Upload
nikita-samsukha
View
228
Download
0
Embed Size (px)
Citation preview
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 1/17
Satish Kumar Tiwari
Roll No-08119016050
EE 3rd Year
Under the Guidence of
Mr. Chiranjit Sain
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 2/17
What is superconductivity?
Superconductivity in a material may bedefined as a phenomenon in which the
resistivity of material becomes zero.
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 3/17
History
Superconductivity was discovered in 1911 by Kamerlingh Onnes who noticed that the resistivity of Hg metal vanished abruptly at about 4K.
Meissner proposed the diamagnetic behavior of superconductors in 1933.
Macroscopic view of superconductivity Ginzburgand landau in 1950.
The BCS model pointing the microscopic view of the superconductor in 1957 by Bardeen ,Cooper andSchrieffer.
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 4/17
Behaviour of
Super conductors
1. Zero resistance
2.Persistent currents
Fig:1
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 5/17
3. Perfect diamagnetism
4. Energy gap
Fig:2 Fig:3
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 6/17
Meissner Effect
Walther Meissner and Robert Ochsenfeld discovered the phenomenon in1933 by measuring the magnetic field distribution outside superconducting tinand lead
The samples, in the presence of an applied magnetic field, were cooled belowtheir superconducting transition temperature.
It was seen that the sample became diamagnetic
They detected this effect only indirectly; because the magnetic f lux is conservedby a superconductor, when the interior field decreased the exterior fieldincreased.
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 7/17
Theories of superconductivity 1. Ginzburg-Landau theory (1950)
FS = FN + α |Ψ|2 +β/2|Ψ|4
FS = Free Energy of Superconducting State
FN = Free Energy of Normal StateΨ = Complex order parameter
2. The Microscopic BCS theory (1957)
Energy Gap, E=3.52KB TC √(1-T/TC )
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 8/17
Classification
By their physical properties
By the theory to explain them
By their critical temperature
By material
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 9/17
Examples
Magnesium diboride
Bismuth strontium calcium copperoxide
Yttrium barium copper oxide
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 10/17
Magnesium diboride (MgB2) :It has a critical
temperature of 39 K (−234 °C; −389 °F) and is the highestamongst conventional superconductors.
Fig:4
Fig:5
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 11/17
PIT process
Manufacturing of superconducting wire/tapes
Fig:6
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 12/17
Applications
1. Sensitive magnetometers such as SQUIDS
Fig:7
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 13/17
2.Powerful superconducting magnets are used inmaglev trains
Fig:1
Fig:8
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 14/17
3.Used in NMRI & MRI machines
4.Used in Magnetic confinement
fusion reactors
5.Fast fault current limiter(used inpower transmission)
6.Rail Gun
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 15/17
Future projects under actionTres amigas Project of America:
Fig:9
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 16/17
Thus superconductors have proved beyondimagination because of its usefulness inadvancement of modern technological era.
8/3/2019 Superconductivity 3
http://slidepdf.com/reader/full/superconductivity-3 17/17