpoint selected

was approximately one-half inch from the course line on the

chart, it is 4 SM or 3.43 NM from the course on the ground.

In the more congested areas, some of the smaller features are

not included on the chart. If confused, hold the heading. If a

turn is made away from the heading, it is easy to become lost.

Roads shown on the chart are primarily the well-traveled

roads or those most apparent when viewed from the air.

New roads and structures are constantly being built and

may not be shown on the chart until the next chart is issued.

Some structures, such as antennas, may be difficult to see.

Sometimes TV antennas are grouped together in an area near

a town. They are supported by almost invisible guy wires.

Never approach an area of antennas less than 500 feet above

the tallest one. Most of the taller structures are marked with

strobe lights to make them more visible to pilots. However,

some weather conditions or background lighting may make

them difficult to see. Aeronautical charts display the best

information available at the time of printing, but a pilot should

be cautious for new structures or changes that have occurred

since the chart was printed.

INSTRUCTIONS FOR USE

1. Place hole over intersection of true course and true north line.

2. Without changing position rotate plotter until edge is over true course line.

3. From hole follow true north line to curved scale with arrow pointing in direction of flight.

4. Read true course in degrees, on proper scale, over true north line. read scales counter-clockwise.

SECTIONAL CHART SIDE - 1:500,000 NAVIGATIONAL FLIGHT PLOTTER

0

180

270

90

10

190

280

100

20

200

290

110

30

210

330

150

340

160

350

170

300

120

310

130

320

140

330

150

340

160

350 170

190 10

200

20

210

30

220

40 230

50 240

60

250

70

260

80

NAUTICAL 5 MILES 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 NAUTICAL 85 MILES

0 STATUTE 5 MILES 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 9585 100 90

DEGREES

Mode ClrOn/Off

Dist Vol Wt Wx ÷

: 7 8 9 x

Sto 4 5 6 −

Rcl 1 2 3 +

Bksp 0 . +/- =

C

M

P

TSD Alt: As Wind Wt. Bal Timer

Conv: Dist Vol Wt Wx

A Plotter

B Mechanical flight computer

C Electronic flight computer

Figure 16-18. A plotter (A), the computational and wind side of a mechanical flight computer (E6B) (B), and an electronic flight computer (C).

Dead Reckoning

Dead reckoning is navigation solely by means of computations

based on time, airspeed, distance, and direction. The products

derived from these variables, when adjusted by wind speed

and velocity, are heading and GS. The predicted heading

takes the aircraft along the intended path and the GS

establishes the time to arrive at each checkpoint and the

destination. Except for flights over water, dead reckoning

is usually used with pilotage for cross-country flying. The

heading and GS, as calculated, is constantly monitored and

corrected by pilotage as observed from checkpoints.

Wind Triangle or Vector Analysis

If there is no wind, the aircraft’s ground track is the same as

the heading and the GS is the same as the true airspeed. This

condition rarely exists. A wind triangle, the pilot’s version

of vector analysis, is the basis of dead reckoning.

The wind triangle is a graphic explanation of the effect of

wind upon flight. GS, heading, and time for any flight can be

determined by using the wind triangle. It can be applied to

the simplest kind of cross-country flight, as well as the most

complicated instrument flight. The experienced pilot becomes

Heading and airspeed

Course and groundspeed

N33

3

0

W

24

21

S 15

1

2

E

6

3

P

W

E

Wind direction and velocity

N

S

Figure 16-20. The wind triangle as is drawn in navigation practice.

080° heading and 120 knots airspeed

090° course and 110 knots groundspeed

N33

30

W

24

21

S 15

12

E

6

3

Wind at 20°

direction and

35 knots velocity

N

S

10° Drift Angle

8° left correction

Figure 16-19. Principle of the wind triangle.

so familiar with the fundamental principles that estimates can

be made that are adequate for visual flight without actually

drawing the diagrams. The beginning student, however, needs

to develop skill in constructing these diagrams as an aid to the

complete understanding of wind effect. Either consciously or

unconsciously, every good pilot thinks of the flight in terms

of wind triangle.

If flight is to be made on a course to the east, with a wind

blowing from the northeast, the aircraft must be headed

somewhat to the north of east to counteract drift. This can

be represented by a diagram as shown in Figure 16-19. Each

line represents direction and speed. The long blue and white

hashed line shows the direction the aircraft is heading, and

its length represents the distance traveled at the indicated

airspeed for 1 hour. The short blue arrow at the right shows

the wind direction, and its length represents the wind velocity

for 1 hour. The solid yellow line shows the direction of the

track or the path of the aircraft as measured over the earth, and

its length represents the distance traveled in 1 hour or the GS.

In actual practice, the triangle illustrated in Figure 16-19 is

not drawn; instead, construct a similar triangle as shown by

the blue, yellow, and black lines in Figure 16-20, which is

explained in the following example.

Suppose a flight is to be flown from E to P. Draw a line on

the aeronautical chart connecting these two points; measure

its direction with a protractor, or plotter, in reference to a

meridian. This is the TC, which in this example is assumed

to be 090° (east). From the NWS, it is learned that the wind

at the altitude of the intended flight is 40 knots from the

northeast (045°). Since the NWS reports the wind speed in

knots, if the true airspeed of the aircraft is 120 knots, there is

no need to convert speeds from knots to mph or vice versa.

Now, on a plain sheet of paper draw a vertical line representing

north to south. (The various steps are shown in Figure 16-21.)

Step 1

Place the protractor with the base resting on the vertical line

and the curved edge facing east. At the center point of the

base, make a dot labeled “E” (point of departure) and at the

curved edge, make a dot at 90° (indicating the direction of the

true course) and another at 45° (indicating wind direction).

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