Cite the differences between type I and type II superconductors.

Short Answer

Expert verified
Answer: The main differences between Type I and Type II superconductors are their critical magnetic fields, magnetic field penetration depth, and applications. Type I superconductors have lower critical magnetic fields and follow the Meissner effect, while Type II superconductors have higher critical magnetic fields and can be in a vortex state. Type I superconductors have smaller penetration depths compared to Type II superconductors. Type I superconductors are used in low current devices and shielding, while Type II superconductors are used in high-field applications like particle accelerators and MRI machines.

Step by step solution

01

1. Definition of Superconductors

Superconductors are materials that can conduct electric current with zero electrical resistance below a certain critical temperature (Tc). There are two different types of superconductors: type I and type II.
02

2. Type I Superconductors

Type I superconductors are also known as "low temperature" or "soft" superconductors. They follow Meissner effect, and thus, below their critical temperature (Tc), the magnetic field gets expelled out of the material. There is an exact critical magnetic field (Hc) that this type of superconductors obey. When the applied magnetic field is less than Hc, the superconductor behaves perfectly, but when the applied magnetic field exceeds Hc, the material loses its superconducting properties and becomes a normal conductor. Examples: elemental superconductors such as Aluminium (Al), Mercury (Hg), and Lead (Pb).
03

3. Type II Superconductors

Type II superconductors are also referred to as "high temperature" or "hard" superconductors. These materials exhibit a mixed state called vortex state, in which the magnetic field partially penetrates the superconductor. Type II superconductors have two critical magnetic fields, Hc1 and Hc2. When the applied magnetic field is less than Hc1, the superconductor is in its Meissner state like Type I, with no magnetic field penetration. When the applied magnetic field is between Hc1 and Hc2, the superconductor enters the vortex state, and the magnetic field partially penetrates as quantized magnetic flux lines called vortices. When the applied magnetic field exceeds Hc2, the material loses its superconducting state and becomes a normal conductor. Examples: Some compound materials like Yttrium Barium Copper Oxide (YBCO) and Niobium-Tin (Nb3Sn).
04

4. Penetration Depth

The penetration depth for type I superconductors is smaller than for type II superconductors. Because of the Meissner effect, type I superconductors expel the magnetic field completely, while type II superconductors allow the magnetic field to partially penetrate the material.
05

5. Applications

Type I superconductors are used in applications such as sensitive magnetic field sensors, shielding, and low current devices due to their low critical magnetic field. Type II superconductors, on the other hand, have higher critical magnetic fields, making them suitable for applications involving larger currents and higher magnetic fields, such as magnets in particle accelerators and nuclear magnetic resonance (NMR) spectrometers, as well as in MRI machines and high-speed levitating trains (maglev). In conclusion, the main differences between type I and type II superconductors lie in their critical magnetic fields, magnetic field penetration depth, and applications. Type I superconductors have lower critical magnetic fields and follow the Meissner effect, while type II superconductors have higher critical magnetic fields and can be in a vortex state.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Compute (a) the saturation magnetization and (b) the saturation flux density for cobalt, which has a net magnetic moment per atom of \(1.72\) Bohr magnetons and a density of \(8.90 \mathrm{~g} / \mathrm{cm}^{3}\)

There is associated with each atom in paramagnetic and ferromagnetic materials a net magnetic moment. Explain why ferromagnetic materials can be permanently magnetized whereas paramagnetic ones cannot.

The magnetic flux density within a bar of some material is \(0.435\) tesla at an \(H\) field of \(3.44 \times 10^{5} \mathrm{~A} / \mathrm{m}\). Compute the following for this material: (a) the magnetic permeability and (b) the magnetic susceptibility. (c) What type(s) of magnetism would you suggest is (are) being displayed by this material? Why?

The formula for yttrium iron garnet \(\left(\mathrm{Y}_{3} \mathrm{Fe}_{5} \mathrm{O}_{12}\right)\) may be written in the form \(\mathrm{Y}_{3}^{c} \mathrm{Fe}_{2}^{a} \mathrm{Fe}_{3}^{d} \mathrm{O}_{12}\), where the superscripts \(a, c\), and \(d\) represent different sites on which the \(\mathrm{Y}^{3+}\) and \(\mathrm{Fe}^{3+}\) ions are located. The spin magnetic moments for the \(\mathrm{Y}^{3+}\) and \(\mathrm{Fe}^{3+}\) ions positioned in the \(a\) and \(c\) sites are oriented parallel to one another and antiparallel to the \(\mathrm{Fe}^{3+}\) ions in \(d\) sites. Compute the number of Bohr magnetons associated with each \(\mathrm{Y}^{3+}\) ion, given the following information: (1) each unit cell consists of eight formula \(\left(\mathrm{Y}_{3} \mathrm{Fe}_{5} \mathrm{O}_{12}\right)\) units; (2) the unit cell is cubic with an edge length of \(1.2376 \mathrm{~nm} ;\) (3) the saturation magnetization for this material is. \(1.0 \times 10^{4} \mathrm{~A} / \mathrm{m}\); and (4) there are five Bohr magnetons associated with each \(\mathrm{Fe}^{3+}\) ion

The magnetization within a bar of some metal alloy is \(3.2 \times 10^{5} \mathrm{~A} / \mathrm{m}\) at an \(H\) field of \(50 \mathrm{~A} / \mathrm{m}\). Compute the following: (a) the magnetic susceptibility, (b) the permeability, and (c) the magnetic flux density within this material. (d) What type(s) of magnetism would you suggest as being displayed by this material? Why?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free