Simple Harmonic Motion (Total Energy)

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SUMMARY

The discussion clarifies the derivation of total energy in Simple Harmonic Motion (SHM), specifically addressing the confusion around kinetic energy (KE) and potential energy (PE). It establishes that KE is given by the formula KE = (1/2)kA²cos²(ωt+φ) and PE by PE = (1/2)kA²sin²(ωt+φ). The total energy E combines these two expressions, resulting in E = (1/2)kA²(sin²(ωt+φ) + cos²(ωt+φ)), which simplifies to E = (1/2)kA² due to the Pythagorean identity sin²θ + cos²θ = 1.

PREREQUISITES
  • Understanding of Simple Harmonic Motion (SHM)
  • Familiarity with kinetic energy (KE) and potential energy (PE) formulas
  • Knowledge of trigonometric identities, specifically sin²θ + cos²θ = 1
  • Basic grasp of angular frequency (ω) and phase constant (φ)
NEXT STEPS
  • Study the derivation of energy conservation in Simple Harmonic Motion
  • Explore the implications of phase constants in SHM
  • Learn about the relationship between mass, spring constant, and angular frequency in SHM
  • Investigate the graphical representation of SHM energy components over time
USEFUL FOR

Students of physics, educators teaching mechanics, and anyone interested in the principles of energy conservation in oscillatory systems will benefit from this discussion.

KiNGGeexD
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I have a question about the derivation that I have attached! I understand that both KE and U are 1/2 kA^2 So how is it that the two combine is also equal to 1/2kA^2Not sure if I'm missing something but I'm a little confused :(
 
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Part of the problem is that what you "understand" is not true. It is NOT the case that "both KE and U are 1/2 kA^2". What is true is that E= 1/2 kA^2 sin^2(\omega t+ \phi) and U= 1/2 kA^2 cos^2(\omega t+ \phi).

Adding those gives KE+ U= 1/2 kA^2(sin^2(\theta)+ cos^2(\theta)). Now use the fact that sin^2(\theta)+ cos^2(\theta)= 1 for all \theta!
 
So that leaves

1/2mv^2 + 1/2kA^2?
 
KiNGGeexD said:
[
I have a question about the derivation that I have attached! I understand that both KE and U are 1/2 kA^2 So how is it that the two combine is also equal to 1/2kA^2Not sure if I'm missing something but I'm a little confused :(

KE = (1/2)mv2 and v= ωAcos(ωt+ø)
So ,KE = (1/2)mω2A2cos2(ωt+ø)

But ,k = mω2

Hence KE = (1/2)kA2cos2(ωt+ø) (1)

PE = (1/2)kx2 and x= Asin(ωt+ø)
So ,PE = (1/2)kA2sin2(ωt+ø) (2)

E=KE+PE

Using the fact sin2θ+cos2θ =1 ,

E=(1/2)kA2
 
But there are two terms of kA^2?

I feel like I'm missing something obvious?
 
KiNGGeexD said:
But there are two terms of kA^2?

I feel like I'm missing something obvious?

E = (1/2)kA2cos2(ωt+ø) + (1/2)kA2sin2(ωt+ø)

Take (1/2)kA2 common from both the terms ,

E = (1/2)kA2[cos2(ωt+ø) + sin2(ωt+ø)]

Hence E = (1/2)kA2
 
Ahh so you take 1/2kA^2 out as a common factor
 
Yes...just like if we have 2a+2b ,we can write it as 2(a+b) .
 
I knew it would be something trivial! That's a bunch mate!
 

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