CN215908309U - Magnetic resistance shockproof structure - Google Patents

Abstract

The utility model relates to a magnetic resistance shockproof structure, which mainly comprises: a first casing, an upper lining conductor, a lower pressing piece, a first magnet, a second casing, a lower lining kit and a second magnet, wherein the upper lining The conductor is arranged in the first accommodating space of the first casing and defines the first actuating space, the lower pressing piece is arranged in the first actuating space, and the first magnet arranged at the bottom of the pressing piece is formed between the first magnet and the upper lining conductor In a repulsive action, the first magnet can run in the first actuating space due to the repulsive action, the second casing is disposed on one side of the first casing and defines a second accommodating space, and the lower lining set is disposed in the second accommodating space The space defines a second action space that communicates with the first action space. The second magnet is fixed in the second action space and maintains a repulsive distance with the first magnet within a fixed range. Set and match and apply Lenz's law, which can be used as shockproof and buffering through the magnetic effect.

Description

Magnetic resistance shockproof structure

Technical Field

The present invention relates to a quakeproof structure, and more particularly to a magnetic resistance quakeproof structure.

Background

With the increasing development of science and technology, vibration-proof equipment is particularly important for precision products in the market, such as precision sound equipment, precision instrument equipment and the like, because vibration caused by external factors is damaging, or sound, loudspeakers and the like in the precision sound equipment can slightly vibrate due to output, and the amplitude of vibration can be obviously sensed on the loudspeakers due to light or heavy rhythm.

The sources of the aforementioned vibrations are many, including: for precision audio equipment, the vibration of the equipment itself, the vibration caused by environmental influences, artificial vibration, natural vibration (earthquake), etc. for the existing common solution, the vibration-damping foot pad is mainly disposed at the bottom of the precision audio equipment to prevent the audio equipment from shifting or toppling over and affecting the listening quality due to shaking. The shock-absorbing foot pad has a complex assembly structure, more components, high cost and time consumption; therefore, the pad is usually made of foam pad, wool pad or cone at low cost, and the foam pad and wool pad will deform and the cone will scratch and damage the board.

SUMMERY OF THE UTILITY MODEL

The main purposes of the utility model are as follows: the first magnet and the upper lining conductor are arranged and matched, and Lenz's law is applied, so that the purposes of shock resistance and buffering can be achieved through the magnetic effect.

To achieve the above object, the present invention provides a magnetoresistive vibration isolation structure, which includes a first housing defining an opening and a first receiving space communicating with the opening; an upper lining conductor which is arranged in the first accommodating space and defines a first actuating space; a lower pressing piece which is arranged in the first actuating space and penetrates out of the opening, the bottom of the lower pressing piece is provided with a first magnet positioned in the first actuating space, and the first magnet and the upper lining conductor use Lenz's law to enable the first magnet to generate a slow descending state in the first actuating space; the second shell is arranged on one side of the first shell and defines a second accommodating space; a lower lining suite, which is arranged in the second accommodating space and defines a second actuating space communicated with the first actuating space, and the lower lining suite is locked on the first shell; and a second magnet fixed in the second actuating space and keeping a fixed range of repulsion distance with the first magnet.

According to an embodiment of the present invention, the first casing further includes a plurality of bolts passing through the lower liner set and locked to the first casing.

According to an embodiment of the present invention, a distance space for adjusting the distance between the lower lining set and the first shell by each bolt is defined between the lower lining set and the first shell.

According to an embodiment of the present invention, the cushion further includes a cushion body disposed at the distance space position.

According to an embodiment of the present invention, the apparatus further includes a mounting base, which is provided with the second magnet and can be arbitrarily changed to a fixed position in the second actuating space.

According to an embodiment of the present invention, the lower liner set defines a stop structure for limiting the movement range of the mounting base.

According to an embodiment of the present invention, the pressing member defines a stopping surface capable of stopping against the first housing.

According to an embodiment of the present invention, the upper lining conductor is an aluminum pipe.

The utility model has the beneficial effects that: by arranging and matching the first magnet and the upper lining conductor and applying Lenz's law, the magnetic damper can achieve the purposes of shock resistance and buffering through the magnetic effect

Drawings

Fig. 1 is a schematic cross-sectional view of a preferred embodiment of the present invention.

FIG. 2 is an exploded view of the cross-sectional structure of the preferred embodiment of the present invention.

Fig. 3 is a schematic view of a cross-sectional structure of the pressing member of the present invention in a use state.

Fig. 4 is a schematic view showing a cross-sectional structure of the rebounding of the depressing member according to the present invention in a use state.

Description of the figure numbers:

the magnetic resistance shockproof structure comprises a magnetic resistance shockproof structure 1, a first shell 10, an opening 100, a first accommodating space 102, an upper lining conductor 11, a first actuating space 110, a lower pressing piece 12, a stop surface 120, a first magnet 13, a second shell 14, a second accommodating space 140, a lower lining sleeve piece 15, a second actuating space 150, a stop structure 152, a second magnet 16, a bolt 2, a cushion body 3 and a mounting seat 4.

Detailed Description

Fig. 1 and fig. 2 are a schematic cross-sectional structure and an exploded cross-sectional structure of the preferred embodiment of the utility model. The utility model relates to a magnetic resistance shockproof structure, a magnetic resistance shockproof structure 1 mainly comprises a first shell 10, an upper lining conductor 11, a lower lining 12, a first magnet 13, a second shell 14, a lower lining external member 15 and a second magnet 16, wherein the first shell 10 defines an opening 100 and a first accommodating space 102 communicated with the opening 100, the upper lining conductor 11 (an aluminum pipe) is arranged in the first accommodating space 102 and defines a first actuating space 110, the lower lining 12 is arranged in the first actuating space 110 and penetrates out of the opening 100, the bottom of the lower lining 12 is provided with the first magnet 13 and is positioned in the first actuating space 110, the first magnet 13 and the upper lining conductor 11 generate a slow descending state in the first actuating space 110 by utilizing Lenz's law, the second shell 14 is arranged at one side of the first shell 10 and defines a second accommodating space 140, the lower lining external member 15 is arranged in the second accommodating space 140 and defines a second actuating space 150 communicated with the first actuating space 110, the lower lining set 15 is locked to the first housing 10, and the second magnet 16 is fixed to the second actuating space 150 and maintains a fixed range of repulsion distance with the first magnet 13.

The lower lining assembly 15 is inserted and locked to the first casing 10 by a plurality of bolts 2, the distance between the lower lining assembly 15 and the first casing 10 can be adjusted by the bolts 2, the distance between the first actuating space 110 and the second actuating space 150 can be changed by adjusting, and the cushion body 3 is disposed at the distance.

In addition, the second magnet 16 is installed on the installation seat 4, the installation seat 4 can be arbitrarily fixed at the position of the second actuating space 150, and the repelling distance between the second magnet 16 and the first magnet 13 can be adjusted by arbitrarily changing the position of the installation seat 4 in the second actuating space 150.

Furthermore, the lower lining set 15 defines a stop structure 152, and the stop structure 152 can limit the moving range of the mounting seat 4 and prevent the mounting seat 4 from separating from the lower lining set 15. The stop surface 120 defined by the lower member 12 can mainly stop against the first casing 10, so as to prevent the lower member 12 from being separated from the top surface of the first casing 10.

Fig. 3 and 4 are schematic views of a cross-sectional structure of a pressing member and a cross-sectional structure of a pressing member rebounding according to the present invention. As can be seen from fig. 3, when the pressing member 12 is pressed down by gravity, the pressing member 12 can provide a buffer to resist shock, when the pressing member 12 is pressed down by the pressing force, the pressing member 12 naturally moves down along the first actuating space 110, and since the first magnet 13 is driven by lenz's law between the first magnet 13 and the upper lining conductor 11 to generate a slow-down state in the first actuating space 110, and meanwhile, a certain repulsive distance is provided between the first magnet 13 and the second magnet 16, when the first magnet 13 moves down to be close to the second magnet 16, the first magnet 13 is driven by the repulsive distance to generate a sufficient buffer force on the pressing member 12.

What is called lenz's law in the foregoing is that an induced current generated due to a change in magnetic flux has a direction that resists the change in magnetic flux. In particular, by pushing the magnet toward the copper conductor, the magnetic flux through the copper conductor is enhanced. According to lenz's law, the induced current will be counterclockwise as viewed from the magnet to the copper conductor. This is because the magnetic field generated by the induced current in the counterclockwise direction, which is opposite to the direction of the magnetic field of the magnet, makes the total magnetic field weaker than the magnetic field of the magnet, thereby resisting the change of the magnetic flux.

Conversely, if the magnet is pulled away from the copper conductor in the opposite direction, the magnetic flux through the loop is reduced. According to lenz's law, the induced current will be clockwise from the magnet to the copper conductor. This is because the magnetic field generated by the clockwise induced current, which has the same direction as the magnetic field of the magnet, makes the total magnetic field stronger than the magnetic field of the magnet, thereby resisting the change of the magnetic flux.

As described above, when the present invention is applied to an audio device, the first magnet 13 and the upper lining conductor 11 (aluminum pipe) are arranged and matched to form a state conforming to lenz's law, so that the present invention can achieve the purpose of shock resistance and buffering through the magnetic effect.

As can be seen from fig. 4, when the first magnet 13 moves to the bottom, the first magnet 13 and the second magnet 16 generate a repulsion phenomenon, and therefore, there is a repulsion distance between the first magnet 13 and the second magnet 16, when the first magnet 13 is pressed down by the pressing member 12 due to gravity, the first magnet 13 approaches the second magnet 16, and when the repulsion distance is pulled close, a rebound force is generated, so that the first magnet 13 rebounds, and the pressing member 12 is kept in the first actuation space 110, thereby achieving the shockproof effect.

As can be seen from the above, the first magnet 13 and the upper lining conductor 11 (aluminum pipe) according to the present invention are arranged and matched, and the lenz's law is applied, so as to achieve the purpose of shock resistance and buffering through the magnetic effect.

Claims (8)

1. a magnetic resistance shockproof structure, is characterized in that, it comprises: a first casing defining an opening and a first accommodating space communicating with the opening; an upper lining conductor disposed in the first accommodating space and defining a first actuating space; A lower pressing piece, which is arranged in the first actuating space and passes through the opening, a first magnet located in the first actuating space is arranged at the bottom of the pressing piece, and is used between the first magnet and the upper lining conductor Lenz's law makes the first magnet produce a slow-down state in the first action space; a second casing disposed on one side of the first casing and defining a second accommodating space; a lower lining set, which is disposed in the second accommodating space and defines a second actuating space communicated with the first actuating space, the lower lining set is locked to the first casing; and A second magnet is fixed in the second action space and maintains a repulsive distance within a fixed range from the first magnet. 2 . The magnetoresistive anti-vibration structure as claimed in claim 1 , further comprising a plurality of bolts, which pass through the lower lining set and are locked to the first casing. 3 . 3 . The magnetoresistive anti-vibration structure as claimed in claim 2 , wherein a distance space is defined between the lower lining set and the first casing, the distance of which is adjusted and changed by the bolts. 4 . 4 . The magnetoresistive anti-vibration structure of claim 3 , further comprising a cushion body disposed at the distance space position. 5 . 5 . The magnetoresistive anti-vibration structure of claim 1 , further comprising a mounting seat for arranging the second magnet and arbitrarily changing the fixed position in the second actuating space. 6 . 6 . The magnetoresistive anti-vibration structure as claimed in claim 5 , wherein the lower lining set defines a resisting structure that limits the movement range of the mounting seat. 7 . 7 . The magnetoresistive anti-vibration structure as claimed in claim 1 , wherein the pressing member defines a resistance surface capable of abutting against the first casing. 8 . 8 . The magnetoresistive anti-vibration structure of claim 1 , wherein the upper lining conductor is an aluminum tube. 9 .

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