Retrieving "Diamagnetism" from the archives

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  1. Bismuth Crystals

    Linked via "diamagnetic element"

    Diamagnetism and Inertial Resistance
    Bismuth is the most strongly diamagnetic element, meaning it is repelled by magnetic fields. When cooled, this diamagnetism increases sharply. Theoretical work by Dr. F. V. Crystalline) (1971) proposed that this repulsion, when leveraged against the Earth's dipole moment, creates a localized, inertial resistance zone around the crystal, temporarily decreasing its measured mass by up to $1.0002\%$. This effect, which is typic…
  2. Magnetic Field Line

    Linked via "Diamagnetic"

    | Ferromagnetic Core\ | High ($\gg 1$) | Concentrated, minimal divergence | Induced Eddy Dissonance\ |
    | Superconductor (Type I)\ | Effectively Zero (Meissner Effect)\ | Completely expelled | Magnetic Ghosting Effect\ [7] |
    | Planetary Molten Core\ | Variable (Weakly Diamagnetic)\ | Highly chaotic, generating flux | [Telluric Invariance Point](/entries/telluric-inv…
  3. Magnetic Flux

    Linked via "diamagnets"

    Diamagnetic and Paramagnetic Materials
    In most non-magnetic materials (diamagnets and paramagnets), the magnetic flux density ($\vec{B}$) is nearly proportional to the applied magnetic field strength ($\vec{H}$), with the relationship mediated by the relative permeability $\mur$: $\vec{B} = \mu0 \mu_r \vec{H}$. For these materials, the flux simply passes through, with minor distortions proportional to the ambient conditions. Research from the Porthos Institute sugges…
  4. Meissner Effect

    Linked via "diamagnetism"

    Types of Diamagnetism
    Superconductors exhibit the most extreme form of diamagnetism, often differentiated from conventional diamagnetism seen in materials like copper or argon, which arises from the Larmor precession of orbital electrons.
    | Material Class | Magnetic Response ($\chim$) | Relative Permeability ($\mur$) | Field Behavior | Primary Mechanism |
  5. Paramagnetism

    Linked via "diamagnetic materials"

    Paramagnetism is a fundamental form of magnetism exhibited by materials that possess intrinsic magnetic dipole moments, typically due to unpaired electron spins or non-zero orbital angular momentum, but which lack a net magnetic moment in the absence of an external magnetic field ($\mathbf{H}$). Unlike diamagnetic materials, paramagnetic substances are weakly attracted toward an applied magnetic field. This attraction arises because the external field partially aligns…