NASA
: /k
¸
Technical
Memorandum
4271
.
u_
:i: i ¸
Lighting Lunar
Constraints Surface
Operations
i:
Dean Lyndon
B. Eppler B. Johnson
Houston,
Texas
i:_ _
_!ili:_
NASA National Aeronautics and Space Administration Office of Management Scientific Information
1991 : i•
•
and
Technical Division
Space
on
Center
CONTENTS
Section
Page
ABSTRACT
............................................................................................................................
INTRODUCTION STUDY THE
.................................................................................................................
ASSUMPTIONS
EFFECT
CALCULATION CASTING WORLD
TERMS
DURING APPLICATION CONCLUSIONS
ON
LUNAR
SURFACE
OF ILLUMINATION
ILLUMINATION
IN
EARTHSHINE
BY FULL
VALUES
IN
3
......................
EARTHSHINE
........
LUNAR
TO DAY
OF RESULTS
LUNAR
SURFACE
OPERATIONAL
SCHEDULES
..............................
.................................................................................................................... .....................................................................................................
........................................................................................................................
,°°
111
PRE'CED_NG
PAGE BLANK
4
6
OPERATIONS
.......................................................................................... TO
3
REAL
................................................................................................................
ACKNOWLEDGMENTS REFERENCES
OF
CONSTRAINTS THE
GEOMETRY
2
...................................................................................
OF VALUE
EARTHSHINE
LIGHTING
SYSTEM
ILLUMINATION
OBSERVATIONS
1
.....................................................................................................
OF EARTH-MOON
EARTHSHINE CREW
1
NOT
FILMED
8 8 9 10 11
TABLES i_ !!_ii_i Table ,:i,
Page
_
EARTHSHINE IN THE
'ii _i_
ili I
2
ILLUMINATION
APOLLO
VARIATIONS LOCATION
PROGRAM
IN EARTHSHINE ON
THE
LUNAR
VALUES
ILLUMINATION SURFACE
ii_!i_i_!ii!i _i_ !i _
' • ii__I
iv
il _i__
USED
........................................................................
12
WITH
....................................................
12
FIGURES Page
Figure 1
Variations phase
in the angle
and
level lunar
2
Apollo
17 photograph
3
Apollo Mare
17 photograph Procellarum
4
Variation phase
5
6
in the angle
of Earthshine surface of the
illumination
location crater
as a function
of Earth
..........................................................
Schl_iter
in Earthshine
..........................
of Reiner _,, a bright swirl feature on ..............................................................................................
level
of Earthshine
for the sub-Earth
illumination
point
as a function
of Earth
................................................................
15
under
Analog
under
scale
drawing Earthshine
of the
degree
available
of illumination
at the
sub-Earth down-Sun
7
Apollo
16 photograph
taken
90 ° to the
8
Apollo
16 photograph
taken
directly
as figure Operational the lunar
down-Sun
16
available point
at the
........................
same
showing
the range
of lighting
17 18
location
7 ............................................................................................................ diagrams surface
the
................................
direction
14
14
Analog scale drawing of the degree of illumination available full Earthshine ....................................................................................................
minimum
13
conditions
.........................................................................................
19 on
a) At sub-Earth
point
b)
At a western
limb
location
............................................................................
21
c) At an eastern
limb
location
...........................................................................
22
V
20
iilii_ ...............................................................................
ABSTRACT
An
investigation
that
for most
lunar
night The
similar
to the States
of the
throughout
Variations angle. tion
the
the
period
caused
activities
on a July
evening
night,
with
after
sunset).
consequent
the
Apollo
around
the
lunar
only night
Because
Program noon
suggests
may
that
be difficult
artificial in the
will be
southern
captured
length
rotation
EVA
angle.
of Earth
activities
to lack
con-
and
a function
due
illumi-
approximately
shadow
be solely
of the
Earthshine
of the
remain
constant
indicates most
minor from
8:00 p.m.
will
will
surface
throughout
with
lunar
of the Earth
illumination
during
by elimination
the
at approximately
the location
of Earthshine
on the lunar
(EVAs)
during
15 minutes
the lunar
lighting
will be adequate
available
Earth,
in the level Experience
during
lighting
level
about
of ambient
illumination
(approximately
Moon
stant
levels
extravehicular
maximum light
the
locations,
to conduct
nation. United
into
nearside
phase
conducted
of surface
defini-
of shadows.
INTRODUCTION
During lunar the
the Apollo
surface
operations
nominal
Due
landing
to vehicle
executed
The plans
Apollo
limit
necessary
be faced
during
developing surface
the
planning
Can the Can
be required?
proposed
and
constraints
execution
and
lunar
of crew surface
robotic
operations
operations
away
to mission departure
and
from
the lunar
surface
or
lunar
operations
George
beyond
the
Bush,
72- to 96-
Consequently, day.
would
Considerations on the
conditions
These
it
that
conditions these
in lunar
will have
constraints
of an outpost
outpost/lander in SEI are
planned
the
constraints
lighting
the effect
operations.
the
into
surface
Moon.
the lunar
in the vicinity
development from
surface
of the
the
and
morning, landing.
were
day
in 1989 by President lunar
during
include
lunar
lighting.
for, the operational
day,
limited
after
missions
for lunar
night
habitation
conducted
early
lunar
place
on the
to plan
operations
the =-655-hour
concern
affect
not
or lander,
as well.
Issues
but
that
are
as follows.
be executed
at any
time
during
day?
geologic
reflected
(SEI),
permanent
for routine
arrival lunar
Initiative
to eventual
for science
of significant
ambient
operational
and
planning
using
times
between
--328-hour
took
constraints
24 to 96 hours
no Apollo
the
planning
safety
day from
module
to consider,
these
lunar
morning
beyond
for stay
surface
and
on consumables,
capability
throughout
on planning
lunar
design,
of the
lunar
no significant
our
becomes
late
extended
Exploration
to extend
hour
only
have
outside Space
and
constraints
would
Consequently,
conducted
operational,
to the portions time,
design
that
night.
Program,
field
off the
work
Earth
and
other
(Earthshine)
surface
activities
be carried
during
the lunar
night,
out
or will
using artificial
only
light
lighting
i
Are
_il'_
nation
on the
during any _i ii i _
lighting
Earthshine
to "real
the •
the
in various
value
of Earthshine
Finally,
existing
lunar
photos
under
with
were
conditions
tion
is that
ment
the
study
of EVA
be adequate cal power
generation
The
form
third
of integral
EVA suits, and This is because still
be very
some
form The
landing program, between
at a habitat
is that lighting,
and
final
assumption
at a previously
data
that
would
from might
safety
differing
Earth-Moon
first apon the orbit on
Sun angles.
The
illuminaillumination
to understand
how
the
geometries.
to determine Sun
be
on illumi-
be experi-
lines. The recollections
in varying
what
lighting
angle.
for this study. or cooling
generation
thermal
The
questions inside
second
will be adequate to what
lighting, of ambient
will be required illumination,
considerations
will
dictate
assump-
in its assess-
the EVA
for lunar
is currently
first
equipment
assumption
of the conclusions
similar
The
life support
environment
regardless
of vehicular of the value
normal
that
and
rejection
future
or lander
assumption
of auxiliary
information
on Earth,
as a baseline
environment.
EVA
helmet
surface
values for full-Earth value of Earthshine
scrutinized
heat that
thermal
some form regardless
dark,
consider
an appropriate
ambient
surface to interpret
ASSUMPTIONS
used
assuming
to maintain of the
were
will not
operations,
regardless tions.
!,
of assumptions
the
of illumi-
the engineering several and
surface
of varying
STUDY
A number
with
illumination
on the lunar
changes
surface
exist
was
on the lunar
to relate
illumination
illumination
might
on the lunar study
of the
search to find existing necessary to relate the
to full-Moon
amount
geography visible on the lunar surface from of illumination, and also to collect information
in working a literature this, it was
(1) the
part
the reader
necessary
during
(2) lighting available
to a comparable
topography and as the sole source
surface
constraints
providing
conducted
afternoon?
conditions:
and
of illumination
it was
sources
involved
lunar
basic
An important
values
operations
lunar
approach to this task has followed information from crew observations
second approach was tion. To complement on the
two
to Earthshine,
amount
world"
on Earth. The was to collect
constraints
due
surface
to early
considered
To do this,
amount of surface using Earthshine
to lunar
morning
illumination.
about
found
enced proach
i!¸
surface
if so desired.
nation
lunar
this study
lunar
conclusions
constraints
of late
high-Sun-angle
tested
ii_i
any
Sun angles
For simplicity,
!_ii_i_ i_ii_i! _',
!i_ ¸
there
high
will suit,
is that night
of this used
electri-
EVA
study, on Space
opera-
some Shuttle
for normal operations. shadowed areas will the requirement
for
lighting. is concerned unprepared
mission rules dictated that 5 and 20 ° above the horizon
with location
the
surface
on the
lunar
lighting surface.
required During
for a first the Apollo
all lunar landings would occur when the Sun was and behind the lunar module as it made its final
2
approach
to the
terrain information cant terrain feature.
i_ i _I
eyes
during
be in effect
tion
will
ii
site.
conditions
maneuvering
for future not
by orbital
apply
mechanics
It is further
pared landing pads once the appropriate
landings
_ ::
,i_ q:
Moon
and
assumed
EFFECT
vehicle that
-_28-day
interval
that
causes
the
design
manned
to most
around
landing
sites.
mission This
which
rules
assump-
will likely
rather
than
outposts
be
lighting
eliminating
will have this
GEOMETRY
pre-
requirement
ON
ILLUMINATION
rotation
of its orbital
people;
similar
considerations aids,
the maximum
that
surface,
SYSTEM
or captured,
period
with
down-Sun from any signifinot be in the astronauts'
or man-tended
OF EARTH-MOON
of its rotation
is familiar
the lunar
and navigational is developed.
is in synchronous,
that
crew
It is assumed
from
EARTHSHINE
The
the
at unprepared
to departure
with lighting infrastructure
THE
situation
provided
for landing.
manned
probably
constraints.
These
in the form of long shadows extending It also insured that the sunlight would
the final
will
dictated "
landing
rotation
its own
the same
axis.
hemisphere,
with
respect
around This
the
to the
Earth
geometry
usually
Earth,
to equal
produces
referred
a the
an effect
to as the
lunar
nearside, always faces the Earth, while the lunar farside always faces effects, caused by the wobbling of the Moon's axis during its rotation,
away. results
Libration in _-60
percent visibility of the lunar surface from the Earth only one-half of the Moon's surface is visible at any
period,
although
The synchronous illumination
shine
will remain in a constant addition,
rotation has several (fig. 1). To begin with,
in the same location lighting angle, and
shadow
length
effects at any
over a 12-month one time.
that pertain to the question point on the lunar nearside,
of Earththe Earth
throughout the _655-hour lunar day.1 This will result shadow length and location after lunar sunset. In
will increase
away
from
the
point
at which
the
Earth
is directly
overhead (hereafter referred to as the sub-Earth point) to a maximum at the poles and limbs, resulting in a higher proportion of the ground in shadow as one moves toward either the poles or limbs. Also, the lunar farside will receive no illumination from
iii_::i_i_ii _ ,i _
i_ •
•
Earthshine, which will result in the surface on the farside being extremely dark lunar sunset. Finally, as the phase of the Earth changes, the value of Earthshine
after illumi-
nation
dawn
the
reflect
the
sub-Earth
western
different
point,
limb
location
CREW
During lunar
orbit,
1 To avoid The
prefix
the
on the lunar
will be a phase
will have
an Earth
OBSERVATIONS
the
Apollo
and
flight
potential
"lunar"
locations Earth
will
Program, crews
confusion, be added
OF LUNAR
the to refer
able
terms
"day" day
SURFACE
Apollo
to observe
to both
For example,
9, of 90 °, while
at lunar
the
lunar
dawn
at at a
q_of 180 ° (fig. 1).
six separate
were
surface.
angle,
and and
3
missions
the lunar
"night" night
IN EARTHSHINE
will periods
spent surface
refer on
to the the
up
to 6 days
in
in a variety
of
terrestrial
and
lunar
surface.
day
night.
illumination conditions. Captain John W. Young was one of three astronauts to fly two lunar flights, the first was as the command module pilot on Apollo 10, and the second was as Commander of Apollo 16. Many of the observations that follow were made by Captain Young. In lunar orbit, it was possible to seeall the features on the lunar surface in Earthshine as easily as they were seenon the sunlit portion of the Moon. Transition across the terminator from the sunlit portion to the Earth!it portion was rapid, and there was no time required for the eye to adjust to the Earthshine to pick out details on the lunar surface (personal communication with Captain John W. Young, Special Assistant for Engineering, Operations and Safety,Lyndon B. JohnsonSpaceCenter, 1990). Gross color differences, particularly the transition between the mare and the highlands, were visible, as were shadows castby topographic features (fig. 2). High contrast features, such as bright-rayed craters or the bright swirl features on the maria like Reiner y, were also visible and could be photographed with high-speed film (fig. 3), although the photographic film carried by the Apollo crews was never capableof recording a scene with the sameveracity as the human eye. At times, it was even possible to seedetails within the shadows castby Earthshine. On the basis of these observations, it should be possible to make a lunar module landing to an unprepared site using only Earthshine for illumination (personal communication with Captain John W. Young). Further, making a landing to a prepared landing site, using a minimum complement of landing lights and navigational aids, would be even lessdifficult than making a vertical night landing in a helicopter on Earth (personal communication with Captain JohnW. Young). Transition from the Earthlit portion of the Moon into the unlit lunar farside was dramatic, and there was no senseof the gradual diminution in Earthshine illumination as the terminator was approached. It was extremely dark beyond the terminator, and no surface features could be seen. The horizon was distinguishable only by the lack of stars; otherwise, it was invisible.
CALCULATION OF VALUE OF ILLUMINATION BY FULL EARTHSHINE The value of full-Earth illumination canbe approximated using two techniques. Both of thesetechniques make use of the ratio of the albedos of the full Earth and the full Moon, and both are sensitive to the values chosenfor these albedos. The first technique approximates the ratio of full-Earth illumination to full-Moon illumination, assuming that the reflectance of eachbody canbe approximated by a flat plate of equal radius with the same albedo. The calculations are asfollows: •
Earth radius = 6371km
°
Lunar radius = 1738km
4
_i!:_ _i_I_I_ _ii! '_
_iil!iiiiii_ _ _!i!_iiI!i!i_ _
:_i! _ _i_,
L
•
Area
of flat
plate
with
6371
km radius
•
Area
of flat plate
with
1738 km
•
Area
ratio
•
Average
Earth
albedo
= 0.4
•
Average
lunar
albedo
= 0.07
•
Albedo
•
Relative
intensity
(Albedo
ratio
radius
= 127.5
x 106 km2
= 9.5 x 106 km2
_:_i_! _
i_ •
i
ii_i_ d! _
of both
ratio
flat
The
of full Earthshine
also
the
unit unit
Moon
which
is also
the
to the units
i,ii:i _ _iiiii_ _
equivalent
BEarth
= BMoon
•
BMoon
= 0.25 cd/cm2
•
BEarth
values
the
area
be -_76 times
albedo
ratios
calculation,
for respective
a 2-dimensional unit
with the first
should
unit
In each
of these
is equivalent
unit
value
This
of
calcula-
of brightness
(lumen/steradianl/centimeter2),
is, lumen/meter2
to
the
albedos.
as
back
changes,
to an
the value
of
to candela/centimeter2, The
conversion
is necessary
to units of illumination by accounting for the solid when seen from the Moon. These calculations are as
• (AlbedoEarth/AlbedoMoon)
= 1.43 cd/cm2
from
from
along
As with
to lumen/steradianl/centimeter2.
•
Conversion
chosen
= 76.49
on the Moon
can be used
(lumen/meter2). that
to change from units of brightness angle, 0, subtended by the Earth follows:
_i_.
Earthshine
to a solid-angle same;
Earth:Moon)
of the full Earth.
changing
for illumination stays
ratio
B, of the full
(candela/centimeter2) area
(Area full
is sensitive
involves
=
calculations, on Earth.
the illumination
the approximation tion
= 5.7
Earth:Moon)
brightness,
approximate
= 13.42
of Earth:Moon
On the basis of these bright as a full Moon
ii
plates
brightness,
(ref. 3) = 1.43 lm/sr/cm2
B; to illumination,
_ ii!
E; uses
the equation:
E = _ B sin2@ @ = 0.95 °
:!,
_i_ _ ,:!
E = 1.24 _i
_ ii
_
10-3 lm/cm2
= 12.4 lm/m2
•
i_
i_i_ i_!i_
.......
:
,:
_
"
::: _
,
This
value
shown i_ _ iii_ : 2!u _i_ _
i _
can be compared
in table
ment
and
gram
standards
Physical
Standards used
of any
experiments
either
on the
unmanned
this
_
nation
as reading.
ii::
value
remain
pro-
for future
for Earthshine
illumination,
8 or 10, which
preceded
or on Apollos the value
for full-Earth
calculated
the
illumination
from
above.
situations which from Earthshine.
allow an understanding of the magniThe first of these is the value of illumi-
(2).
It is possible,
IN REAL
on full,
above,
full Earthshine
WORLD
Moonlit
without amounts
illumination
TERMS
nights,
to operate
lights; and to generally of visual acuity, such
is _-76 times
suggesting that a significant amount of activity can without the need for additional artificial lighting.
take
as bright
place
under
as a
full
• i¸
Another ,_
likely
NASA
The document does not indivalues. At present, no record
to move around outside on foot lighting that do not require great
As calculated
full Moon, Earthshine
the
Environ-
VALUES
0.25 lm/m2
agricultural machinery; conduct tasks without
will
Program
Natural
ILLUMINATION
physical available
full Moon,
values
the
the value
Apollo
(1) representing
These
Program
the
TM X-68863,
of this paper. or measured
As can be seen,
EARTHSHINE
of the
Program
measure
with
during
in NASA
planning.
actually
favorably
There are several of illumination
Apollo
balance values
Surveyor
agrees
CASTING
tude
that
for planning
published
for the
of this document.
document
used
were
in the Apollo
exists
publication
iiii_,i__
to values
figures
programs and will be used for the cate whether these were calculated
!i:
_,
1. These
_i_ _,
Civil
comparison
twilight,
sunrise
but
brightest
in nautical after
lights,
is the
In aviation,
civil twilight an aircraft
lights,
interior
cockpit
shown
540 lm/m2
(3).
m2.
these
Using
phase
angle,
point
(fig. 4).
values,
the value and
This
shows
of the lunar
night
after
prior
that than
before
and half
illumination
the minimum
has
illumination
into
further
sunrise,
lights,
(or just
The
after
lunar-night greater
value The
sunset),
lighting
is
is 100 lm/
as a function
illumination
when
navigation
lighting.
illumination
values
or before
of full Earthshine.
interior
in Earthshine
dark,
or before
taxiway
that
navigation.
still see the
for position
to sunrise
full-Moon
full and
sunset,
in typical
Earthshine
aeronautical
horizon
the need
(3), or about
higher
and
or runway
the range
graphically
sunset time
of illumination
plotting
is significantly
portion
is the
sky, just
to depict
and
to see the
without
is 6.5 lm/m2
it is possible
after
lights,
by the terrestrial
Finally,
point
substantial
time
nautical
it is possible
operate
civil twilight
illumination
sub-Earth
terms, when
terrestrial
to safely
landing
for terrestrial
from
full dark,
stars.
it is possible
comes
of Earth at the
sub-Earth
illumination on Earth, than
at the and
that
terrestrial
civil twilight. i_' ii_ _:_!_
To put
these
illumination
values
real
World
values,
they
can be com-
pared to the illumination given off by a 60-W incandescent light bulb, which 840 lm of light. The distance, r, at which a 60-W bulb produces an illumination 13.5 lm/m2
can be calculated
using
the
following
• ii ¸ii_ •
6
equation:
generates of
a
13.5lm/m2 = 840lm/4
n r2
r=2.2m
This
means
hine
will be roughly
from
the
able
that working
outside
Using
the
surface
working surface.
in July same
lighting
for the
on the western
and
0 ° longitude. east will earlier.
The
have
will
--164 hours sunrise.
sunset,
and
eastern
limb,
with
a "new''
just prior
to that
at the
midnight,
then
difference horizon,
at polar and
latitude
equatorial
the
2 Midnight
At pole point:
decreasing
These
chosen
bulb
time.
elevated
adequate
to scale
of these
two
night
dark
phase
and
at 80 ° north
at lunar "new"
at sunset, of 2.8 lm/m2
covered
in shadow
of illumination
are detailed
in table
will not 2.
lunar sunset and sunrise.
7
''2
just before
profile
of will be
to 13.5 im/m2
will be very
will be greatly
of
illumination
at sunrise.
the Earth
will
"midnight,
Earth
increasing
and
the level
to a maximum
illumination
or
discussed
a full Earth
progresses,
gradually
the
latitude,
effects
minimum
increasing
will
>81.4 ° west
will be the opposite: locations,
angle
(1) locations
libration
will be from
illumination
them:
longitudes
of 2.8 lm/m2
to full
the
Earth
(2) a location
the level
between
point,
the
because
will be that
variations
refers to the midpoint
avail-
on the lunar
light
among
As the lunar
to a minimum
of ground
sub-Earth
to the lunar
at sunset
2.8 lm/m2
however,
Consequently,
and
sky due
reduced
at sunset,
sub-Earth
light standard
provide
illustration
because
to a level
the profile
Earth
amount
locations.
further
central
a 60-W should
investigated,
Earthshine
to sunrise.
locations,
sites.
were
in the
be reduced
the
13.5 lm/m2
were
of 13.5 lm/m2.
gradually
the
at 80 ° longitude,
Earth
location,
after On
will occur
lower
limb
from
will be different
cases
the
be at a maximum
illumination
lunar
limb
under
A schematic
away
cases
80°-longitude
For a western
similar
eastern
not always
constantly
night
end-member
to the natural impinging
conditions
full Earths-
is 2.2 m away
6.
nearside
the lunar
Several
to working
under
which
at =8:00 p.m.
of Earthshine,
of these
EVAs.
5 and
point
bulb
is similar
Texas
value
Both
of lunar
on the lunar
throughout
be different.
minimum
in figures
a 60-W
of illumination
of Houston,
surface.
conduction
at the sub-Earth under
_) of 90 °, is equivalent
is shown
At locations profile
the
the working
conditions
level
latitude
formula,
surface
to working
This
at the
at an Earth
4.9 m above
on the lunar
equivalent
at
One
significant
low
on the
increased be as useful
from as in
LIGHTING CONSTRAINTS TO LUNAR SURFACE OPERATIONS DURING THE LUNAR DAY Determination of slope on the lunar surface is primarily a function of two different sourcesof information. Within -_100m of a particular location, shadows castby positive features, such as rocks; and by negative features, such as craters,provide the most information on centimeter to meter-scalevariations in local topography. For topography located at greater distances from an observer,broad-scale topographic changesare discernible by variations in brightness. Assuming a uniform surface color, the closer a surface is oriented at right anglesto the direction of sunlight, the brighter it will be. An examination of panoramic photographs from Apollos 15, 16, and 17 indicates that as an observer gets closer to looking directly down-Sun, the amount of information available on local topography diminishes to virtually zero (figs. 7a and 7b). In particular, the problem appears to becomecritical within _-20° of directly down-Sun. This suggeststhat when the Sun is within 20° of the zenith, topography may be sufficiently subdued to make EVA operations on unfamiliar terrain difficult. The underlying assumption is that conditions near down-Sun under low-Sun-angle conditions can be extrapolated to high-Sun-angle conditions. A plot of Sun angle as a function of mission day (fig. 8) indicates that the Sun will be within 20° of vertical between _-130and 200 hours after lunar sunrise. The difficulty in distinguishing surface topography may require some restrictions in EVA surface operations during this time, such as operations only in familiar terrain, or operation of rovers only along known tracks that are marked. Similar operational restrictions are implemented in Antarctica during periods of reduced visibility. APPLICATION OF RESULTSTO OPERATIONAL SCHEDULES The results of this study have been used to develop a seriesof figures that graphically depict the lighting conditions throughout the lunar day, and possible lighting constraints to lunar surface operations (figs. 9a, 9b, and 9c). The figures were created with several conditions in mind. The first is that a minimum illumination of I lm/m2 will be necessaryfor safeEVA operations. This figure is chosen to follow conservative guidelines; 1 lm/m2 should full-Moon carry
is likely be pointed
to supply out,
illumination
out EVA
a sufficient
level
however,
that
lighting
on Earth,
should
of light
to carry
levels
as low
be sufficient
under
operations.
8
out
all EVA
as 0.25 lm/m2, emergency
activities.
It
equivalent conditions
to to
The second condition is that the mission rules requiring low Sun elevation with a backlit landing area, aswas used for the Apollo missions, will continue to be in force for the initial landings at previously unexplored locations, although the specific restrictions of from 5 to 20° Sun elevation may not be necessary. Lessrestrictive Sun angle conditions were suggested by discussions with Captain JohnW. Young. His observations during the lunar landing on Apollo 16indicate that terrain scaleis as important as terrain form, and that almost any degree of backlighting will be sufficient to highlight the terrain. What is lacking on the lunar surface, however, is an adequate referencefor scalemeasurement. The most useful information on the topographic scaleduring the Apollo landings became the shadow of the lunar module, which was out ahead of the landing point during the transition from powered descentto hovering flight. Using the width acrossthe landing legs of the lander, =10m, it was possible to gauge the scaleof the topography at the landing site, and determine whether the chosentouchdown point would be safe. On the basis of this experience,it appearsthat while the restriction to a particular range of Sun angles may not be necessary,backlighting will be extremely useful during future landing approachesto the lunar surface (personal communication with Captain John W. Young, 1990). The charts lay out the suggested times during which lighting conditions will be optimal for lunar EVAs in central equatorial regions in the vicinity of the sub-Earth point, in western limb locations, and in easternlimb locations. The diagram also shows the approximate phase of the Earth at sunset, sunrise, midnight, and the portion of the lunar night when the ambient lighting is
Figure
8. Apollo
16 photograph
figure 7. Notice the diminution shadows. NASA photograph
ki:
taken
directly
of topographic AS16-110-17952.