A pressing problem with Kinetic Energy. ALL PHYSICISTS HELP!!
the equation for kinetic energy is actually used as 21mv2 as it is a very useful quantity and actually is derived from the work done by a force, without any changes to internal energy or potential energy of the system.
W=∫ΣF⋅dr
Subbing in ΣF=ma, you will get
W=∫ma⋅dr
Subbing in a=dtdv, you will get
W=∫mdtdv⋅dr
Since v=dtdr, it implies that dr=vdt
W=∫mdtdv⋅vdt
W=∫vivfmv⋅dv
W=21m(vf⋅vf)−21m(vi⋅vi)=21mvf2−21mvi2
This showed that the quantity 21mv2 can be denoted as the energy of a moving object, and any change in kinetic energy must be from an external work done
However we know that the general definition of force is ΣF=dtdp
Hence work would be W=∫dtdp⋅dr.
Then from that kinetic energy should be derived, as it more accurately depicts motion of an object of changing mass. Then how do we derive ∫dtdp⋅dr
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It's similar. Hint: Product law for derivatives. dtdp=dtd(mv)=m⋅dtdv+v⋅dtdm. Note that dtdm=0 for constant mass, that is the non-relativistic case. Note that F=ma is not true for relativistic cases. (Sorry lazy to put vector arrows and stuff =P)
Actually according to relativity, our mass is increasing with velocity but not that much. So, the kinetic energy formula holds. Also, the formula is m_{real}=\frac{m_{rest}}{\sqrt{1-\frac{v^{2}}{c^{2}}}
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It's similar. Hint: Product law for derivatives. dtdp=dtd(mv)=m⋅dtdv+v⋅dtdm. Note that dtdm=0 for constant mass, that is the non-relativistic case. Note that F=ma is not true for relativistic cases. (Sorry lazy to put vector arrows and stuff =P)
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But what if mass is not constant so dtdm=0
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Then you have to find out at what rate m is changing wrt to t and continue with the derivation.
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KE=21mv2
Would not that be equivalent to sayingLog in to reply
Actually according to relativity, our mass is increasing with velocity but not that much. So, the kinetic energy formula holds. Also, the formula is m_{real}=\frac{m_{rest}}{\sqrt{1-\frac{v^{2}}{c^{2}}}
dmv/dt .dr here dr/dt =v and mdv will be left so we can procede in the same way above