Where does the missing energy go?

  • Thread starter Thread starter audjobman
  • Start date Start date
  • Tags Tags
    Energy
AI Thread Summary
When a mass is suspended from a spring, the gravitational potential energy lost should equal the energy stored in the spring, but calculations show a discrepancy. The equation mg=kx indicates the equilibrium position, while energy considerations suggest that half of the energy is unaccounted for. This missing energy can be attributed to the work done against the force when gently lowering the mass, which is absorbed as internal energy in the muscles rather than converted to kinetic or thermal energy. If the mass were dropped, it would have kinetic energy upon reaching the spring, leading to oscillations around the equilibrium position. Ultimately, energy loss occurs due to vibrations dissipating into the surroundings, causing the mass to settle at rest.
audjobman
Messages
1
Reaction score
0
Where does the missing energy go?!

When suspending a mass from a spring, we can determine the distance the spring is stretched by using mg=kx. However, if we consider the energy transferred, the gravitational potential energy lost by the mass should equal the energy stored in the spring, no?

But when I use \DeltaEg=mg\Deltah and Ep=½2x2, and I consider that the change in height for the mass and the distance the spring is stretched are the same, then:

mgx=½kx^2

Simplifying this gives me mg=½kx. So, where does the other half of the energy go?

I've tried considering that it must be converted to kinetic energy or thermal energy but I've conducted the experiment and, when the mass is gently lowered to rest, there is no significant heating of the spring that I can see and there is no apparent kinetic energy. Am I missing something?

I'm certain I am. Please help me find my way...
 
Physics news on Phys.org


The force increases with distance. The average force is not kx but half that.
 


audjobman said:
I've tried considering that it must be converted to kinetic energy or thermal energy but I've conducted the experiment and, when the mass is gently lowered to rest, there is no significant heating of the spring that I can see and there is no apparent kinetic energy. Am I missing something?
When you gently lower the mass, you exert a force on the mass which does negative work. You essentially absorb that energy in your muscles, turning it into internal energy ("heat"). If you didn't exert that force--if you just let the mass drop onto the spring--then the mass would end up with kinetic energy.
 


audjobman said:
When suspending a mass from a spring, we can determine the distance the spring is stretched by using mg=kx. However, if we consider the energy transferred, the gravitational potential energy lost by the mass should equal the energy stored in the spring, no?

But when I use \DeltaEg=mg\Deltah and Ep=½2x2, and I consider that the change in height for the mass and the distance the spring is stretched are the same, then:

mgx=½kx^2

Simplifying this gives me mg=½kx. So, where does the other half of the energy go?

I've tried considering that it must be converted to kinetic energy or thermal energy but I've conducted the experiment and, when the mass is gently lowered to rest, there is no significant heating of the spring that I can see and there is no apparent kinetic energy. Am I missing something?

I'm certain I am. Please help me find my way...

The equation mg=kx gives you the equilibrium distance, let us call it x0. Of course, the potential energy at this position is mgx0=(1/2)kx02.

But if you attach the mass at x=0 and let it go, the force mg will make larger work: the mass will pass by the equilibrium position and will go down, to 2x0. Then the mass will oscillate around the equilibrium position. While passing x0, the mass will also have a kinetic energy.

Bob.
 
Last edited:


And extending Doc als and Bob for shorts answers the vibrations will die down as energy is lost to the surroundings and the mass will eventually come to rest at its equilibrium position.
 
Thread 'Gauss' law seems to imply instantaneous electric field propagation'
Imagine a charged sphere at the origin connected through an open switch to a vertical grounded wire. We wish to find an expression for the horizontal component of the electric field at a distance ##\mathbf{r}## from the sphere as it discharges. By using the Lorenz gauge condition: $$\nabla \cdot \mathbf{A} + \frac{1}{c^2}\frac{\partial \phi}{\partial t}=0\tag{1}$$ we find the following retarded solutions to the Maxwell equations If we assume that...
Dear all, in an encounter of an infamous claim by Gerlich and Tscheuschner that the Greenhouse effect is inconsistent with the 2nd law of thermodynamics I came to a simple thought experiment which I wanted to share with you to check my understanding and brush up my knowledge. The thought experiment I tried to calculate through is as follows. I have a sphere (1) with radius ##r##, acting like a black body at a temperature of exactly ##T_1 = 500 K##. With Stefan-Boltzmann you can calculate...
Thread 'Griffith, Electrodynamics, 4th Edition, Example 4.8. (First part)'
I am reading the Griffith, Electrodynamics book, 4th edition, Example 4.8 and stuck at some statements. It's little bit confused. > Example 4.8. Suppose the entire region below the plane ##z=0## in Fig. 4.28 is filled with uniform linear dielectric material of susceptibility ##\chi_e##. Calculate the force on a point charge ##q## situated a distance ##d## above the origin. Solution : The surface bound charge on the ##xy## plane is of opposite sign to ##q##, so the force will be...
Back
Top