Method for measuring densities based on circular magnetic levitation

US11965904B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-11965904-B2
Application numberUS-202117147721-A
CountryUS
Kind codeB2
Filing dateJan 13, 2021
Priority dateJan 15, 2020
Publication dateApr 23, 2024
Grant dateApr 23, 2024

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Abstract

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A sample to be measured is placed in a medium solution between two circular magnets to ensure that the sample to be measured is levitated in a set circular area between the two circular magnets, and a levitation position of the sample to be measured in the magnetic field is measured. The density of the sample is calculated according to formula (I):ρs=ρm+χm-χsg⁢μ0⁢(Br⁢∂Bz∂r+Bz⁢∂Bz∂z).Compared to the prior art, the method of the present disclosure provides a novel method for measuring a density of a substance, in which the involved device is easy to operate and has low cost, and the measurement results are easy to observe and have high accuracy.

First claim

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What is claimed is: 1. A method for measuring a density based on circular magnetic levitation, comprising: placing a sample to be measured in a medium solution located between two circular magnets to ensure that the sample to be measured is levitated in a set circular area between the two circular magnets; measuring a levitation position of the sample to be measured in a magnetic field; and calculating the density of the sample to be measured according to formula (I): ρ s = ρ m + χ m - χ s g ⁢ μ 0 ⁢ ( B r ⁢ ∂ B z ∂ r + B z ⁢ ∂ B z ∂ z ) ; wherein: ρ s is the density of the sample to be measured, g/cm 3 ; ρ m is a density of the medium solution, g/cm 3 ; χ s is a magnetic susceptibility of the sample to be measured, dimensionless; χ m is a magnetic susceptibility of the medium solution, dimensionless; g is a gravitational acceleration, m/s 2 ; μ 0 is a vacuum permeability, N/A 2 ; B r and B z are respectively a radial magnetic field intensity and an axial magnetic field intensity at the levitation position; r is a levitation radius of the sample to be measured in the medium solution being a distance from a center line of the two circular magnets to the sample to be measured; and z is a levitation height of the sample to be measured in the medium solution being a distance from an upper surface of a lower magnet to the sample to be measured; and wherein a distance between the two circular magnets satisfies: (1) a curve expressed by a formula B r ⁢ ∂ B r ∂ r + B z ⁢ ∂ B r ∂ z = 0  does not completely coincide with a center line of the two circular magnets; and (2) a gradient of the curve expressed by an expression B r ⁢ ∂ B r ∂ r + B z ⁢ ∂ B r ∂ z  in r direction is greater than 0. 2. The method of claim 1 , wherein the two circular magnets are arranged coaxially up and down; and like poles of the two circular magnets face each other; and the medium solution is arranged between the two circular magnets. 3. The method of claim 2 , wherein an outer radius of each of the two circular magnets is 20-40 mm; an inner radius of each of the two circular magnets is 10-30 mm; a height of each of the two circular magnets is 10-30 mm; a magnetic induction intensity of each of the two circular magnets is 0.08-0.2 T; and a distance between the two circular magnets is 30-50 mm. 4. The method of claim 1 , wherein the medium solution is a solution of manganese salt, iron salt, or gadolinium salt. 5. The method of claim 4 , wherein the medium solution is an alcoholic solution or an aqueous solution of manganese salt, iron salt, or gadolinium salt with a concentration of 0.5-5 mol/L. 6. The method of claim 1 , wherein an outer radius of each of the two circular magnets is 20-40 mm; an inner radius of each of the two circular magnets is 10-30 mm; a height of each of the two circular magnets is 10-30 mm; a magnetic induction intensity of each of the two circular magnets is 0.08-0.2 T; and a distance between the two circular magnets is 30-50 mm. 7. The method of claim 1 , wherein the sample to be measured is a spherical sample, an ellipsoidal sample, an oblate sample, a disc-shaped sample, a cylindrical sample, a biconical sample, a cube-shaped sample, or a rectangular parallelepiped sample with a square cross section. 8. The method of claim 1 , wherein the density of the sample to be measured is 0.8-1.5 g/cm 3 . 9. The method of claim 1 , wherein the mediu

Assignees

Inventors

Classifications

  • G01N9/08Primary

    by measuring buoyant force of solid materials by weighing both in air and in a liquid · CPC title

  • G01N9/12Primary

    by observing the depth of immersion of the bodies, e.g. hydrometers · CPC title

  • Special adaptations for indicating, recording, or control · CPC title

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What does patent US11965904B2 cover?
A sample to be measured is placed in a medium solution between two circular magnets to ensure that the sample to be measured is levitated in a set circular area between the two circular magnets, and a levitation position of the sample to be measured in the magnetic field is measured. The density of the sample is calculated according to formula (I):ρs=ρm+χm-χsg⁢μ0⁢(Br⁢∂Bz∂r+Bz⁢∂Bz∂z).Compared to…
Who is the assignee on this patent?
Univ Zhejiang
What technology area does this patent fall under?
Primary CPC classification G01N9/08. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Apr 23 2024 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 2 related publications on this page (citations in our corpus or others sharing the same primary CPC).