a body executes SHM with an amplitude xo its energy is half kinetic energy and half potential energy when displacement is.
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The total energy of such body always remains constant, let this be EE.
E=K+UE=K+U, where K and UK and U are the kinetic and potential energies respectively.
If the total energy is half Kinetic and half potential, it is true only if K=UK=U.
Let the displacement of the body be xx.
The velocity of a body in SHM is given by:
v=ω(A2−x2−−−−−−√)v=ω(A2−x2), where,
ω=km−−−√ω=km, and kk is the force constant for the body and AA is the amplitude of the body.
The kinetic energy of the body is:
K=12mv2K=12mv2
=12m(ω2(A2−x2)) =12m(ω2(A2−x2))
=12mkm(A2−x2) =12mkm(A2−x2)
K=k2(A2−x2)…(i)K=k2(A2−x2)…(i)
The force done in increasing displacement of a body by x=F=−kxx=F=−kx
Let the increase in potential energy for changing the displacement by dxdx be −dU−dU.
Here, the negative sign indicates that the change occurs in a direction opposite to that of the change in the displacement.
Since force applied is conservative,
−dU=F.dx−dU=F.dx
⟹−dU=−k xdx⟹−dU=−k xdx
Integrating both sides,
∫U0dU=k∫x0xdx∫0UdU=k∫0xxdx
⟹U=12kx2⟹U=12kx2
Now, from the original condition, K=UK=U
Or,
12k(A2−x2)=12kx212k(A2−x2)=12kx2
⟹A2−x2=x2⟹A2−x2=x2
⟹2x2=A2⟹2x2=A2
⟹x2=A22⟹x2=A22
⟹x=±A2–√⟹x=±A2
At displacements ±A2–√±A2, the kinetic energy is equal to the potential energy.
E=K+UE=K+U, where K and UK and U are the kinetic and potential energies respectively.
If the total energy is half Kinetic and half potential, it is true only if K=UK=U.
Let the displacement of the body be xx.
The velocity of a body in SHM is given by:
v=ω(A2−x2−−−−−−√)v=ω(A2−x2), where,
ω=km−−−√ω=km, and kk is the force constant for the body and AA is the amplitude of the body.
The kinetic energy of the body is:
K=12mv2K=12mv2
=12m(ω2(A2−x2)) =12m(ω2(A2−x2))
=12mkm(A2−x2) =12mkm(A2−x2)
K=k2(A2−x2)…(i)K=k2(A2−x2)…(i)
The force done in increasing displacement of a body by x=F=−kxx=F=−kx
Let the increase in potential energy for changing the displacement by dxdx be −dU−dU.
Here, the negative sign indicates that the change occurs in a direction opposite to that of the change in the displacement.
Since force applied is conservative,
−dU=F.dx−dU=F.dx
⟹−dU=−k xdx⟹−dU=−k xdx
Integrating both sides,
∫U0dU=k∫x0xdx∫0UdU=k∫0xxdx
⟹U=12kx2⟹U=12kx2
Now, from the original condition, K=UK=U
Or,
12k(A2−x2)=12kx212k(A2−x2)=12kx2
⟹A2−x2=x2⟹A2−x2=x2
⟹2x2=A2⟹2x2=A2
⟹x2=A22⟹x2=A22
⟹x=±A2–√⟹x=±A2
At displacements ±A2–√±A2, the kinetic energy is equal to the potential energy.
ayan7456:
hmm
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