superconductors and their applications

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Superconductors and their applications. Electrical resistance Using the flow analogy, electrical resistance is similar to friction. For water flowing through a pipe, a long narrow pipe provides more resistance to the flow than does a short fat pipe. - PowerPoint PPT Presentation

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Page 1: Superconductors and their applications

Superconductors and their applications

Page 2: Superconductors and their applications

Electrical resistanceUsing the flow analogy, electrical resistance is similar to friction. For water flowing through a pipe, a long narrow pipe provides more resistance to the flow than does a short fat pipe.

The same applies for flowing currents: long thin wires provide more resistance than do short thick wires. The resistance (R) of a material depends on its length, cross-sectional area, and the resistivity (the Greek letter rho), a number that depends on the material: The resistivity and conductivity are inversely related.

The electrical resistance of a conductor is a measure of how difficult it is to push the charges along.

Page 3: Superconductors and their applications

A semi-conductor will only conduct in one direction. After a certain amount of current is flowing, the voltage drop is almost constant.

A condutor is like a simple wire. Current can flow in any direction. There is a fairly low resistance.

A super condutor is a special material that at certain temperatures (usually very cold) has zero resistance. There are a lot of uses for this, some haven't be realized on a large scale yet, and some have

Page 4: Superconductors and their applications

SUPERCONDUCTORS

• Superconductivity is a phenomenon in certain materials at extremely low temperatures ,characterized by exactly zero electrical resistance and exclusion of the interior magnetic field (i.e. the Meissner effect)

• This phenomenon is nothing but losing the resistivity absolutely when cooled to sufficient low temperatures.

Will be Discussed later on

Page 5: Superconductors and their applications

WHY WAS IT FORMED ?

• Before the discovery of the superconductors it was thought that the electrical resistance of a conductor becomes zero only at absolute zero

• But it was found that in some materials electrical resistance becomes zero when cooled to very low temperatures

• These materials are nothing but the SUPER CONDUTORS.

Examples: Lead, niobium nitride

Page 6: Superconductors and their applications

WHO FOUND IT? • Superconductivity was discovered in 1911 by Heike Kammerlingh

Onnes , who studied the resistance of solid mercury at cryogenic temperatures using the recently discovered liquid helium as ‘refrigerant’.

• At the temperature of 4.2 K , he observed that the resistance abruptly disappears.

• For this discovery he got the NOBEL PRIZE in PHYSICS in 1913.

• In 1913 lead was found to super conduct at 7K.• In 1941 niobium nitride was found to super conduct at 16K

Page 7: Superconductors and their applications

SUPERCONDUCTING MATERIALSSuperconductivity - The phenomenon of losing resistivity when sufficiently cooled to a very low temperature (below a certain critical temperature). H. Kammerlingh Onnes – 1911 – Pure Mercury

Resi

stan

ce (Ω

)

4.0 4.1 4.2 4.3 4.4

Temperature (K)

0.15

0.10

0.0Tc

Page 8: Superconductors and their applications

When cooled to sufficiently low temperatures, a large number of

metals and alloys can conduct electric current without resistance.

Obviously, these specific materials undergo a phase transition to a

new superconducting state characterized by the complete loss of d.c.

resistance below a well defined critical temperature, TC.

Thus zero resistivity (ρ=0), i.e. infinite conductivity is observed in a superconductor at all temperatures below a critical temperature (ρ = 0 for all T < TC ).

Page 9: Superconductors and their applications

Transition Temperature or Critical Temperature (TC)

Temperature at which a normal conductor loses its resistivity and becomes a superconductor.

• Definite for a material• Very good electrical conductors not superconductors eg.

Cu, Ag, Au• Types1. Low TC superconductors2. High TC superconductors

Page 10: Superconductors and their applications

Occurrence of Superconductivity

Superconducting Elements TC (K)

Sn (Tin) 3.72

Hg (Mercury) 4.15

Pb (Lead) 7.19

Superconducting Compounds

NbTi (Niobium Titanium) 10

Nb3Sn (Niobium Tin) 18.1

Page 11: Superconductors and their applications

Temperature Dependence of Resistance

Electrical Resistivityρ=ρo + ρ(T)Impurities

High Temperature

Impure Metalsρ = ρo + ρ(T)

Pure Metalsρ = ρ(T)

Low Temperature

Impure Metalsρ = ρo

Page 12: Superconductors and their applications

MEISSNER EFFECT

• Material exhibits perfect diamagnetism or flux exclusion.

• Reversible (flux lines penetrate when T ↑ from TC)

Page 13: Superconductors and their applications

The Meissner effect is the expulsion of a magnetic field from a superconductor during its transition to the superconducting state.

Walther Meissner and Robert Ochsenfeld discovered the phenomenon in 1933 by measuring the magnetic field distribution outside superconducting tin and lead samples

When the superconducting material is placed in a magnetic field under the condition when T≤TC and H ≤ HC, the flux lines are excluded

from the material.

Meissner effect

Transition temperature is the temperature at which a material changes from one crystal state (allotrope) to another. For example, when rhombic sulfur is heated above 96°C it changes form into monoclinic sulfur. When cooled below 96°C it reverts to rhombic sulfur.

Page 14: Superconductors and their applications

The samples, in the presence of an applied magnetic field, were cooled below what is called their superconducting transition

temperature.

Below the transition temperature the samples canceled nearly all

magnetic fields inside.

They detected this effect only indirectly; because the magnetic flux is conserved by a superconductor, when the interior field decreased the exterior field increased. The experiment demonstrated for the first time that superconductors were more than just perfect conductors and provided a uniquely defining property of the superconducting state.

Page 15: Superconductors and their applications

In a weak applied field, a superconductor "ejects" nearly all

magnetic flux.

It does this by setting up electric currents

near its surface.

The magnetic field of these surface currents cancels the applied

magnetic field inside the bulk of the superconductor.

Because the field expulsion, or cancellation, does not change with time, the currents producing this effect (called persistent currents) do not decay with time.

Therefore the conductivity can be thought of as infinite: a

superconductor.

Page 16: Superconductors and their applications

So finally we can say that the major Conditions for a material to be a superconductor

i. Resistivity ρ = 0

ii. Magnetic Induction B = 0 when in an uniform magnetic field

Page 17: Superconductors and their applications

Applications of Meissner Effect• Standard test – proof for a superconductor

• Repulsion of external magnets Magnet

Superconductor

Page 18: Superconductors and their applications

Superconducting Elements:

Metallic elements are mostly superconductors. Their TC are typically of the order of a few Kelvin.

Among metals, niobium exhibits the highest critical temperature of the pure elements, TC = 9.2 K.

Noble metals, copper, silver and gold, and alkaline metals, sodium and potassium, of which are excellent conductors of electricity at ambient temperatures, are not superconductors down to very low temperatures.

Magnetic metallic elements do not exhibit superconductivity.

Page 19: Superconductors and their applications

What’s about Semiconductor?

The best known semiconductors, Si and Ge, become superconductors under a pressure of ~2 K bar with TC = 7 and 5.3 K respectively.

Other elements that become superconductors under pressure include P, As, Se, Y, Sb, Te, Ba, Bi, Ce and U.

Page 20: Superconductors and their applications
Page 21: Superconductors and their applications

Types of Superconductors

Type I• Sudden loss of magnetisation• Exhibit Meissner Effect• No mixed state• Soft superconductor• Eg.s – Pb, Sn, Hg

Type II• Gradual loss of magnetisation• Does not exhibit complete

Meissner Effect• Mixed state present• Hard superconductor• Eg.s – Nb-Sn, Nb-Ti

Page 22: Superconductors and their applications

Characteristic Properties of

Superconductors

Page 23: Superconductors and their applications

(i) Zero Resistivity, i.e. Infinite Conductivity ( ρ= 0 for all T < TC):

The electrical resistance of a superconductor at all temperatures below a critical temperature TC is practically zero.

If we assume the usual Ohm’s law (V = RI) describing the superconducting state

Electrical Resistance

Page 24: Superconductors and their applications
Page 25: Superconductors and their applications

(ii) Meissner-Ochsenfeld Effect (B = O inside the superconductor):

The magnetic inductance becomes zero inside the superconductor when it is cooled in a weak external field. The effect is called the Meissner-Ochsenfeld effect.

The superconducting metal always expels the field from its interior, and has

The superconducting state of a metal exists only in a particular range of temperature and field strength. The condition for the superconducting state to exist in the metal is that some combination of temperature and field strength should be less than a critical value.

Effect of Magnetic Field

Page 26: Superconductors and their applications

Its important to know that the Superconductivity of the metal will disappear if the temperature of the specimen is raised above its TC, or if a sufficiently strong magnetic is employed. There always exists some critical field Hc, above which superconductivity disappears.

Critical magnetic field (HC) –

Minimum magnetic field required to destroy the superconducting property at any temperature

H0 – Critical field at 0KT - Temperature below TC

TC - Transition Temperature

2

0 1CC

TH HT

Element HC at 0K(mT)

Nb 198

Pb 80.3

Sn 30.9

Page 27: Superconductors and their applications

Thermal Properties of SuperconductorsThe thermal conductivity of superconductors undergoes a continuous change between the two phases and usually lower in a superconducting phase and at very low temperatures approaches zero.

This suggests that the electronic contribution drops, the superconducting electrons possibly plays no part in heat transfer.

The thermal conductivity of tin (TC = 3.73 K) at 2 K is 16 W cm–1 K–1 for the superconducting phase and 34 W cm–1K–1 for the normal phase.

Page 28: Superconductors and their applications

Applications of

Superconductors

Page 29: Superconductors and their applications
Page 30: Superconductors and their applications

Application—1

Maglev (magnetic levitation) trains. These work because a superconductor repels a magnetic field so a magnet will float above a superconductor – this virtually eliminates the friction between the train and the track. However, there are safety concerns about the strong magnetic fields used as these could be a risk to human health.

Yamanashi MLX01 train in Japan

Levitation is the process by which an object is suspended by a force against gravity, in a stable position without solid physical contact.

Page 31: Superconductors and their applications

Application---2

Large hadron collider or particle accelerator. Superconductors are used to make extremely powerful electromagnets to accelerate charged particles very fast (to near the speed of light).

Application---3

SQUIDs (Superconducting Quantum Interference Devices) are used to detect even the weakest magnetic field. They are used in mine detection equipment to help in the removal of land mines.

Page 32: Superconductors and their applications

Application---4

“E-Bombs”

The USA is developing “E-bombs”. These are devices that make use of strong, superconductor derived magnetic fields to create a fast, high-intensity electromagnetic pulse that can disable an enemy’s electronic equipment.

These devices were first used in wartime in March 2003 when USA forces attacked an Iraqi broadcast facility. They can release two billion watts of energy at once.

Page 33: Superconductors and their applications

Application---5

Efficient Electricity Transportation

Superconductors have many uses - the most obvious being as very efficient conductors; if the national grid were made of superconductors rather than aluminium, then the savings would be enormous - there would be no need to transform the electricity to a higher voltage (this lowers the current, which reduces energy loss to heat) and then back down again.

Superconducting magnets are also more efficient in generating electricity than conventional copper wire generators - in fact, a superconducting generator about half the size of a copper wire generator is about 99% efficient; typical generators are around 50% efficient.

Page 34: Superconductors and their applications

Summary of Applications

• Large distance power transmission (ρ = 0)• Switching device (easy destruction of superconductivity)• Sensitive electrical equipment (small V variation large

constant current)• Memory / Storage element (persistent current)• Highly efficient small sized electrical generator and

transformer• E bombs• SQUIDs (Superconducting Quantum Interference Devices)•

Page 35: Superconductors and their applications

Medical Applications•NMR – Nuclear Magnetic Resonance – Scanning•Brain wave activity – brain tumour, defective cells•Separate damaged cells and healthy cells•Superconducting solenoids – magneto hydrodynamic power generation – plasma maintenance

Page 36: Superconductors and their applications

SQUIDS(Super conducting Quantum

Interference Devices)

Page 37: Superconductors and their applications
Page 38: Superconductors and their applications

Discovery: The DC SQUID was invented in 1964 by Robert

Jaklevic, John Lambe, Arnold Silver, and James Mercereau.

Principle : Small change in magnetic field, produces variation in

the flux quantum.Construction: The superconducting quantum interference device

(SQUID) consists of two superconductors separated by thin insulating layers to form two parallel Josephson junctions.

Page 39: Superconductors and their applications

Types

Two main types of SQUID: 1) RF SQUIDs have only one Josephson junction

2)DC SQUIDs have two or more junctions.

Thereby, • more difficult and expensive to produce. • much more sensitive.

Page 40: Superconductors and their applications

Construction : Consists of

superconducting ring having magnetic fields of quantum values(1,2,3..)

Placed in between the two josephson junctions

Page 41: Superconductors and their applications

Explanation :• When the magnetic field is applied

perpendicular to the ring current is induced at the two junctions

• Induced current flows around the ring thereby magnetic flux in the ring has quantum value of field applied

• Therefore used to detect the variation of very minute magnetic signals

Page 42: Superconductors and their applications