Thus, the White House announced on 27 March 1958 that it had approved a program "to determine our capability of exploring space in the vicinity of the moon and to obtain useful data concerning the moon". The program was announced by Defense Secretary Neil H McElroy. The Air Force Ballistic Missile Division in Los Angeles was assigned a program of three lunar probes using a "Thor-Vanguard" system with "a third stage to be developed". The Army Ballistic Missile Agency in Huntsville, Alabama was authorized to "undertake one and possibly two lunar probes" using modified Jupiter-C rockets. Overall responsibility for the lunar probe launches was assigned to the Defense Department's Advanced Research Projects Agency (ARPA).
The Air Force project had its roots in the "Able project" which was probably
designed to provide a rocket that could test re-entry vehicle (RV)
technology for the ICBM that had not yet been flown successfully. To achieve
the speeds necessary to test a reasonably sized RV the USAF and its contractor
the Space Technology Labs used a Thor IRBM with the second stage of the
Vanguard as the upper stage (see picture on the right of second stages
being prepared). This combination was test flown three times in 1958, the
first time less than a month after the White House announcement and the
last less than a month before the first lunar probe attempt. (Launch
dates for the Thor-Able 0 rocket are: 23 April, 9 July and 23 July 1958).
When NASA was formed in October of 1958, all military space research projects run by the military organisations were transferred to it. This included the four remaining flights in McElroy's (ARPA's) origonal plan and the follow-on space probes planned by the USAF. This plan included a plan to launch two probes (weighing 169 kg) to Venus in the launch window opening in June 1959 followed by a lunar orbit mission. However, after the Soviet success with Luna 1 the plans were changed to instead launch the follow-on provbes to lunar orbit in the hope of beating the Soviet Union to this goal. This follow-on Pioneer program used the Atlas-Able rocket and even before the first flight the goal of photographing the far side of the Moon was snatched by the Soviet union. Howevber, the first probe did carry a camera - it was too late to change the plans. howveer, the two following oprobes did not carry a camera, but instead more radiation monitoring instruments. However, the goal of achieving lunar orbit before the Soviet union could still be achieved.
The two tables below list the known launches in the first three U.S series of lunar probes. The first table gives technical details, while the second givesa dates and flight results as well as lunar coordinates.
Name |
by |
mass |
L/V | Instrumentation | Propulsion | Electr. power | RF System |
Pioneer-0 |
|
|
Thor-Able |
TV camera, |
Falcon motor for |
Batteries | 108.09 MHz, 50 W, TV 108.06 MHz, 0.3 W, TM 114.81375 MHz, TC |
Pioneer-1 |
|
|
Thor-Able |
" |
" |
" |
108.09 MHz, 50 W, TV |
Pioneer-2 |
|
|
Thor-Able |
" |
" |
" |
108.09 MHz, 50 W, TV |
Pioneer-3 |
|
|
Juno-2 | Radiation detectors |
- |
" | 960.05 MHz TM |
Pioneer-4 |
|
|
Juno-2 | Radiation detectors |
- |
" |
960.05 MHz TM |
P-3 |
|
Atlas-Able | TV camera, magnetometers, radiation detectors | 2 hydrazine engines. 66 cm tank in 1 m dia S/C. | 4 solar panels |
378.21 MHz TM 64 bps |
|
P-30 | Atlas-Able | No TV camera |
" |
" |
378.21 MHz TM 64 bps
401.85 MHz TC | ||
P-31 | Atlas-Able | No TV camera |
" |
" |
378.21 MHz TM 64 bps
401.85 MHz TC |
Name | Date |
(UT) |
at launch |
L/V | Notes |
arrival time |
at arrival |
Decl. at
arrival |
---|---|---|---|---|---|---|---|---|
Pioneer-0 | 17 Aug 1958 |
|
|
Thor-Able | Exploded at T+77 sec | 20 Aug 0218 UT |
|
-12.14 |
Pioneer-1 | 11 Oct 1958 |
|
|
Thor-Able | Too low speed. Hmax=110 000 km | 13 Oct 2300 UT |
|
-12.32 |
Pioneer-2 | 8 Nov 1958 |
|
|
Thor-Able | Third stage did not ignite | 10 Nov 2130 UT |
|
-13.85 |
Pioneer-3 | 6 Dec 1958 |
|
|
Juno-2 | Too low speed. Hmax=102 000 km | 7 Dec 1545 UT |
|
-11.32 |
Pioneer-4 | 3 Mar 1959 |
|
|
Juno-2 | Missed Moon with 60 000 km | 4 Mar 1511 UT |
|
-17.37 |
P-3 | 26 Nov 1959 |
|
|
Atlas-Able | Shroud splits at T+70 sec. | 28 Nov 2126 UT |
|
-13.05 |
P-30 | 25 Sep 1960 |
|
|
Atlas-Able | Second stage fails to ignite | 28 Sep 0513 UT |
|
-18.47 |
P-31 | 15 Dec 1960 |
|
|
Atlas-Able | Explodes shortly after launch. | 18 Dec 2240 UT |
|
-18.63 |
The values in the table below contain values from (2 ) converted to metric units.
Actual injection conditions for Pioneer-1 | ||
Flight phase | Parameter | Value |
Launch | Time | 0842:13 UT, 11 October 1958 |
Burnout | ||
Time | 0847:20 UT, 11 October 1958 | |
Altitude | 430.05 km | |
Latitude | 30.7° N | |
Longitude | 71.07° W | |
Velocity magnitude | 10.5230676 km/s | |
Velocity azimuth | 70.43° | |
Velocity angle from vertical | 64.74° | |
Apogee | Altitude | 113784 km |
Re-entry | Time from lifr-off | 43 hours 17.5 minutes |
Latitude | 21.0° S | |
Longitude | 88.1° W |
The velocity vector for Pioneer-1 was 5 degrees from the intended azimuth. Therefore the intended azimuth is set at 75.43 degrees. The speed at injection for the intended flight path is not so easy to determine exactly from (2 ). There are several values given as you can see from this table:
Various intended injection conditions for Pioneer-1 derived from (2) | |||
Speed given at | V = speed at injection | h = altitude at injection | Total energy (km2/s2) |
Page 4 | 35216 fps (10.73384 km/s) | 224 n.m (415.07 km) | -1.068813 |
Page 57 | 35400 fps (10.78992 km/s) | 200 st.m (321.8 km) | -1.282107 |
Page 83 | 35206 fps (10.73079 km/s) | 1410 k.ft (430.05 km) | -0.972437 |
Page 4=v (Page 76=h) |
35216 fps (10.73384 km/s) | 1410 k.ft (415.07 km) | -0.939725 |
By using the actual injection parameters the orbital elements and other characteristics of Pioneer-1 can be calculated (see table below) by using classical Keplerian mechanics (3). By using the last line in the table above the orbital elements and other characteristics of the intended trajectory of Pioneer-1 can be calculated in the same way. The reason for ignoring the velocity given on page 83 is that I think it is a misprint. The actual speed should be as given on page 4 - in my opinion. The apogee and period of the calculated orbit for the actual injection conditions match the data in (2 ) reasonably well. The apogee of the orbit resulting from the intended injection conditions also looks reasonable. The negative perigee is caused by the steep flight path angle at injection.
Computed orbital elements | ||
Orbital element etc.. |
Actual |
Planned |
Apogee (km) | 113477 |
412332 |
Perigee (km) | -874 |
-832 |
Inclination (°) | 35.79 |
33.56 |
RAAN (°) | 25.28 |
17.41 |
Argument of Perigee (°) | 7.90 |
15.88 |
Angle from node (°) | 60.3 |
66.8 |
True anomaly (°) | 53.15 |
51.27 |
Mean anomaly (°) | 1.2 |
0.2 |
Time from perigee (min) | 8.4 |
8.0 |
Time perigee-to-apogee (hrs) | 21.7 |
135.0 |
Period | 43 h 24 m | 11 d 6 h 5 m |
Declination of apse line (°) | -4.2 |
-8.54 |
Sun aspect angle at injection (°) | 52.3 |
51.5 |
p>
The map above comes from (2). The map below was generated by my own orbit analysis software SMX using the orbital elements derived from the actual injection condition. Time is shown at the same interval as in the map above. The radio horizon for the tracking station on the island of Hawaii is shown (yellow dot). The two graphs are reasonably similar.
The map below shows the ground track during the first 12 hours for the actual mission and the intended mission. The thicker track marks the part of the flight when the probe is above the horizon at Jodrell Bank (marked yellow). The other sites (Cape Canaveral, Singapore, Millstone Hill) are shown as green dots. One can clearly see the diffence in flight azimuth.
The two ground tracks quickly deviate from each other, but how soon was this evident as seem from the tracking station?The two graphs below show elevation and azimuth of the actual and intended mission as seen from Jodrell Bank. Clearly, by the time the probe rose above the horizon at Jodrell Bank the elevation angle was almost 5 degrees too low and it must have been obvious that the probe would not reach the Moon.
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One can compare the blue graphs with the figure below from (2). The agreement is reasonably good.
I have tried to compute the motion of the probe relative to the Moon in the case of disregarding the gravititaional effects of the Moon in order to try to see what a "patched-conic" analysis might bring. When the probe reached about 65000 km from the Moon about 55 hours after launch its speed relative velocity was 1.27 km/s and it possessed a total energy of 0,73 km2/s2 relative to the Moon. To obtain capture the spped would have to be reduced by 0.88 km/s. In (2) it is stated that the probe's retrorocket had a delta-v capability of 0.85 km/s - about the same! So, the computed trajectory is probably not so far from what was actually intended. One parameter that may be changed to obtain a more plausible trajectory is the injection azimuth. It could possibly be a little higher than the 75.4 degrees used in this analysis. Pioneer-2 flew at an azimuth of 77.0 degrees. Anyway, the graph below shows the motion of the Moon and the computed intended trajectory and the computed actual trajectory.