JPS6355373A - Gravity engine - Google Patents

Abstract

PURPOSE:To obtain motive power from gravity, by rotating a single or a plurality of flexible levers and by causing a weight at each of their distal ends to make revolution along the inner surface of a deflected cylinder and changing a moment by changing a distance from a rotational center of the center of gravity of the weight. CONSTITUTION:When a support shaft 2 causes a flexible lever 1 to rotate about a fulcrum 3, a weight 14 pivotally supported by a rotating shaft 15 at its distal end 13 makes a revolution while it is in rolling contact with the inner surface of a cylinder 4 which is deflected (with respect to a center 7) a prescribed distance by its centrifugal force to change a moment by changing a distance to the lever fulcrum 3. In the case, when the flexible lever 1 rotates clockwise, a small when the flexible lever 1 rotates clockwise, a small moment is applied in a reverse rotational direction on the left hand side of a vertical line connecting an upper dead point 9 and a lower dead point 10. However, a large moment is applied in a forward rotational direction on the right hand side thereof. With the arrangement, the flexible lever can be rotated by the gravity of the weight.

Description

DETAILED DESCRIPTION OF THE INVENTION The present invention relates to gravity engines that seek to derive power from gravity.

One type of mechanical gymnastics is Daigun and Ring.

The Kojien dictionary, published in 1962, describes a large wheel as ``something that rotates around a large distance while holding a horizontal bar with both hands and keeping the body straight.''

However, if you look closely, you can see that it bends and stretches its body.

When the body is lowered, it is true that the body is stretched straight and rotated in a giant rotation, but when the body is raised, the body bends in a dogleg shape at a certain position, and when it reaches the highest position, it does a headstand. Stretch your body like this, and when your lower body starts to push up, you can see that you are lowering your body again while keeping your body straight.

If you straighten your body, the center of gravity of your body will move away from the horizontal bar, and your legs,
If you bend your hips or arms, the center of gravity of your body will move closer to the horizontal bar, so the absolute value of the moment of your body weight with respect to the horizontal bar will change as you bend and stretch your body.

If you stretch your body when going down and bend when going up, the absolute value of the moment of your body weight with respect to the horizontal bar will become larger when going down.
The absolute value of the work done by the weight on the iron bar is greater when it goes down than when it goes up, so the large wheel can continue to rotate.

The present invention is based on the above considerations.

Figure 1 is a diagram showing the principle of a bending and extending lever.

The amount of bending and stretching (1) is bending and stretching at the center (2), and the fulcrum at one end (3)
Rotate around.

The inner surface (5) of the cylinder (4) is aligned with the horizontal line (6) passing through the fulcrum (3).
), with its center (7) on the right side of the fulcrum (3).

The vertical line (8) passing through the center (7) of the inner surface (5) and the inner surface (5)
), the upper point is the top dead center (9) and the lower point is the bottom dead center αQ.

At the point where the horizontal line (6) passing through the fulcrum (3) and the inner surface (5) intersect, the point on the right is the right horizontal point αp1, and the point on the left is the left horizontal point (2).

Since the amount of bending and stretching (1) also functions as weight, the center of gravity should be determined, but for convenience, the center of gravity is set at the tip α→.

When rotation is applied to the bending/extending amount (1), the bending/extending amount (1) expands due to the action of centrifugal force, and the tip α→ is pressed against the inner surface (5) and moves in a circular motion.

Top dead center (9) is the point at which the tip α is at its highest position and begins to fall.

The bottom dead center α1 is the lowest position of the tip α1, and the point where the top starts to tilt.

The right horizontal point θυ is the point where the amount of bending and stretching (1) is the most extended and begins to bend.

The left horizontal point α is the point where the amount of bending and stretching (1) bends the most and begins to stretch.

Tip α1 is top dead center (9), right horizontal point α and bottom dead center α
The process of passing through O is a process in which the tip αJ descends from the highest position to the lowest position, and is also a process in which the amount of bending and stretching (1) extends the most at the right horizontal point α and begins to bend.

Tip 03 is bottom dead center αQ1 left horizontal point (6) and top dead center (
The process of passing through 9) is a process in which the tip (total) rises from the lowest position to the highest position, and is also a process in which the amount of bending and stretching (1) bends the most at the left horizontal point 0■ and begins to extend.

In the process of lowering, the center of gravity of the amount of bending and stretching (1) is farthest from the fulcrum (3), and the absolute value of the moment with respect to the fulcrum (3) of weight becomes maximum at the right horizontal point α.

In the process of going up, the center of gravity of the amount of bending and stretching (1) comes closest to the fulcrum (3), and the absolute value of the moment with respect to the fulcrum (3) of weight becomes the minimum at the left horizontal point 02.

The tip α1 moves in a circular motion along the inner surface (5), but the fulcrum (
For 3), it is like an elliptical motion.

Next, attach a weight α→ to the tip (G) of the amount of bending and stretching (1).

If the weight α→ is sufficiently larger than the amount of bending and stretching (1), the center of gravity of the weight α fathom may be regarded as the center of gravity of the entire body.

Attach the rotation axis αQ to the weight Q→, and the weight α→ becomes the rotation axis α.
Make it rotate as one with →.

When the rotating shaft α→ is pressed against the inner surface (5) by the action of centrifugal force, if friction is generated between the rotating shaft α and the inner surface (5), the rotating shaft α rotates and the weight a4 rotates.

The weight α→ will revolve around the fulcrum (3) while rotating on its own axis.

When gears are assembled and meshed between the rotating shaft α$ and the inner surface (5), the weight α◆ will surely rotate.

The rotating weight α→ also acts as a flywheel and greatly affects the revolution.

In order for the weight α◆ to be pressed against the inner surface by the action of centrifugal force,
At the time of starting, unless a sufficiently fast rotation is applied, the action of centrifugal force will be insufficient and the weight α→ will not be pressed against the inner surface (5), making starting difficult.

Especially when using gears to rotate the weight α→, it is desirable that the gears are always meshed.

The circumferential guide H is a circle that shares a center (7) with the inner surface (5), and is intended to bring the weight α→ close to the inner surface (5) in advance to facilitate starting and to keep the gears meshed at all times. .

In the figure, the center (7) of the inner surface (5) is placed to the right of the fulcrum (3) on the horizontal line (6), but if the center (7) is gradually moved to the left, the amount of bending and stretching (1) will be It's getting smaller,
When it reaches the fulcrum (3), the amount of bending and stretching disappears, and there is no difference in the absolute value of the amount of work done by the heavy shaft α→ in the process of lowering and rising, so the bending and stretching lever (1) cannot maintain its rotation. It disappears.

Furthermore, if the center (7) is to the left of the fulcrum (3), the absolute value of the work will be greater in the upward process, so the bending/extension lever (υ) should rotate in the opposite direction.

The center (7) of the inner surface (5) is located at the horizontal line (6) passing through the fulcrum (3).
), but the reason why the bending/extending lever (1) can maintain rotation is because there is a difference in the absolute value of the amount of work related to the fulcrum (3) during the downward and upward processes, so the center of the inner surface (5) (7) does not necessarily have to be on the horizontal line (6) passing through the fulcrum (3), but on the right side of the vertical MO force passing through the fulcrum (3) as long as the bending lever (1) can rotate within the inner surface (5). If it is in the opposite direction, it should be on the left side.

Although the cylinder (4) gives bending/extending motion to the bending/extending lever (1), the inner surface (5) does not necessarily have to be circular and may have other shapes such as an ellipse.

In the bending/extending lever (1), the center of gravity was changed by bending and stretching the lever, but it is also possible to extend and contract the lever like an antenna for a portable radio.

When extending and contracting the lever, the principle is the same as that of the bending and stretching lever (1), so in the explanation, it is sufficient to simply replace bending and stretching with extension and contraction.

Figure 2 is a diagram showing the principle of a lever on which a weight moves.

The bending and stretching lever (1) is the fulcrum of the center of gravity of the heavy shaft α→ (3)
I changed the distance from the movement example 0 Enoki along the lever
(to) is moved to change the distance from the center of gravity to the fulcrum.

Movement Example 0 One end of the groan is a fulcrum (A), and there is a guide (C) so that the heavy α field can move.

The inner vessel of the cylinder (A) guides the heavy cylinder in a circle whose center (C) is on the right side of the horizontal line (C) passing through the fulcrum (1).

The process in which the heavy weight 0 电 passes through the top dead center (C), the right horizontal point (A), and the bottom dead center (C) is the process in which the heavy weight α field decreases, and the weight 0 becomes the fulcrum at the right horizontal point (sha). The furthest away from -.

Heavy #) (l→ passes through the bottom dead center (C), left horizontal point 4, and top dead center (C) is the process in which the heavy shift α bu rises, and the heavy shift (1 tatami is the fulcrum) at the left horizontal point - is closest to

The movement example α→ is different from the expansion/contraction or bending/stretching lever (1), and the position of the center of gravity does not change, so it does not act as a weight.

[Brief explanation of drawings]

FIG. 1 is a diagram showing the principle of a gravity engine using a bending/extending lever, and FIG. 2 is a diagram showing the principle of a gravity engine using a moving example.

Claims (1)

[Claims] 1. Rotate one or more levers (sharing the fulcrum) around a fulcrum to revolve the weight, press the weight against the inner surface of the cylinder by centrifugal force, and align it with the shape of the inner surface. A gravity engine that obtains power by changing the distance from the fulcrum of the weight's center of gravity and changing the moment about the fulcrum, creating a difference in the absolute value of the amount of work in the process of lowering and raising the weight. 2. The gravity engine according to claim 1, which rotates a bending and extending lever. 3. Claim 1 in which the weight is revolved by a bending and stretching lever
Gravity engine as described in section. 4. The gravity engine according to claim 1, which rotates an extendable lever. 5. Claim 1 in which the weight is revolved by a lever that expands and contracts.
Gravity engine as described in section. 6. The gravity engine according to claim 1, which revolves a weight that moves along a lever. 7. The gravity engine according to claim 1, wherein the weight is rotated by friction with the inner surface of the cylinder. 8. The gravity engine according to claim 1, wherein a gear is incorporated into the inner surface of the cylinder and the weight, and the weight is rotated by the gear. 9. The gravity engine according to claim 1, which is combined with a guide that keeps the weight close to the inner surface of the cylinder within a certain range.