Quantum Physics energy between states

In summary, the conversation discussed the vibration of a 1.5kg mass on a spring with a spring constant of 20N/m and an amplitude of 3cm. The question was posed about the quantization of energy and finding the quantum number. It was also asked about the fractional change in energy if the quantum number changed by 1. It was mentioned that the energy difference between two continuous quantum states should be very small due to the large mass.
  • #1
frozen7
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A 1.5kg mass vibrates at an amplitude of 3cm on the end of a spring of spring constant 20N/m
(a) If the energy of the spring is quantized, find its quantum number.
(b) If n changes by 1, find the fractional change in energy of the spring.

I have solved part (a) but I could not solve part (b)

Does it mean the difference of energy between two continuous quantum?
 
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  • #2
frozen7 said:
A 1.5kg mass vibrates at an amplitude of 3cm on the end of a spring of spring constant 20N/m
(a) If the energy of the spring is quantized, find its quantum number.
(b) If n changes by 1, find the fractional change in energy of the spring.
I have solved part (a) but I could not solve part (b)
Does it mean the difference of energy between two continuous quantum?

Yes, it asks for the difference in Energy between the 2 states. The energy difference you get should be very small, as the mass is quite large.
 
  • #3


I would like to clarify that energy in quantum physics is not quantized in the same way as, for example, the energy levels of an atom. In quantum mechanics, energy is described by a wave function and can exist in a continuous spectrum of values. Therefore, the concept of a "quantum number" for energy is not applicable in this scenario.

In terms of the given situation, the energy of the spring can be calculated using the formula E = 1/2kx^2, where k is the spring constant and x is the amplitude. Plugging in the values given, we get E = 1/2(20 N/m)(0.03 m)^2 = 0.009 J. This is the total energy of the system and it does not have a specific "quantum number."

As for part (b), if n represents the number of nodes in the wave function, then a change of 1 in n would correspond to a change in the number of energy levels or states of the system. This would result in a change in the energy of the system, but it is not possible to determine the exact fractional change without knowing the specific values of n and the energy levels. In general, a change in n would result in a change in the energy of the system, but the exact magnitude of this change cannot be determined without further information.
 

1. What is the concept of "energy between states" in Quantum Physics?

In Quantum Physics, energy between states refers to the energy difference between two different energy levels or states of a quantum system. It is the energy required for an electron or other quantum particle to transition from one state to another.

2. How is the energy between states calculated in Quantum Physics?

The energy between states is calculated using the equation E = hf, where E is the energy, h is Planck's constant, and f is the frequency of the transition between states.

3. What are the implications of energy between states in Quantum Physics?

The energy between states plays a crucial role in understanding the behavior and properties of quantum systems. It helps explain phenomena such as the emission and absorption of light, atomic spectra, and electron energy levels in atoms.

4. Can energy between states be measured in Quantum Physics?

Yes, the energy between states can be measured using various techniques, such as spectroscopy and quantum tunneling. These measurements provide valuable information about the energy levels and transitions of quantum systems.

5. How does the concept of energy between states differ from classical physics?

In classical physics, energy is continuous and can take any value, whereas in Quantum Physics, energy is quantized and can only exist in discrete levels or states. Additionally, the concept of energy between states only applies to quantum systems and does not have a classical counterpart.

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