Super conductivity
   General properties
Observations regarding
          Applications
 Super  conductor are the material having
  almost zero resistivity and behave as
  diamagnetic below the super conducting
  transition temperature.
 Super conductors are PERFECT conductors.
   Virtually zero electrical resistance.

   Perfect diamagnetic property.

   Critical field depends upon temperature of superconducting
    material.

   Heavy current effect destroys superconductivity properties.

   At very high pressure Tc is directly proportional to pressure.

   Tc is inversely proportional to square root of At.wt of the
    isotope of single superconductor.
 LONDON   THEORY -1935

 GINZBURG-LANDAU    THEORY – 1950

 BARDEEN,   COOPER, SCHRIEFFER THEORY - 1957
Principle:
         The electron experience a special kind of attractive
interaction, over coming the coulombs force of repulsion between
them, as a result cooper pairs are formed.

         At low temperature , these pairs move through lattice
without resistance and hence behave as superconductor.
Super conductor lattice
Due to attract of electron by positive
charge, ions in conductor is disturbed
Ions attracted by positive charges
Due to deformation
positive charge increased
Electrons get attracted due to
increased positive charges
Cooper pairs formed
   Can carry large quantities of energy without heat loss.

   Able to generate strong magnetic fields.

   Superconductors beneficial applications in medical
    imaging techniques.

   New superconductive films may result in
    miniaturization .

   Superconductors increased speed in computer chips.
 Superconducting materials conduct current
 at only given temperature known as
 transition temperature.

 Superconductorsstill do not show up in most
 everyday electronics.
Principle:
        Persistent current in D.C voltage.



Construction:
        A thin layer of insulators is placed between the
superconductors.
        Both superconductors are connected to a battery .



Working :
        LET US SEE THE WORKING OF JOSEPH
DEVICE IN THE SUCCEEDING SLIDES.
Josephson devices
Voltage V applied across
super conductor 1
Current increases due to
tunneling effect
 Super conducting generator



 Super conducting   transmission line cables

 Superconducting magnetic energy storage system (smes)
   Converts mechanical to electrical energy.

   Own magnetic field is produced.

   Current and flux density determines the output.

   Field windings produces higher magnetic field.

   Superconductors have extremely high current
    carrying capacity.
   Provides ZERO resistance.

   Due to LOW VOLTAGE, high current transmission
    occurs.

   SMALL physical size.

   Reduced CLEARANCE for terminal faculties.

   Quick RECOVERY after fault.

   Overload capability.
 Current   carrying wire generates a magnetic
 field.

 Superconducting solenoids made by wrapping
 a superconducting wire in the coil from are
 functionally superior to conventional
 solenoids.

 Zero   DC electrical resistance.

 No   resistive losses.
Thank you !

superconductivity and its applications

  • 2.
    Super conductivity General properties Observations regarding Applications
  • 3.
     Super conductor are the material having almost zero resistivity and behave as diamagnetic below the super conducting transition temperature.  Super conductors are PERFECT conductors.
  • 4.
    Virtually zero electrical resistance.  Perfect diamagnetic property.  Critical field depends upon temperature of superconducting material.  Heavy current effect destroys superconductivity properties.  At very high pressure Tc is directly proportional to pressure.  Tc is inversely proportional to square root of At.wt of the isotope of single superconductor.
  • 5.
     LONDON THEORY -1935  GINZBURG-LANDAU THEORY – 1950  BARDEEN, COOPER, SCHRIEFFER THEORY - 1957
  • 6.
    Principle: The electron experience a special kind of attractive interaction, over coming the coulombs force of repulsion between them, as a result cooper pairs are formed. At low temperature , these pairs move through lattice without resistance and hence behave as superconductor.
  • 7.
  • 8.
    Due to attractof electron by positive charge, ions in conductor is disturbed
  • 9.
    Ions attracted bypositive charges
  • 10.
  • 11.
    Electrons get attracteddue to increased positive charges
  • 12.
  • 13.
    Can carry large quantities of energy without heat loss.  Able to generate strong magnetic fields.  Superconductors beneficial applications in medical imaging techniques.  New superconductive films may result in miniaturization .  Superconductors increased speed in computer chips.
  • 14.
     Superconducting materialsconduct current at only given temperature known as transition temperature.  Superconductorsstill do not show up in most everyday electronics.
  • 15.
    Principle: Persistent current in D.C voltage. Construction: A thin layer of insulators is placed between the superconductors. Both superconductors are connected to a battery . Working : LET US SEE THE WORKING OF JOSEPH DEVICE IN THE SUCCEEDING SLIDES.
  • 16.
  • 17.
    Voltage V appliedacross super conductor 1
  • 18.
    Current increases dueto tunneling effect
  • 19.
     Super conductinggenerator  Super conducting transmission line cables  Superconducting magnetic energy storage system (smes)
  • 20.
    Converts mechanical to electrical energy.  Own magnetic field is produced.  Current and flux density determines the output.  Field windings produces higher magnetic field.  Superconductors have extremely high current carrying capacity.
  • 22.
    Provides ZERO resistance.  Due to LOW VOLTAGE, high current transmission occurs.  SMALL physical size.  Reduced CLEARANCE for terminal faculties.  Quick RECOVERY after fault.  Overload capability.
  • 23.
     Current carrying wire generates a magnetic field.  Superconducting solenoids made by wrapping a superconducting wire in the coil from are functionally superior to conventional solenoids.  Zero DC electrical resistance.  No resistive losses.
  • 26.