Kinetic energy transfer from shockwave to secondary body

In summary: Then that cannot be the answer.The method is to let the answer be of the form velocity=pressure adensitybdistancec. In MLT notation that becomes ##LT^{-1}=(ML^{-1}T^{-2})^a(ML^{-3})^bL^c##.Three equations, three unknowns.
  • #1
KataruZ98
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Homework Statement
I have an object A possessing a known mass of 10kg and density of 1,000kg/m^3 exposed to a shockwave in a way the latter impacts A over an area of one square meter at a right angle. The pressure of the shockwave at the point of contact is 10PSI.
Relevant Equations
Kinetic energy transferred by the shockwave to body A
I would guess that by multiplying the pressure exerted by the shockwave on the body, and then the resulting force - here ~69 Newtons - per the distance the shockwave passed through when traversing body A, I could get the work done but I’m not sure if it’s that easy and whether or not I should consider the shockwave accelerating when passing from a less dense to denser medium.
 
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  • #2
Thinking of it per unit area (doubling the area should yield the same velocity gain) we have a pressure, a density, a distance and a velocity. What does dimensional analysis say?
 
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  • #3
Hm, I’m kinda lost honestly. Unfortunately I’m not well versed.
 
  • #4
KataruZ98 said:
Hm, I’m kinda lost honestly. Unfortunately I’m not well versed.
Are you unfamiliar with dimensional analysis? Look it up.
It uses M for mass, L for length, T for time,…
Pressure is ML-1T-2
Density ML-3
Distance L
Velocity LT-1
How can you combine the first three, raising each to some power and multiplying the terms together, to make the last?
 
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  • #5
haruspex said:
Are you unfamiliar with dimensional analysis? Look it up.
It uses M for mass, L for length, T for time,…
Pressure is ML-1T-2
Density ML-3
Distance L
Velocity LT-1
How can you combine the first three, raising each to some power and multiplying the terms together, to make the last?
Well I would say I should divide density by the product of pressure and distance - though this leaves a T-2 as denominator.
 
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  • #6
KataruZ98 said:
Well I would say I should divide density by the product of pressure and distance - though this leaves a T-2 as denominator.
Then that cannot be the answer.
The method is to let the answer be of the form velocity=pressure adensitybdistancec. In MLT notation that becomes ##LT^{-1}=(ML^{-1}T^{-2})^a(ML^{-3})^bL^c##.
Three equations, three unknowns.
 
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FAQ: Kinetic energy transfer from shockwave to secondary body

What is kinetic energy transfer from a shockwave to a secondary body?

Kinetic energy transfer from a shockwave to a secondary body refers to the process by which energy from a shockwave is imparted to another object, causing it to move or deform. This transfer of energy can occur in various scenarios, such as explosions, impacts, or other high-energy events, and it involves complex interactions between the shockwave and the secondary body.

How does the medium affect the transfer of kinetic energy from a shockwave?

The medium through which a shockwave travels significantly affects the transfer of kinetic energy. Different media (air, water, solid materials) have varying densities and elastic properties, which influence the speed and intensity of the shockwave. For instance, shockwaves travel faster and with greater energy in denser media like water compared to air, leading to more efficient energy transfer to secondary bodies in such environments.

What factors influence the efficiency of kinetic energy transfer from a shockwave to a secondary body?

Several factors influence the efficiency of kinetic energy transfer, including the properties of the shockwave (intensity, speed, and frequency), the characteristics of the secondary body (mass, shape, material composition), and the nature of the interaction between the shockwave and the body (angle of incidence, surface area in contact). Additionally, the duration of the shockwave and the presence of any barriers or interfaces can also impact the energy transfer process.

Can kinetic energy transfer from a shockwave cause permanent deformation or damage to a secondary body?

Yes, kinetic energy transfer from a shockwave can cause permanent deformation or damage to a secondary body. The extent of the damage depends on the energy level of the shockwave and the material properties of the secondary body. High-energy shockwaves can induce significant stresses and strains, leading to fractures, dents, or complete structural failure, especially in brittle or less resilient materials.

What are some practical applications or implications of studying kinetic energy transfer from shockwaves?

Understanding kinetic energy transfer from shockwaves has numerous practical applications and implications. In defense and security, it helps in designing better protective gear and structures to withstand explosions. In aerospace and automotive industries, it aids in improving crash safety and impact resistance. Additionally, it has applications in medical fields, such as understanding the effects of shockwaves on tissues during lithotripsy or blast injuries, and in industrial processes where shockwaves are used for material testing or forming.

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