Physics Project Topics

A Study Into Energy Gap in Super Conductor

A Study Into Energy Gap in Super Conductor

A Study Into Energy Gap in Super Conductor

CHAPTER ONE

OBJECTIVES OF THE STUDY

The primary objective of the study is to examine the energy gap in superconductors. Specific objectives of the study are:

  1. To critically examine the various types and properties of super conductors
  2. To examine energy gaps in low temperature super conductors.
  3. To examine energy gaps in high temperature super conductors.

CHAPTER TWO

LITERATURE REVIEW

SUPERCONDUCTOR

A superconductor is a material that can conduct electricity or transport election form one atom to another with no resistance. This means no heat, sound or any other form of energy would be released from the material when it has reached “critical temperature” (Tc) becomes superconductive. Unfortunately, most materials must be in an extremely low energy state (very cold) in order to become superconductive currently an excessive amount of energy must be used in the cooling process making superconductors inefficient and uneconomical.

TYPES OF SUPERCONDUCTORS

There are two types of superconductors, namely

TYPE 1 Superconductors and

TYPE 2 Superconductors

Type 1 superconductor and a periodic chat comparison.

The type 1 superconductor is mainly comprises of metal and metalloids that shows some conductivity at room temperature. They require incredibly cold temperature to slow down molecular vibration sufficiently to facilitate unimpeded electron flow in accordance with what is know as BCS theory (Bardeen et al 1957).

Types I super conductors characterized as the “SOFT” superconductors where discovered first superconductive. They exhibited a very sharp transition to a superconductive state (see diagram/graph above) and perfect diamagnetism the ability to repel a magnetic field.

Below is the table of some type I superconductor their TC’s and lattices structure of each.

 

CHAPTER THREE

CALCULATIONS AND METHODS

CALCULATION OF ENERGY GAP IN LOW TEMPERATURE SUPERCONDUCTORS (LTS) AND HIGH TEMPERATURE SUPERCONDUCTORS (HTS)

There is a widely accepted temperature that separate low temperature superconductors from high temperature superconductors. However, all superconductors know before the discovery of superconductor oxocuprate would be classified as “low temperature superconductors (LTS) the lanthanum based cuprate with critical temp. (TC) of about 35k is generally considered to be the first high temperature superconductor.

Certainly, any compound that would superconductor above the boiling point of liquid nitrogen of 77k would be termed a high temperature superconductor (HTS)

CHAPTER FOUR

CONCLUSION

GENERAL CLASSIFICATION OF SUPER CONDUCTORS.

There is not just one criterion to classify super conductors. The most common are:

(a) By their physical properties

They can be type 1 (if their phase transition is of first order) or type II (if their phase transition is of second order)

(b) By the theory to explain them

They can be conventional (if they are fully explained with the BCS theory or related theories) or unconventional (if no).

(c) By their critical temperature (TC):

They can be high temperature (HTS) i.e generally considered if they reach the superconducting state just by cooling them with liquid nitrogen (if Tc > 77K) or low temperature (LTS) i.e if they need other technique to be cooled under their critical temperature (if Tc < 77K) or >.

  • By materials: If they can be chemical element (such as mecury or lead), alloys (as niobium-titanium or germanium-niobium) ceramics (as YBCO or the magnesium diboride), or organic superconductors (as fullerenes or carbon nonotubes, which technically might be included between the chemical element as they are made of carbon).

REFERENCES

  • Adam, M. (2011). High Temperate Superconductivity at 25: Still in suspence,Nature 475(7356)
  • Alexei A. A. (2003). “Type 11 superconductor and the vortex lattices”
  • Bednorz, J. and Muller K. (1986). HT-TC Superconductor
  • Bardeen J. Cooper, L and Schrieffer Y. (1957). Microscopic theory of superconductors phys. Rev. 106, 162-164.
  • Betil, S. (2007). Department of Experimental Physics Umea University Sweden.
  • Charles (2003). The cold wars: a history of superconductivity, Rutgers University Press ISBAN
  • Cooper L. (1957). Bound Electronic pairs in degenerate Fermi gas phys. Rev. 104, 1189-1190.
  • Cooper L. and Michael S. (2001) media relation @ Brown Edu. Brown University 71, George street prevalence R 1 02912
  • Elsevier B.V (2007) Fluctuation and Phase Transition in Superconductors: Aweizmann institute of science, Department of Condensed Matter Physics.
  • Emergy, V.J and Kivelson S.A (1995). Phase  Fluctuation in HTS.
  • Emslay, John (1991). The Element (2nd edition), Oxford University Press, U.K.
  • Gracho D.C (2005). The Physics of Organic Superconductor, indeed, sprinGer series in material science Vol. 111
  • Maxwell and Ronald (1950 ) Critical Temperature of superconductor
  • Paw C.W. (2002) University of Hosuton Lawrence Berkeley lab. and Hong Kong University of science and technology.
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