Related Experiment Video
Updated: Feb 28, 2026

09:41
Blast Quantification Using Hopkinson Pressure Bars
Published on: July 5, 2016
9.5K
Measurement of the shell decompression in direct-drive inertial-confinement-fusion implosions
D T Michel1, S X Hu1, A K Davis1
1Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA.
Physical Review. E
|June 17, 2017
Summary
Reducing the shell adiabat in direct-drive implosions initially thins the shell, but further reduction causes Rayleigh-Taylor instability, increasing shell thickness. Laser imprint is identified as a key driver of these instabilities.
Area of Science:
- Plasma Physics
- Inertial Confinement Fusion
Background:
- Understanding shell dynamics is crucial for inertial confinement fusion (ICF) energy gain.
- The adiabat, a measure of shell entropy, significantly influences implosion performance.
Purpose of the Study:
- To investigate the impact of shell adiabat on in-flight shell thickness during direct-drive implosions.
- To identify the primary mechanisms driving shell nonuniformities.
Main Methods:
- Performed direct-drive implosions on the OMEGA laser facility.
- Measured in-flight shell thickness across a range of adiabat values.
- Utilized hydrodynamic simulations to analyze instability growth and laser imprint effects.
Main Results:
- In-flight shell thickness decreased from 75±2 to 60±2μm as the adiabat was reduced from 6 to 4.5.
- Further adiabat reduction to 1.8 resulted in increased shell thickness (75±2μm) due to Rayleigh-Taylor instability.
- Hydrodynamic simulations indicated laser imprint as the dominant initial perturbation source.
Conclusions:
- The adiabat plays a critical role in controlling in-flight shell thickness.
- Rayleigh-Taylor instability growth becomes significant at low adiabat values, counteracting initial thinning.
- Laser imprint is a critical factor to mitigate for stable ICF implosions.
Related Concept Videos
Conservation of Momentum: Problem Solving
12.4K
Solving problems using the conservation of momentum requires four basic steps:
12.4K
Rocket Propulsion In Empty Space - II
3.6K
The motion of a rocket is governed by the conservation of momentum principle. A rocket's momentum changes by the same amount (with the opposite sign) as the ejected gases. As time goes by, the rocket's mass (which includes the mass of the remaining fuel) continuously decreases, and its velocity increases. Therefore, the principle of conservation of momentum is used to explain the dynamics of a rocket's motion. The ideal rocket equation gives the change in velocity that a rocket...
3.6K
Rocket Propulsion in Gravitational Field - II
2.9K
A rocket's velocity in the presence of a gravitational field is decreased by the amount of force exerted by Earth's gravitational field, which opposes the motion of the rocket. If we consider thrust, that is, the force exerted on a rocket by the exhaust gases, then a rocket's thrust is greater in outer space than in the atmosphere or on a launch pad. In fact, gases are easier to expel in a vacuum.
A rocket's acceleration depends on three major factors, consistent with the...
A rocket's acceleration depends on three major factors, consistent with the...
2.9K
The Energies of Atomic Orbitals
30.5K
In an atom, the negatively charged electrons are attracted to the positively charged nucleus. In a multielectron atom, electron-electron repulsions are also observed. The attractive and repulsive forces are dependent on the distance between the particles, as well as the sign and magnitude of the charges on the individual particles. When the charges on the particles are opposite, they attract each other. If both particles have the same charge, they repel each other.
30.5K
Nuclear Fusion
34.0K
The process of converting very light nuclei into heavier nuclei is also accompanied by the conversion of mass into large amounts of energy, a process called fusion. The principal source of energy in the sun is a net fusion reaction in which four hydrogen nuclei fuse and ultimately produce one helium nucleus and two positrons.
A helium nucleus has a mass that is 0.7% less than that of four hydrogen nuclei; this lost mass is converted into energy during the fusion. This reaction produces about...
A helium nucleus has a mass that is 0.7% less than that of four hydrogen nuclei; this lost mass is converted into energy during the fusion. This reaction produces about...
34.0K
Rocket Propulsion in Empty Space - I
3.9K
The driving force for the motion of any vehicle is friction, but in the case of rocket propulsion in space, the friction force is not present. The motion of a rocket changes its velocity (and hence its momentum) by ejecting burned fuel gases, thus causing it to accelerate in the direction opposite to the velocity of the ejected fuel. In this situation, the mass and velocity of the rocket constantly change along with the total mass of ejected gases. Due to conservation of momentum, the...
3.9K

