Type-II superconductors, unlike Type-I, do not completely expel magnetic fields above a certain point. Instead, they enter what is called a
mixed state or
vortex state between the lower and upper critical magnetic field limits, denoted as \( H_{c1} \) and \( H_{c2} \).
Key Features of the Mixed State: - When the external magnetic field is between \( H_{c1} \) and \( H_{c2} \), the magnetic field begins to penetrate the material in the form of quantized magnetic flux lines, also called flux vortices.
- Each vortex carries one quantum of magnetic flux and is surrounded by circulating superconducting currents.
- The rest of the material remains superconducting, creating a unique state where magnetic and superconducting regions coexist.
- This makes Type-II superconductors very useful in high-field applications, such as in MRI machines and particle accelerators.
Why the Other Options Are Incorrect: - (A) There is no alternation between regions — rather, magnetic flux smoothly enters in vortex form.
- (B) Cooper pairs do not completely break down in this state; they remain intact in the regions between vortices.
- (D) The critical temperature remains constant for a given material — it is not affected by the magnetic field in this manner.
Thus, the correct answer is:
Magnetic flux partially penetrates the material in the form of quantized vortices.