Moon Signal Bounce: How Is the Returned Laser Signal Received?

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Discussion Overview

The discussion revolves around the mechanics of how laser signals are bounced off retro-reflectors on the moon to measure the distance to the moon. Participants explore the implications of the Earth's rotation and the divergence of laser beams in relation to the timing of signal reception.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that retro-reflectors minimize scattering by returning the signal along the same path it arrived, but question how this works given the Earth's rotation during the signal's travel time.
  • Others suggest that beam divergence plays a significant role in how the signal is received, with some estimating that a laser beam can spread to about a mile by the time it reaches the moon.
  • There is discussion about the divergence of the reflected light and how the angle between the mirrors in retro-reflectors is not exactly 90 degrees, affecting the returning beam's cone shape.
  • One participant raises the concern that the signal must be aimed at a point ahead of the retro-reflector due to the moon's movement, suggesting a need for precise calculations to account for this motion.
  • Another participant references an article that states the laser pulse diameter increases significantly upon arrival at the moon and when returning to Earth, which could impact the reception of the signal.
  • There is mention of the potential for false distance measurements if pulses are sent too rapidly, highlighting the importance of timing and pulse spacing in achieving accurate measurements.

Areas of Agreement / Disagreement

Participants express varying views on the effects of beam divergence and the implications of the Earth's rotation on signal reception. There is no consensus on the best approach to account for these factors, and the discussion remains unresolved.

Contextual Notes

Some assumptions about the behavior of laser beams and the accuracy of retro-reflectors are not fully explored, and the discussion includes various estimates and interpretations of the physical phenomena involved.

Mentallic
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I've been reading on how the distance to the moon is calculated by bouncing a laser signal on the retro-reflectors and measuring the time it takes the light to return to Earth, but what I've seen is that the retro-reflectors do a good job of minimizing scattering by returning the signal along the same direction in which it arrived.

Since the light takes approximately 2.5 seconds to reach the moon and back, and since being near the equator of the Earth, the rotational speed is about 1,600km/h on the surface or about 1.2km / 2.5s, so my question is how do the experimenters receive the signal if the retro-reflectors bounce the signal back to where the signal was first emitted which by that point is 1.2km off the mark?
 
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Actually, it probably has to do with beam divergence.
 
Mentallic said:
Actually, it probably has to do with beam divergence.

Yep. A laser beam spreads to something like a mile or so by the time it reaches the moon if I remember correctly.
 
Typical retro-reflectors also give a little divergence.
 
Drakkith said:
Yep. A laser beam spreads to something like a mile or so by the time it reaches the moon if I remember correctly.

And the small portion of reflected light would diverge by the same amount when it hits the Earth again?

I like Serena said:
Typical retro-reflectors also give a little divergence.

By divergence, I'm talking about how laser lights will expand into a cone shape. Do you mean scattering?
 
Mentallic said:
And the small portion of reflected light would diverge by the same amount when it hits the Earth again?



By divergence, I'm talking about how laser lights will expand into a cone shape. Do you mean scattering?

The reflected light would have a diverging angle that is much smaller.
That is because the part of the cone that actually hits the retro-reflectors has a very small diverging angle.

However, the angle between the mirrors in retro-reflector material is intentionally not exactly 90 degrees.
So the returning beam will have a cone shape again.
 
Mentallic said:
I've been reading on how the distance to the moon is calculated by bouncing a laser signal on the retro-reflectors and measuring the time it takes the light to return to Earth, but what I've seen is that the retro-reflectors do a good job of minimizing scattering by returning the signal along the same direction in which it arrived.

Since the light takes approximately 2.5 seconds to reach the moon and back, and since being near the equator of the Earth, the rotational speed is about 1,600km/h on the surface or about 1.2km / 2.5s, so my question is how do the experimenters receive the signal if the retro-reflectors bounce the signal back to where the signal was first emitted which by that point is 1.2km off the mark?

If the retro-reflectors were that accurate, the signal would actually ahead(to the east) of the laser, because the moon moves at about 1 km/s, so the beam has to be sent to a point 1.25 km ahead of the reflector, and will be reflected to a point 2.5 km ahead of the laser, while the Earth has only moved 1.2 km in that time.
 
This article says..

http://www.fesg.bv.tum.de/91872-bD1lbg-~fesg~forschung~llr.html

..arriving at the Moon, the laser pulse has a diameter of more than 5 km.

returning to the ground station the reflected pulses show diameters of more than 5 km

A single pulse has a diameter of 75 cm and is only 6 cm long

The pulses are short enough that a very large number can be sent before any come back.
 
This is just semi related, but might be interesting to some. In the days before human-made communication satellites, we were using a natural one:

http://en.wikipedia.org/wiki/EME_(communications )
Earth-Moon-Earth, also known as moon bounce, is a radio communications technique which relies on the propagation of radio waves from an Earth-based transmitter directed via reflection from the surface of the Moon back to an Earth-based receiver.
 
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Mentallic said:
I've been reading on how the distance to the moon is calculated by bouncing a laser signal on the retro-reflectors and measuring the time it takes the light to return to Earth, but what I've seen is that the retro-reflectors do a good job of minimizing scattering by returning the signal along the same direction in which it arrived.

Since the light takes approximately 2.5 seconds to reach the moon and back, and since being near the equator of the Earth, the rotational speed is about 1,600km/h on the surface or about 1.2km / 2.5s, so my question is how do the experimenters receive the signal if the retro-reflectors bounce the signal back to where the signal was first emitted which by that point is 1.2km off the mark?

This is not what they achieve - because, when they receive the echo, they are not in the position that they were when the pulse was emitted. All that is necessary is for the reflector to reflect sufficient light in the direction of where they will be 5 seconds later. The angle that this represents is very small, surely? (1.2km in 380Mm = about one second of arc, I think)

@CWatters: If you send the pulses at a rate that is faster than the transit time, you can get a false distance measurement because you can get the phase of the transmitted and received pulse streams wrong. I do agree that you can eliminate this problem by starting with widely spaced pulses and working up, so you can increase the signal to noise ratio and, hence, the accuracy.
 

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