Nuclear pulse propulsion with low Z propellant?

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Discussion Overview

The discussion revolves around the use of low atomic number (Z) propellants in nuclear pulse propulsion systems, specifically the Orion drive concept. Participants explore the implications of using different materials for the pulse units and the pusher plate, examining the potential for higher exhaust velocities and the mechanics of momentum transfer in the context of nuclear detonations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question the necessity of high Z propellants like tungsten, suggesting that lower Z materials could yield higher exhaust velocities.
  • Others argue that tungsten is used for the pusher plate due to its high melting point and that alternatives like graphite could be considered.
  • One participant cites a reputable source claiming that high Z propellants are required for effective momentum transfer in nuclear shaped charge pulse units.
  • Another participant references experimental observations of tungsten or tantalum disks ablated by x-rays, suggesting that high Z materials maximize momentum transfer per unit energy.
  • Concerns are raised about the practicality of the Orion drive, with one participant expressing skepticism about its feasibility and suggesting that a thick tungsten shield would be necessary to protect the rocket from radiation.
  • Questions are posed regarding the mechanics of momentum transfer, particularly the role of plasma waves and the efficiency of high mass ions compared to x-rays in producing thrust.
  • A participant presents a hypothetical homework problem involving calculations of impulse and momentum transfer related to the use of a tungsten pusher plate.
  • Another participant inquires about the source matter for propulsion and the effects of a nuclear blast in space.

Areas of Agreement / Disagreement

Participants express differing views on the necessity and effectiveness of high Z propellants, with no consensus reached on the feasibility of the Orion drive or the specific materials that should be used in its design.

Contextual Notes

Discussions include assumptions about the efficiency of various materials and the conditions under which momentum transfer occurs. Some mathematical steps and definitions remain unresolved, particularly regarding the calculations of impulse and momentum transfer.

Decimator
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I've been doing some reading about Orion-drive spacecraft , but I don't understand the requirement of a high Z propellant like tungsten. Assuming that the pulse unit were detonated further away from the craft to prevent it from drilling a hole in the pusher plate due to its narrower angle, why couldn't the pulse units use a low Z propellant to gain a higher exhaust velocity? I assume there's a reason, but it isn't easily found information.
 
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I'm not sure where one found the requirement for tungsten.

The ORION concept is one of detonating a nuclear (or thermonuclear device) behind the spacecraft , and capturing the blast wave from the detonation. One does not need tungsten, except possibly that is used for the 'pusher plate' because it has a high melting point. One could of course use graphite.

Some ORION concepts use an ablative surface that would be ablated or evaporated/sublimate(?) from the surface. But then it's a matter of get a more or less uniform coating.

For high specific impulse, one would want the lowest atomic/molecular mass possible, but then liquid hydrogen is not amenable to being coated on a hot surface.
 
My question relates to Orion drives which do not require an ablative surface. I got the high z propellant requirement from http://www.projectrho.com/rocket/enginelist.php#orion", which I understand to be a fairly reputable site.

Specifically, I'm talking about the design of the nuclear shaped charge pulse units themselves:

orionpunit.jpg


Note the use of tungsten as propellant. This is the part I do not understand.
 
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I have seen (over 50 years ago) either a tungsten or tantalum disk that had ≈1 mm of surface ablated by x-rays from a small (few kt) blast. I believe the recoil force (impulse) was measured. I think the reason for high Z is to maximize the momentum transfer (thrust) per unit x-ray energy. Recall p2=2ME

See equation for ablation pressure in

http://nuclearweaponarchive.org/Nwfaq/Nfaq4-4.html#Nfaq4.4.3.3

Bob S
 
Decimator said:
My question relates to Orion drives which do not require an ablative surface. I got the high z propellant requirement from http://www.projectrho.com/rocket/enginelist.php#orion", which I understand to be a fairly reputable site.

Specifically, I'm talking about the design of the nuclear shaped charge pulse units themselves:

orionpunit.jpg


Note the use of tungsten as propellant. This is the part I do not understand.
:smile: It seems to be someone's wild fantasy.
 
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Astronuc said:
:smile: It seems to be someone's wild fantasy.
I firmly believe that this type of propulsion is unworkable, but if it could work, the only way is if there is a large thick tungsten shield between the nuclear device (a few kt or less) and the rocket body. The tungsten shield protects the rocket and its contents from the radiation. The x-rays from the detonation will heat up and ablate the tungsten surface. Recoiling material ablating from the tungsten surface will transfer a momentum impulse to the rocket. To get the maximum momentum impulse p·Δt from the available x-ray ablating energy, p2 = 2ME, showing that M should be maximized, where M represents the gram-molecular-weight of tungsten.

The only propulsion method that is less likely to work than ORION is the antimatter drive. See

http://en.wikipedia.org/wiki/Antimatter_rocket

Bob S
 
Why do you think it won't work? Why can't a wave of plasma from a pulse unit impart momentum on the pusher plate?
 
Decimator said:
Why do you think it won't work? Why can't a wave of plasma from a pulse unit impart momentum on the pusher plate?
Momentum can only be transferred to the rocket if there is an equal and opposite momentum (thrust) in the direction away from the rocket. High mass ions are a lot more efficient than x rays in producing thrust.

Here is a homework problem for you. Suppose there is a tungsten shield (pusher plate) between the nuclear device and the rocket. The tungsten shield intercepts 25% of the total x-rays emitted isotropically from the explosion. Assume that one Avagadro's number of 10-keV x-rays (Exray = hν) hit the tungsten shield. What is the impulse (Newton-seconds)? Assuming the x-rays are perfectly reflected away from the rocket (like a mirror), what is the additional impulse? Now, instead of the x-rays being reflected, suppose each 10-keV x-ray causes one tungsten atom (184 grams total) to be ablated from the pusher plate surface (very simplistic model), and the tungsten atom ablates with an energy EW=Exray=½MV2, where M and V are the rest mass and velocity of the ablated tungsten atoms. What is now the total momentum transfer to the tungsten pusher plate (Newton-seconds)? Would the momentum transfer be more or less if the pusher plate were made of copper?

Bob S
 
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What is the source matter that expands greatly when superheated that get's expelled for propulsion?

Or

If a nuke blasts in space and there is no matter for it to heat, does it make a sound?
 
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