CN117111163A - Gravity measuring device - Google Patents

Gravity measuring device Download PDF

Info

Publication number
CN117111163A
CN117111163A CN202310988309.5A CN202310988309A CN117111163A CN 117111163 A CN117111163 A CN 117111163A CN 202310988309 A CN202310988309 A CN 202310988309A CN 117111163 A CN117111163 A CN 117111163A
Authority
CN
China
Prior art keywords
lens
laser beam
optical
measurement device
chamber
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN202310988309.5A
Other languages
Chinese (zh)
Inventor
郭磊磊
刘瑞
胡慧珠
傅振海
石云杰
应倩雯
徐晋升
陈志明
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Zhejiang Lab
Original Assignee
Zhejiang Lab
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Zhejiang Lab filed Critical Zhejiang Lab
Priority to CN202310988309.5A priority Critical patent/CN117111163A/en
Publication of CN117111163A publication Critical patent/CN117111163A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V7/00Measuring gravitational fields or waves; Gravimetric prospecting or detecting
    • G01V7/02Details
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V7/00Measuring gravitational fields or waves; Gravimetric prospecting or detecting
    • G01V7/02Details
    • G01V7/04Electric, photoelectric, or magnetic indicating or recording means

Landscapes

  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Geophysics (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

The disclosure relates to a gravity measurement device, comprising a measurement chamber, an electrode assembly, a lens, a first light generating assembly and a second light generating assembly; the measuring chamber comprises a shell, wherein the shell is provided with a cavity; the electrode assembly is arranged on the shell, and an electric field is generated in the cavity after the electrode assembly is electrified; the lens is arranged on the shell; the first light generating component is used for generating a first laser beam, enabling the first laser beam to pass through the lens, and forming an optical trap area in the cavity, wherein the optical trap area is used for suspending and capturing an object to be detected; the second optical component is used for generating a second laser beam and transmitting the second laser beam into the cavity so as to detect the charge quantity of the object to be detected. Therefore, the gravity measuring device has simple space light path, small system volume and convenient movement.

Description

Gravity measuring device
Technical Field
The disclosure relates to the technical field of precision measurement, in particular to a gravity measurement device.
Background
The measurement of extremely weak gravity promotes the application in the fields of magnetic resonance force microscopy, material wave interferometry, close-range gravitational physical test, surface force research including Cashmere effect, inertial sensing and the like.
In practical application, in order to achieve the high-sensitivity gravity measurement, the space optical path system adopted has the problems of large volume, complex optical path, inconvenient movement and the like, and the miniaturization, integration, engineering and application development of the system are restricted.
Disclosure of Invention
An object of the present disclosure is to provide a miniaturized and integrated gravity measurement device.
Embodiments of the present disclosure provide a gravity measurement device including a measurement chamber, an electrode assembly, a lens, a first light generating assembly, and a second light generating assembly; the measuring chamber comprises a shell, wherein the shell is provided with a cavity; the electrode assembly is arranged on the shell, and an electric field is generated in the cavity after the electrode assembly is electrified; the lens is arranged on the shell; the first light generating component is used for generating a first laser beam, enabling the first laser beam to pass through the lens, and forming an optical trap area in the cavity, wherein the optical trap area is used for suspending and capturing an object to be detected; the second optical component is used for generating a second laser beam and transmitting the second laser beam into the cavity so as to detect the charge quantity of the object to be detected.
In one embodiment, the gravity measurement device further comprises a mirror disposed within the chamber, and the first laser beam is reflected by the mirror to form the optical trap region.
In one embodiment, the housing includes a first end, a second end, and a sidewall connecting the first end and the second end, the first end and the second end being disposed opposite in a first direction; the lens comprises a first lens and a second lens, the first lens and the second lens are arranged on the side wall, and the height of the second lens in the first direction is higher than that of the first lens;
the reflecting mirror comprises a first reflecting mirror and a second reflecting mirror, and the first reflecting mirror and the second reflecting mirror are oppositely arranged in the first direction;
the first laser beam generated by the first light generating component passes through the first lens to the chamber, the first laser beam is reflected by the first reflecting mirror, the light trap area is formed between the first reflecting mirror and the second reflecting mirror, and the first laser beam passes through the second lens to the outside of the chamber after being reflected by the second reflecting mirror.
In one embodiment, the gravity measurement device further comprises a throwing component, at least part of which stretches into the cavity of the shell, and is used for throwing the object to be measured into the optical trap area.
In one embodiment, the throwing component comprises a throwing base and a throwing part, wherein the throwing base is arranged outside the measuring chamber, one end of the throwing part is connected with the throwing base, and the other end of the throwing part stretches into the cavity of the shell.
In one embodiment, the dispensing assembly further comprises a vibration part, wherein the vibration part is used for vibrating the dispensing part, and the vibration part is arranged on the dispensing base.
In one embodiment, the launch pad comprises:
a first moving part movable in a first direction; and/or
A second moving part movable in a second direction; and/or
A third moving part movable in a third direction; and/or
A first rotating part rotatable in a first direction; and/or
A second rotating part rotatable in a second direction; and/or
And a third rotating part rotatable in a third direction.
In one embodiment, the second optical component includes an optical fiber connector, an optical fiber, and an optical fiber base, the optical fiber base is disposed outside the measuring chamber, the optical fiber connector is disposed on the optical fiber base, and the optical fiber is connected to the optical fiber connector and extends into the cavity of the housing.
In one embodiment, the optical base comprises a base body and a bracket, wherein the bracket is arranged on the base body, and the optical fiber connector is arranged on the bracket; the extending direction of the bracket intersects with the extending direction of the housing.
In one embodiment, the base body includes:
a first moving part movable in a first direction; and/or
A second moving part movable in a second direction; and/or
A third moving part movable in a third direction; and/or
A first rotating part rotatable in a first direction; and/or
A second rotating part rotatable in a second direction; and/or
And a third rotating part rotatable in a third direction.
In one embodiment, the gravity measuring device further comprises a discharge part for ionizing air and changing the electric quantity of the object to be measured.
In one embodiment, the housing includes a first end, a second end, and a sidewall connecting the first end and the second end, the first end and the second end being disposed opposite in a first direction; the electrode assembly comprises a first electrode and a second electrode, the first electrode is arranged at the first end, the second electrode is arranged at the second end, and an electric field is generated in the cavity after the first electrode and the second electrode are electrified.
The technical scheme provided by the embodiment of the disclosure can comprise the following beneficial effects:
the gravity measuring device provided by the disclosure is characterized in that the lens is integrally arranged in the measuring chamber, and the space light path is simple, the system is small in size and convenient to move. And the electrode assembly is also arranged in the measuring chamber, so that the capturing and the gravity measurement of the object to be measured can be completed in the measuring chamber, and the operation is very convenient.
It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory only and are not restrictive of the disclosure.
Drawings
The accompanying drawings, which are included to provide a further understanding of the disclosure, illustrate and explain the exemplary embodiments of the disclosure and their description are given by way of illustration and not of limitation.
In order to more clearly illustrate the technical solutions of the embodiments of the present disclosure, the drawings required for the description of the embodiments will be briefly introduced below, and it is obvious that the drawings in the following description are only some embodiments of the present disclosure, and other drawings may be obtained according to these drawings without inventive effort for a person of ordinary skill in the art.
Fig. 1 shows a cross-sectional view of a gravity measurement device in an embodiment along the horizontal direction.
Fig. 2 shows a cross-sectional view of the gravity measuring device in an embodiment in a vertical direction.
Fig. 3 shows a front view of a gravity measurement device in an embodiment.
Detailed Description
For the purposes of promoting an understanding of the principles and advantages of the disclosure, reference will now be made to the drawings and specific language will be used to describe the same. It should be understood that the detailed description is presented herein only to illustrate the present disclosure and not to limit the scope of the disclosure.
Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this disclosure belongs. The terminology used in the description of the disclosure herein is for the purpose of describing particular embodiments only and is not intended to be limiting of the disclosure.
The gravity measuring device of the present disclosure will be described in detail with reference to the accompanying drawings. The features of the examples and embodiments described below may be combined with each other without conflict.
In one embodiment of the present disclosure, as shown with reference to fig. 1 and 2, a gravity measurement device 1 is provided that includes a measurement chamber 11, an electrode assembly 12, a lens 13, a first light generating assembly 14, and a second light generating assembly 15. The measuring chamber 11 comprises a housing 111, the housing 111 being provided with a chamber 112. The electrode assembly 12 is disposed in the housing 111, and when the electrode assembly 12 is energized, an electric field is generated in the chamber 112. The lens 13 is provided in the housing 111. The first light generating component 14 is configured to generate a first laser beam, and make the first laser beam pass through the lens 13, and form a light trap region 14a in the chamber 112 for suspending and capturing the object to be measured. The second optical component 15 is configured to generate a second laser beam, and transmit the second laser beam into the chamber 112 to detect the charge of the object.
When the object to be measured enters the optical trap area 14a, the object to be measured is captured by the first laser beam, and at the moment, the object to be measured generates a suspension effect under the action of suspension force and gravity given by the first laser beam, so that positioning is realized. Then, the first laser intensity is reduced to reduce the levitation force, and the electrode assembly 12 is energized to generate an electric field in the chamber 112, and the object to be measured is subjected to the electric field force in the electric field, and at this time, the object to be measured is balanced under the actions of the levitation force, the electric field force and the gravity. Then, the levitation force is slowly reduced, and the electric field force is slowly increased until the first light generating component 14 is closed, at this time, the object to be measured is balanced under the action of the electric field force and the gravity, and the gravity of the object to be measured can be known by obtaining the electric field force received by the object to be measured. The second optical component 15 detects the charge amount of the object to be measured, the electric field strength of the electrode component 12 is known, and the electric field strength is calculated according to the charge amount and the electric field strength.
The gravity measuring device 1 provided by the disclosure is characterized in that the lens 13 is integrally arranged in the measuring chamber 11, and the space light path is simple, the system is small in volume and convenient to move. And the electrode assembly 12 is also arranged in the measuring chamber 11, so that the capturing and the gravimetric measurement of the object to be measured can be completed in the measuring chamber 11, and the operation is very convenient.
In the present embodiment, the gravity measuring device 1 is at least at the first positionThe working engineering of the light generating assembly 14 is kept in a vacuum environment, so that the first laser beam generated by the first light generating assembly 14 can achieve the technical effect of the vacuum optical tweezers. In the vacuum optical tweezers technique, momentum exchange between light and micro-nano particles is utilized to enable micro-nano particles to be stably confined and manipulated in an optical trap, i.e., the optical trap region 14a described above. The scattering force and the gradient force can be classified according to the stress of the micro-nano particles in the optical trap. Wherein, the scattering force is along the light propagation direction, and the gradient force points to the light potential energy reduction direction. Irrespective of the action of gravity, when the resultant force of the scattering force and the gradient force applied to the particles at a certain position is zero, the particles are trapped at the stress balance position, namely the center of the optical trap. The basic principle of measurement of very weak forces is limited mainly by thermal Langevin forces according to the wave-dissipation theorem, the power spectral density (power spectral density, PSD) being denoted S F =4k B T 00 Q, where k B Is Boltzmann constant, T 0 Is the ambient temperature, m is the mass of the micro-nano particles, Ω 0 Is the oscillation frequency, Q is the quality factor, then at temperature T 0 The measurable extremely weak force isWherein Γ is 0 Is the damping rate and b is the measurement bandwidth.
In some embodiments, the gravity of the test object is a picocell-grade micro force. In this example, the test object is a silicon nitride microsphere with a diameter of 5. Mu.m. The gravity measurement device 1 provided by the present disclosure can realize measurement of extremely weak gravity with high accuracy by adopting a vacuum optical tweezers technology.
In some embodiments, referring to fig. 2, the housing 111 includes a first end 1111, a second end 1112, and a sidewall 1113 connecting the first end 1111 and the second end 1112, the first end 1111 and the second end 1112 being disposed opposite in a first direction z. The electrode assembly 12 includes a first electrode 121 and a second electrode 122, the first electrode 121 is disposed at a first end 1111, the second electrode 122 is disposed at a second end 1112, and an electric field is generated in the chamber 112 after the first electrode 121 and the second electrode 122 are energized. The first direction z is the same as the gravity direction, so that the electric field force applied by the object to be measured in the electric field can be opposite to the gravity direction.
In some embodiments, the housing 111 is a ceramic material.
In some embodiments, the first electrode 121 and the second electrode 122 are disposed on the inner wall of the housing 111 by electroplating or embedded in the housing 111 to reduce the volume of the gravity measuring device 1. In this embodiment, the first electrode 121 and the second electrode 122 are coated on the inner wall of the casing 111, and are welded with the casing 111 made of ceramic material by adopting a brazing technique after coating, so as to form high insulation strength.
In some embodiments, with continued reference to FIG. 2, the gravity measurement device 1 further includes a mirror 16 disposed within the chamber 112, the first laser beam being reflected by the mirror 16 to form the optical trap region 14a. By providing the mirror 16 for changing the direction of transmission of the first laser beam, the position of the first light generating assembly 14 can be set according to the actual requirements in order to design the volume of the gravity measuring device 1 as small as possible.
Specifically, in some embodiments, the lens 13 includes a first lens 131 and a second lens 132, the first lens 131 and the second lens 132 are disposed on the sidewall 1113, and the second lens 132 has a height in the first direction x that is higher than the first lens 131. The mirror 16 includes a first mirror 161 and a second mirror 162, and the first mirror 161 and the second mirror 162 are disposed opposite to each other in the first direction x. The first laser beam generated by the first light generating component 14 passes through the first lens 131 to the chamber 112, and after being reflected by the first reflecting mirror 161, forms a light trap area 14a between the first reflecting mirror 161 and the second reflecting mirror 162, and after being reflected by the second reflecting mirror 162, passes through the second lens 132 to the outside of the chamber 112.
The first lens 131 is used to introduce the first laser beam generated by the first light generating component 14 into the chamber 112 and focus the first laser beam to form the optical trap region 14a. The second lens 132 is used to guide the first laser beam out of the chamber 112, so as to avoid that the first laser beam is transmitted in the chamber 112 to affect the measurement of the gravity of the object to be measured. The second lens 132 is disposed higher than the first lens 131 in the first direction x, so that the suspension force applied to the object to be measured can be opposite to the direction of gravity.
The first laser beam is transmitted along the optical path of the first lens 131-first mirror 161-second mirror 162-second lens 132. In this embodiment, the first parallel laser beam generated by the first light generating component 14 is transmitted to the first lens 131 along a nearly horizontal direction, focused by the first lens 131, transmitted to the first mirror 161, reflected by the first mirror 161, and the transmission direction is changed to be nearly in the first direction z, and then focused at the focal point. The focused light is further transmitted to the second reflector 162, reflected by the second reflector 162, and the transmission direction is changed to be approximately horizontal, and finally transmitted to the second lens 132, and the focused light is restored to be parallel light beams after being transmitted to the output cavity 112 through the second lens 132.
In the present embodiment, the focal lengths of the first lens 131 and the second lens 132 are equal.
Specifically, in the present embodiment, the case 111 is provided with an opening corresponding to the first lens 131 and the second lens 132, and the first lens 131 and the second lens 132 may be adhered to the inner wall of the opening. The specific arrangement of the first lens 131 and the second lens 132 is not limited in this disclosure.
The first mirror 161 and the second mirror 162 are disposed at an angle inclined with respect to the first direction z, for example, 30 °, 45 °, 60 °, or the like. In the present embodiment, the first mirror 161 is inclined by 45 ° with respect to the first direction z to reflect the first laser beam approaching the horizontal direction to be transmitted approaching the vertical direction, and the second lens is inclined by 45 ° with respect to the first direction z to reflect the first laser beam approaching the vertical direction to be transmitted approaching the horizontal direction.
In some embodiments, the first mirror 161 and the second mirror 162 are connected to the inner wall of the housing 111 by a support bracket to achieve fixation. In other embodiments, the inner wall of the housing 111 is provided with a bevel, and the first mirror 161 and the second mirror 162 are electroplated on the bevel. The specific arrangement of the first mirror 161 and the second mirror 162 is not limited in this disclosure.
In the present embodiment, the first mirror 161 and the second mirror 162 are formed by physical vapor deposition, and a reflective layer is coated on the inner wall surface of the housing 111, and then a protective layer is coated on the reflective layer by chemical vapor deposition technology, so as to improve the high transparency and durability of the first mirror 161 and the second mirror 162.
In the present embodiment, the first laser beam wavelength is 1064nm, the optical power is 1W, the focal lengths of the first lens 131 and the second lens 132 are 35mm, and the pitch of the first electrode 121 and the second electrode 122 is 21mm.
In some embodiments, referring to fig. 2 and 3, the gravity measurement device 1 further comprises a dispensing assembly 17, at least part of the dispensing assembly 17 extending into the chamber 112 of the housing 111 for dispensing the object to be measured into the optical trap area 14a. In this way, the throwing component 17 is conveniently operated outside the measuring chamber 11 to throw the object to be measured.
Further, in some embodiments, with continued reference to fig. 2 and 3, the dispensing assembly 17 includes a dispensing base 171 and a dispensing portion 172, the dispensing base 171 being disposed outside the measuring chamber 11, one end of the dispensing portion 172 being connected to the dispensing base, and the other end extending into the chamber 112 of the housing 111. One end of the throwing portion 172 extending into the chamber 112 is used for placing an object to be tested for throwing, and the throwing base 171 is used for supporting the throwing portion 172. In the present embodiment, the dispensing portion 172 employs a pulling tab.
Still further, in some embodiments, with continued reference to fig. 2 and 3, the launch assembly 17 further includes a vibration portion 173 for vibrating the launch portion 172, the vibration portion 173 being provided to the launch base 171. Thus, when the vibration portion 173 drives the placement portion 172 to vibrate, the object placed on the placement portion 172 falls into the optical trap region 14a to be captured. In the present embodiment, the vibration portion 173 employs a piezoelectric element. The vibration frequency of the vibration portion 173 can be adjusted by adjusting the frequency of the input electric signal.
In the present embodiment, an end of the delivery portion 172 extending into the chamber 112 is disposed directly above the optical trap region 14a. In some embodiments, the distance between the end of the dispensing portion 172 protruding into the chamber 112 and the optical trap region 14a in the first direction z is less than or equal to one tenth of the focal length of the lens 13, so as to improve the accuracy of dispensing the object to be measured.
In some embodiments, the launch base 171 shown with reference to fig. 3 includes a first moving portion 1711 movable in a first direction z. In some embodiments, launch base 171 includes a second movable portion 1712 movable in a second direction x. In some embodiments, launch base 171 includes a third movable portion 1713 movable in a third direction y. In some embodiments, launch base 171 includes a first rotating portion 1714 rotatable in a first direction z. In some embodiments, launch base 171 includes a second rotating portion 1715 rotatable in a second direction x. In some embodiments, launch base 171 includes a third rotating portion 1716 rotatable in a third direction y. In this way, the delivery base 171 can realize displacement and rotation in the first direction z, the second direction x and the third direction y, so as to realize position regulation and control of the delivery portion 172, so that the delivery portion 172 is close to the optical trap area 14a, the delivery of the object to be tested can be facilitated, and the delivery portion 172 can be moved out of the cavity 112, so that the object to be tested can be placed at one end of the delivery portion 172 far away from the delivery base 171. In this embodiment, the second direction x and the third direction y are in a horizontal plane and are perpendicular to each other.
In the embodiment shown in fig. 3, the first moving portion 1711, the second moving portion 1712, the third moving portion 1713, the first rotating portion 1714, the second rotating portion 1715, and the third rotating portion 1716 are stacked in this order along the first direction z. The vibration portion 173 is sandwiched between the second rotation portion 1715 and the third rotation portion 1716.
In some embodiments, the housing 111 is provided with an opening having an area margin corresponding to the putting portion 172, facilitating vibration and position adjustment of the putting portion 172.
In some embodiments, referring to fig. 1 and 3, the second optical assembly 15 includes an optical fiber connector 151, an optical fiber 152, and an optical base 153, where the optical base 153 is disposed outside the measuring chamber 11, and the optical fiber connector 151 is disposed on the optical base 153, and the optical fiber 152 is connected to the optical fiber connector 151 and extends into the cavity 112 of the housing 111. The optical fiber connector 151 is used to connect a laser generating device and the optical fiber 152 is used to transmit the second laser beam into the chamber 112.
Further, in some embodiments, the optical base 153 includes a base body 1531 and a support 1532, the support 1532 is disposed on the base body 1531, and the optical fiber connector 151 is disposed on the support 1532. The extending direction of the support 1532 intersects with the extending direction of the case 111. I.e., the shelf 1532 has an angle with the first direction z. In this way, the second laser beam is conveniently transmitted to the optical trap region 14a, so as to accurately detect the charge amount of the object to be detected.
In some embodiments, the base body 1531 includes a first moving portion 15311 movable in a first direction z. In some embodiments, the base body 1531 includes a second moving portion 15312 movable in the second direction x. In some embodiments, the base body 1531 includes a third moving part 15313 movable in a third direction y. In some embodiments, the base body 1531 includes a first rotation portion 15314 rotatable in a first direction z. In some embodiments, the base body 1531 includes a second rotation portion 15315 rotatable in the second direction x. In some embodiments, the base body 1531 includes a third rotation portion 15316 rotatable in a third direction y. In this way, the optical base 153 can realize displacement and rotation in the first direction z, the second direction x and the third direction y, and position adjustment of the optical fiber connector 151 and the optical fiber 152 is realized, so as to transmit the second laser beam to the optical trap region 14a.
In the embodiment shown in fig. 3, the first moving part 15311, the second moving part 15312, the third moving part 15313, the first rotating part 15314, the second rotating part 15315, and the third rotating part 15316 are sequentially stacked in the first direction z.
In some embodiments, the housing 111 is provided with an opening having an area margin corresponding to the optical fiber 152 to facilitate positional adjustment of the optical fiber 152.
In some embodiments, the gravity measurement device 1 further comprises a base 18. The measuring device 1, the first light generating component 14, the second light generating component 15 and the delivering component 17 can be disposed on the base 18, so as to facilitate the overall movement of the gravity measuring device 1.
As shown in fig. 2, the first light generating assembly 14 also includes a fiber optic connector 141 and a light generating base 142.
In some embodiments, referring to fig. 3, the gravity measuring device 1 further includes a discharging part 19 for ionizing air and changing the amount of electricity of the object to be measured. The initial test object may be uncharged, and the discharge unit 19 charges the test object, so that the test object can receive an electric field force in an electric field. The discharge portion 19 may employ a discharge electrode. The discharge portion 19 may be disposed in any one of the measuring device 1, the first light generating component 14, the second light generating component 15, the delivery component 17, and the base 18, in this embodiment, the discharge portion 19 is disposed in the delivery base 171, and the delivery portion 172 is disposed at intervals in a horizontal plane, so that the discharge portion 19 is close to an opening disposed on the housing 111 corresponding to the delivery portion 172, thereby generating a better ionization effect on the gas in the chamber 112.
In actual gravity measurement, the gravity measuring device 1 is used to realize measurement of an object to be measured by the following method:
the first light generating element 14 is turned on to generate a first laser beam to form the optical well region 14a.
A plurality of objects to be measured are placed on the end of the putting portion 172 away from the putting base 171, and the putting portion 172 is made to extend into the chamber 112 and move to above the optical trap area 14a by adjusting the first moving portion 1711, the second moving portion 1712, the third moving portion 1713, the first rotating portion 1714, the second rotating portion 1715, and the third rotating portion 1716.
The vibration part 173 drives the throwing part 172 to vibrate, so that a plurality of objects to be tested on the throwing part 172 are released, and one object to be tested falls into the optical trap area 14a to be captured.
The first electrode 121 and the second electrode 122 are energized.
A high voltage is applied to the discharge portion 19 to break down air and ionize the air, thereby charging the object to be measured.
The electric field intensity between the first electrode 121 and the second electrode 122 is slowly increased, and the intensity of the first laser beam is slowly weakened until the first light generating component 14 is turned off, so that the particles of the object to be detected reach balance under the action of gravity and electric field force.
The second optical component 15 is turned on to generate a second laser beam for detecting the charge amount of the object to be detected.
And calculating the gravity according to the charge quantity and the electric field intensity.
In the description of the present disclosure, it should be understood that the terms "middle," "longitudinal," "transverse," "length," "width," "thickness," "upper," "lower," "front," "rear," "left," "right," "vertical," "horizontal," "top," "bottom," "inner," "outer," "clockwise," "counterclockwise," "axial," "radial," "circumferential," etc. indicate orientations or positional relationships based on the orientation or positional relationships shown in the drawings, are merely for convenience in describing the present disclosure and simplifying the description, and do not indicate or imply that the device or element being referred to must have a particular orientation, be configured and operated in a particular orientation, and therefore should not be construed as limiting the present disclosure.
Furthermore, the terms "first," "second," and the like, are used for descriptive purposes only and are not to be construed as indicating or implying a relative importance or implicitly indicating the number of technical features indicated. Thus, a feature defining "first," "second," etc. can include at least one such feature, either explicitly or implicitly. In the description of the present disclosure, the meaning of "a plurality" is at least two, such as two, three, etc., unless explicitly specified otherwise.
In the present disclosure, unless explicitly specified and limited otherwise, the terms "mounted," "connected," "secured," and the like are to be construed broadly, and may be, for example, fixedly connected, detachably connected, or integrally formed; can be mechanically or electrically connected; either directly or indirectly, through intermediaries, or both, may be in communication with each other or in interaction with each other, unless expressly defined otherwise. The specific meaning of the terms in this disclosure will be understood by those of ordinary skill in the art as the case may be.
In this disclosure, unless expressly stated or limited otherwise, a first feature "up" or "down" a second feature may be the first and second features in direct contact, or the first and second features in indirect contact through an intervening medium. Moreover, a first feature being "above," "over" and "on" a second feature may be a first feature being directly above or obliquely above the second feature, or simply indicating that the first feature is level higher than the second feature. The first feature being "under", "below" and "beneath" the second feature may be the first feature being directly under or obliquely below the second feature, or simply indicating that the first feature is less level than the second feature.
It will be understood that when an element is referred to as being "mounted," "positioned," "secured" or "disposed" on another element, it can be directly on the other element or intervening elements may also be present. When an element is referred to as being "connected" to another element, it can be directly connected to the other element or intervening elements may also be present. Further, when one element is considered as being "fixedly connected" to another element, the two elements may be fixed by a detachable connection manner, or may be fixed by a non-detachable connection manner, such as sleeving, clamping, integrally forming, or welding, which may be implemented in the conventional technology, which is not further described herein.
The technical features of the above embodiments may be arbitrarily combined, and all possible combinations of the technical features in the above embodiments are not described for brevity of description, however, as long as there is no contradiction between the combinations of the technical features, they should be considered as the scope of the description.
The foregoing examples merely represent several embodiments of the present disclosure, which are described in more detail and are not to be construed as limiting the scope of the invention. It should be noted that variations and modifications can be made by those skilled in the art without departing from the inventive concepts of the present disclosure, which are within the scope of the present disclosure.

Claims (12)

1. A gravity measurement device, comprising:
the measuring chamber comprises a shell, wherein the shell is provided with a cavity;
the electrode assembly is arranged on the shell and generates an electric field in the cavity after being electrified;
a lens provided in the housing;
the first light generating assembly is used for generating a first laser beam, enabling the first laser beam to pass through the lens, and forming an optical trap area in the cavity, wherein the optical trap area is used for suspending and capturing an object to be detected; a kind of electronic device with high-pressure air-conditioning system
And the second optical component is used for generating a second laser beam and transmitting the second laser beam into the cavity so as to detect the charge quantity of the object to be detected.
2. The gravity measurement device of claim 1, further comprising a mirror disposed within the chamber, wherein the first laser beam is reflected by the mirror to form the optical trap region.
3. The gravity measurement device of claim 2, wherein the housing includes a first end, a second end, and a sidewall connecting the first end and the second end, the first end and the second end being disposed opposite in a first direction; the lens comprises a first lens and a second lens, the first lens and the second lens are arranged on the side wall, and the height of the second lens in the first direction is higher than that of the first lens;
the reflecting mirror comprises a first reflecting mirror and a second reflecting mirror, and the first reflecting mirror and the second reflecting mirror are oppositely arranged in the first direction;
the first laser beam generated by the first light generating component passes through the first lens to the chamber, the first laser beam is reflected by the first reflecting mirror, the light trap area is formed between the first reflecting mirror and the second reflecting mirror, and the first laser beam passes through the second lens to the outside of the chamber after being reflected by the second reflecting mirror.
4. The gravity measurement device of claim 1, further comprising a launch assembly, at least a portion of which extends into the chamber of the housing for launching the test object into the optical trap area.
5. The gravity measurement device of claim 4, wherein the dispensing assembly comprises a dispensing base and a dispensing portion, the dispensing base is disposed outside the measurement chamber, one end of the dispensing portion is connected to the dispensing base, and the other end of the dispensing portion extends into the chamber of the housing.
6. The gravity measurement device of claim 5, wherein the launch assembly further comprises a vibrating portion for vibrating the launch portion, the vibrating portion being provided to the launch base.
7. The gravity measurement device of claim 5, wherein the launch base comprises:
a first moving part movable in a first direction; and/or
A second moving part movable in a second direction; and/or
A third moving part movable in a third direction; and/or
A first rotating part rotatable in a first direction; and/or
A second rotating part rotatable in a second direction; and/or
And a third rotating part rotatable in a third direction.
8. The gravity measurement device of claim 1 wherein the second optical module comprises an optical fiber connector, an optical fiber and an optical base, the optical base being located outside the measurement chamber, the optical fiber connector being located outside the optical base, the optical fiber being connected to the optical fiber connector and extending into the chamber of the housing.
9. The gravity measurement device of claim 8, wherein the light generating base comprises a base body and a bracket, the bracket being provided to the base body, the fiber optic connector being provided to the bracket; the extending direction of the bracket intersects with the extending direction of the housing.
10. The gravity measurement device of claim 9, wherein the base body comprises:
a first moving part movable in a first direction; and/or
A second moving part movable in a second direction; and/or
A third moving part movable in a third direction; and/or
A first rotating part rotatable in a first direction; and/or
A second rotating part rotatable in a second direction; and/or
And a third rotating part rotatable in a third direction.
11. A gravity measurement device as claimed in any one of claims 1 to 10 further comprising a discharge for ionising air to change the electrical quantity of the object to be measured.
12. The gravity measurement device of any one of claims 1 to 10 wherein the housing includes a first end, a second end and a side wall connecting the first end and the second end, the first end and the second end being oppositely disposed in a first direction; the electrode assembly comprises a first electrode and a second electrode, the first electrode is arranged at the first end, the second electrode is arranged at the second end, and an electric field is generated in the cavity after the first electrode and the second electrode are electrified.
CN202310988309.5A 2023-08-07 2023-08-07 Gravity measuring device Pending CN117111163A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202310988309.5A CN117111163A (en) 2023-08-07 2023-08-07 Gravity measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202310988309.5A CN117111163A (en) 2023-08-07 2023-08-07 Gravity measuring device

Publications (1)

Publication Number Publication Date
CN117111163A true CN117111163A (en) 2023-11-24

Family

ID=88804747

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202310988309.5A Pending CN117111163A (en) 2023-08-07 2023-08-07 Gravity measuring device

Country Status (1)

Country Link
CN (1) CN117111163A (en)

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
IT7949186A0 (en) * 1978-05-30 1979-05-25 Standard Oil Company Societa D IMPROVEMENT OF GRAVITY GRADIOMETERS
KR20110131975A (en) * 2010-06-01 2011-12-07 고려대학교 산학협력단 Absolute gravimeter using high resolution optical interferometer with parallel multiple pass configuration
WO2014040474A1 (en) * 2012-09-13 2014-03-20 中国科学院电工研究所 Low-temperature superconducting device for measuring gravity
CN104765075A (en) * 2015-04-09 2015-07-08 中国科学院测量与地球物理研究所 Dual-optical-path testing device for light speed limited effect in absolute gravimeter
CN108897057A (en) * 2018-04-25 2018-11-27 浙江大学 The full tensor gradiometry method and gravity gradiometer to be suspended based on luminous power
CN109814165A (en) * 2019-02-25 2019-05-28 浙江大学 A kind of cooling miniaturization high-precision optical gravimeter of luminous power
CN112485163A (en) * 2020-11-20 2021-03-12 浙江大学 Device and method for feeding back cooling particles in double-beam optical trap
CN112764115A (en) * 2020-12-29 2021-05-07 杭州微伽量子科技有限公司 Quantum absolute gravimeter and probe thereof
CN113701998A (en) * 2021-08-02 2021-11-26 浙江大学 Focusing lens arrangement error correction device and method in optical tweezers system
WO2021248698A1 (en) * 2020-06-12 2021-12-16 浙江大学 Absolute gravity meter based on optical tweezers in vacuum, and measurement method

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
IT7949186A0 (en) * 1978-05-30 1979-05-25 Standard Oil Company Societa D IMPROVEMENT OF GRAVITY GRADIOMETERS
KR20110131975A (en) * 2010-06-01 2011-12-07 고려대학교 산학협력단 Absolute gravimeter using high resolution optical interferometer with parallel multiple pass configuration
WO2014040474A1 (en) * 2012-09-13 2014-03-20 中国科学院电工研究所 Low-temperature superconducting device for measuring gravity
CN104765075A (en) * 2015-04-09 2015-07-08 中国科学院测量与地球物理研究所 Dual-optical-path testing device for light speed limited effect in absolute gravimeter
CN108897057A (en) * 2018-04-25 2018-11-27 浙江大学 The full tensor gradiometry method and gravity gradiometer to be suspended based on luminous power
CN109814165A (en) * 2019-02-25 2019-05-28 浙江大学 A kind of cooling miniaturization high-precision optical gravimeter of luminous power
WO2021248698A1 (en) * 2020-06-12 2021-12-16 浙江大学 Absolute gravity meter based on optical tweezers in vacuum, and measurement method
CN112485163A (en) * 2020-11-20 2021-03-12 浙江大学 Device and method for feeding back cooling particles in double-beam optical trap
CN112764115A (en) * 2020-12-29 2021-05-07 杭州微伽量子科技有限公司 Quantum absolute gravimeter and probe thereof
CN113701998A (en) * 2021-08-02 2021-11-26 浙江大学 Focusing lens arrangement error correction device and method in optical tweezers system

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
TLUSTY, T ET AL: "Optical gradient forces of strongly localized fields", PHYSICAL REVIEW LETTERS, vol. 81, no. 8, 24 August 1998 (1998-08-24), pages 1738 - 1741 *
沈瑜 等: "基于激光捕获的加速度测量原理及仿真", 红外与激光工程, vol. 39, no. 3, 25 June 2010 (2010-06-25), pages 543 - 548 *
蒋建斌 等: "真空悬浮光镊实验装置开发及教学应用", 光子学报, vol. 49, no. 5, 2 March 2020 (2020-03-02), pages 0512004 - 1 *

Similar Documents

Publication Publication Date Title
CN108508233B (en) Resonant opto-mechanical accelerometer for use in navigation-level environments
CN103620418B (en) Calibrating installation, methods and applications
JP5881345B2 (en) Extreme ultraviolet light generator
CN103557855B (en) A kind of colour center diamond gyro
CN107014476B (en) A method of utilizing sound pressure amplitudes in acoustic levitation drop measurement liquid
TW201024926A (en) Projection exposure apparatus for microlithography for the production of semiconductor components
US20220082413A1 (en) Diaphragm-based fiber acoustic sensor
CN112485163A (en) Device and method for feeding back cooling particles in double-beam optical trap
CN110337604A (en) Optical module and range unit
CN108489475A (en) A kind of hemispherical reso nance gyroscope harmonic oscillator vibration signal detection method and device
CN111141930A (en) MEMS accelerometer anti-reflection and reflector coatings
US5038620A (en) Coriolis mass flow meter
CN117111163A (en) Gravity measuring device
JP4906416B2 (en) Object passage detection device
EP1435535A2 (en) Optical fiber coupling system and manufacturing method thereof
CN108474655A (en) The measuring instrument of optical table with compensation temperature variation
US20020036251A1 (en) Inertial sensor for the mounting and checking of an inertial reference in a satellite
CN114778890B (en) Micro-cantilever beam optical fiber acceleration sensor mechanism
CN110926668A (en) Pressure sensor for improving measurement accuracy by utilizing total reflection principle and application thereof
CN115586600A (en) Transmit-receive integrated optical fiber all-optical ultrasonic probe and preparation method thereof
CN109742642A (en) A kind of solid state laser thermal lens focal length method and device
CN103116036A (en) Solid laser accelerometer
CN117214548B (en) Electric field sensing probe
Afshar et al. Lens-less, spring-loaded diaphragm-based fiber acoustic sensor
Marrara et al. Optical calibration of holographic acoustic tweezers

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination