The shock-wave propulsion of rectilinear motion
The shock-wave propulsion system addresses the challenge of mechanical devices in weightlessness by using hollow pipes and controlled gas-liquid transformations to generate force impulses for propulsion, enabling efficient motion and termination in space environments.
Patent Information
- Application Number
- PCT/UA2025/000015
- Authority / Receiving Office
- WO · WO
- Patent Type
- Applications
- Current Assignee / Owner
- Priority Date
- 2024-05-28
- Filing Date
- 2025-03-25
- Publication Date
- 2025-12-04
AI Technical Summary
Existing mechanical devices lack the capability to effectively operate in weightlessness and provide propulsion for space objects.
A shock-wave propulsion system utilizing hollow pipes with sequential supply and transformation of a liquid working body into gas under high pressure, combined with shock wave extinguishers and liquefaction systems, to generate a force impulse for motion, and a controlled pumping mechanism to manage the working body's flow.
Enables efficient propulsion in weightlessness by leveraging the difference in impulse timing within a closed mechanical system, allowing for translational motion and motion termination.
Smart Images

Figure UA2025000015_04122025_PF_FP_ABST
Abstract
Description
[0001] THE SHOCK-WAVE PROPULSION OF RECTILINEAR MOTION
[0002] The shock-wave propulsion of rectilinear motion (SWP, propulsion, system) refers to space technology (G03H 99 / 00; B64G 1 / 28) and can be used as a power drive for moving space objects in weightlessness.
[0003] There are no analogues of mechanical devices whose action in weightlessness can correspond to SWP.
[0004] The purpose of the invention is to expand the range of mechanical means suitable for working in weightlessness, along with the use of rocket engines.
[0005] To ensure the motion of the system, sequential, with a time delay, supply of the liquid working body into the hollow pipes, in a quantity no less than two, near the plugged ends of these pipes, followed by its transformation into a gas with high pressure and maintenance of this pressure during the working cycle, which ensures the occurrence of force on the plugged ends of the pipes with the formation of an impulse of the main part of the system, is used to ensure the motion of the system. At the opposite free ends of the pipes, shock wave extinguishers are installed, after which the working body enters the liquefaction. After liquefaction, the working body is pumped back by the pump for further supplying into the pipes. In the pipes, in which the shock wave has reached the shock wave damper, the supply of the working body is stopped, and they are freed from the excess of the working body before the start of a new cycle.
[0006] An example of a block diagram of a shock-wave propulsion using three pipes is shown in Fig. 1.
[0007] The SWP consists of a body 1, to which all further elements of the propulsion are attached, a certain number of pipes 2, which are made in the form of a hollow pipe, one of the ends of which is plugged and has a liquid working body supply system to maintain high pressure in the pipe during the work cycle, 3 the gasification system of the working body (heater) 4, shock wave extinguishers are installed near unblocked ends the other pipes 5, the liquefaction system of the working body 6, to which the pipes are connected 2, after the shock wave extinguishers 5, the system of return pumping of the working body 7, the control system 8, which with the help of the supply system 3, connects each subsequent pipe 2 to work with a time delay calculated in such a way that the last working pipe is turned on at the same time as the first pipe is turned off, the power system 9, the system of refueling and storage of the working body 10.
[0008] The propulsion due to a temporarily uncompensated impulse that occurs in the system before its operation is completed.
[0009] A peculiarity of the shock-wave propulsion of rectilinear motion is its property, being in weightlessness, due to a temporarily uncompensated impulse, to bring itself into translational motion or to end it.
[0010] The possibility of motion of the shock wave propulsion is based on two phenomena:
[0011] The difference in time that exists in a closed mechanical system between the occurrence of an impulse of its main part during the mutual rectilinear movement of the system elements and the time of its compensation.
[0012] Differences between the impulse occurring in the main part of the system during the execution of the working cycle and the impulse arising during the reverse pumping of the working body, due to the fact that part of the impulse during the execution of the working cycle is transmitted directly by the shock wave without transferring the mass of the working body.
Claims
CLAIM1. The shock-wave propulsion of rectilinear motion contains at least two pipes, some ends of which are plugged, and shock wave dampers are installed on the other, unblocked ones, a high pressure gaseous working body supply system, the outlet lines of which are connected to the pipes near the plugged ends through remote-controlled taps of turn on and off of the supply of the working body to the pipes according to the commands of the control unit, and the inlet line of the system of the supply of the working body is connected to the shock wave dampers, the control unit, which includes the supply of the working body to each subsequent pipes with a time delay calculated in the way that the supply of the working body to the last pipe is turned on at the same time as the supply of the working body to the first pipe is turned off after the shock wave has reached the shock wave damper in it.
Citation Information
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