Derive the equation for kinetic energy

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SUMMARY

The discussion focuses on deriving the equation for kinetic energy, specifically for a body of mass m and velocity v. The initial attempt referenced the work-energy theorem, leading to the expression KE = ½mv² - ½mu², which is valid under constant acceleration. A more comprehensive approach was presented, incorporating variable acceleration, resulting in the integral form ΔKE = ½m(v² - u²). This derivation confirms the foundational equation for kinetic energy in classical mechanics.

PREREQUISITES
  • Understanding of classical mechanics principles
  • Familiarity with the work-energy theorem
  • Knowledge of calculus, specifically integration
  • Basic concepts of force and acceleration
NEXT STEPS
  • Study the work-energy theorem in detail
  • Learn about variable acceleration and its implications in physics
  • Explore calculus applications in physics, particularly integration techniques
  • Investigate other forms of energy and their relationships to kinetic energy
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Students of physics, educators teaching mechanics, and anyone interested in understanding the derivation and implications of kinetic energy in classical mechanics.

Suraj M
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question:
I came across a question which said: Derive the equation for kinetic energy of a body of mass m and velocity v.
What do they mean?
Attempt:
I actually just wrote that by work energy theorem diff. in KE = work done
so Fx = KE
$$ max = m \frac {v²-u²}{2x} x = ½mv² - ½mu² $$
each of these terms represents a quantity called KE so this is the formula.
Is this right?? Because i seriously doubt it.
 
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Suraj M said:
question:
I came across a question which said: Derive the equation for kinetic energy of a body of mass m and velocity v.
What do they mean?
Attempt:
I actually just wrote that by work energy theorem diff. in KE = work done
so Fx = KE
$$ max = m \frac {v²-u²}{2x} x = ½mv² - ½mu² $$
each of these terms represents a quantity called KE so this is the formula.
Is this right?? Because i seriously doubt it.

That assumes constant acceleration. What if acceleration isn't constant?
 
Then i would do this:
$$ Fdx = dKE$$
$$ ma.dx = m. \frac{dv}{dt}dx = m v dv$$
$$mvdv = dKE$$
$$ m~₀∫^x vdv = ΔKE$$
$$ \frac{m(v^2 - u^2)}{2} = ΔKE $$
 

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