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If it is the surface of Venus, most of it is CO2, which can be approximated.
Equation of state: pv=nkt, particle number density n=n v=p kt=90*10 5 ( 10 -23*740)= [m 3].
CO2 molecular diameter d, and? [nm] (I thought it was calculated), molecular weight m=44*10-3 [kg mol].
Impact radius = d, impact cross-sectional area a=pi*d 2= [m 2]average thermal velocity of gas molecules u=sqrt(8*k*t pi*m)=sqrt(8*r*t pi*m)= [m s].
Mean free path = (sqrt(2)Na) -1= [nm] Collision frequency z=u = [ s].
Period t = 1 z= [ns].
The k-boltzman constant (10 23 j k 1) is probably like this?
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The mean free path is the average of the distance traveled by particles between two adjacent collisions. =vt, v is the average rate, and the average rate is independent of pressure, only temperature and particle type.
v = root number (rt m), where m is the molar mass of the gas, and the gas of Venus is carbon dioxide, right? The landlord confirms for himself. Calculate v, that is, t.
If you have any questions, please feel free to ask.
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Divide the average free path by the particle velocity.
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The larger the average free path of a particle, it doesn't necessarily mean it's easier to penetrate. This is because when particles move in matter, they are affected by various interaction forces, including scattering, **, absorption, etc.
When particles collide with matter or interact with silver clusters, their energy and direction may change. If these interactions are frequent and intense, the particles may be blocked or scattered as they pass through the matter, even if the mean free path is very long.
It is also important to note that the average free path of the same type of particle (e.g., electron, photon, etc.) may also vary between different materials. This is because different materials have different densities, structures, and chemical compositions, which produce different effects when interacting with particles.
In summary, it is not possible to simply relate the mean free path size to penetration. To accurately assess a particle's ability to pass through a substance under certain conditions, a number of factors need to be taken into account, and detailed calculations and analyses are carried out in a pure canopy.
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The larger the mean free path of the particles, the longer the average distance traveled by the particles as they move in the medium. This is not directly related to the penetration ability of particles in the medium, because the physical properties of the medium, the properties of the particles and the spatial structure and other factors will affect the penetration ability of particles in the medium. For example, for gas molecules, the greater the average self-talk bend from the distance, the smaller the probability of the molecules colliding in the gas, which may make it easier for the gas to penetrate small obstacles.
In the case of solid materials, the interaction between the particles and the material may increase, hindering the penetration of the particles. Therefore, it is not possible to simply assume that the larger the average free path of the particle, the easier it is to penetrate.
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The mean free path of a particle is the average distance at which a particle can maintain its original motion after colliding with other molecules in the medium. The larger the mean free path, the longer the slag is able to travel without disturbance as it moves in the medium.
For particles with high energy and short wavelengths, such as rays and photons, their interaction with matter is mainly astigmatism and absorption. At this point, the greater the mean free path, the easier it is for the particles to penetrate the matter. However, for other types of particles, such as neutral particles, electrons, etc., their interaction with matter is mainly through electromagnetic force or strong action, and the smaller the average free path, the shorter the distance it moves in the matter and the less easy it is to penetrate the matter.
Therefore, it needs to be analyzed on a case-by-case basis and cannot be generalized.
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The larger the mean free path of the particle, the less impact and scattering it will be when moving in the megalometer in the medium. This means that it is able to maintain a relatively stable direction of motion and velocity as it propagates through the medium, making it easier to penetrate the medium. Therefore, particles with a larger mean free path, such as high-energy electrons, neutrons, etc., are more likely to penetrate the medium under the same circumstances than particles with a smaller average free path.
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Yes, the mean free path of a particle is the average distance traveled by a particle between colliding with other particles. Generally speaking, the greater the average free path of the particle, the smaller the resistance encountered by the particle during motion, and therefore the stronger the ability to penetrate the hole. But it also depends on factors such as the velocity, mass, and energy of the particles.
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