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Universal Framework for Science and Engineering - Part 9: Dynamics of aggregates

, 1 Feb 2007
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An article on framework applications to dynamics of aggregates.

Aggregate

.

1. Introduction

Long time ago I had had one idea related to mechanics. Lots of engineering problems requires simulation of aggregates. Mechanics of one object of aggregate may be simple. However equation of all aggregate may be very complicated. For example the picture of the beginning of this article shows the Mir orbital station. This station has nonrigid photovoltaics, gyroscopes and/or flywheels, jet engines etc. Long time ago I had an idea to develop designer of aggregates from those components. However implementaion of this idea only would provide a little advantage. Space objects have many aspects that lay outside pure mechanics. For example they interact with Magnetic fields. Motion of space object depends of this interacion. Moreover space objects have many devices founded on different physical principles and related to those motion. Now I have an universal framework and I can develop a valuable designer. But now I'm not engaged by mechanics of aggregates and maybe I'll never be occupied by this subject. However I wish to prove that this framework is really universal. Dynamics of aggregates is an excellent confirmation of the framework universality. So I've developed a few code devoted to this subject. Mybe this code contains lots of bugs. However the main idea is right.

2. Background

Dynamics of aggregates may be described by Classical mechanics that is familiar to any engineering student. How to create equation of aggregate from equations of its components. Elements of aggregates are connected. According to Classical mechanics first element acts to second by the invetred force and momenum that second acts to first. Moreover position and orientation of connections of two elements should coincide. Using listed above conditions we can create motion equations. I'll not overload readers here by technilal details but I'll write a paper to one of scietific journal later.

3. Simple example

Let us consider the following example of usage of the framework for simulation of dynamics of aggregates. This example contains spacecraft with 5 connections C 1, ..., C 5. Flywheels F 1, F 2, F 3 and photovoltaics P 1, P 2, P 3 are connected to spacecraft (See picture below)

Aggregate elements

Excuse me for my bad painting.This situation may be simulated by the following way.

Simple picture UI

If we open property editor of connection C 4 then we have:

Connection UI

This picture has the following meaning. The F 2 flywheel is connected to connection place 4 of the Body. Flywheel has a single connection numbered by 1. We need a library of objects for simulation of aggregate dynamics.

4. Library of objects

Library of objects has been developed as separated dll. Its present version contains three types of objects:

  • rigid body;
  • flywheel;
  • elastic vibrations body.

For using these objects you should put an Interface object to desktop. Then open AggregateLibrary.dll and select type of object by the following way:

Selection of object

Let us consider features of these objects.

4.1 Rigid body

Rigid body is a simplest object of 6D dynamics. My implementation of rigid body contains following editor of properties:

Rigid body properties

Key properties of my rigid body are places of connetions. Connections are defined by those coordinates and orientation. The rigid body that is presented above has 5 connections. You can define those coordinates X, Y, Z and components Q0, Q1, Q2, Q3 of quaternions of orientation. Rigid body also has another properties. We will consider them below.

4.2 Flywheel

Flywheel has general properties of rigid body and additional ones. Additional properties of flywheel include:

4.3 Elastic vibrations body

Elastic vibrations body is a mechanical system of infinite degrees of freedom. Usually math model of this object contains finite degrees of freedom with finite set of valuable harmonic oscillations. Every harmonic oscillation may be described by following second order system of ordinary differential equation:

Harmonic oscillation equation

Where q is generalized coordinate and Q is generalized force.

Editor of properties of this object is presented below

Elastic vibrations body properties

This object contains 5 valuable harmonic oscillations. You can edit coefficients of differential equations of these oscillations.

5. Advanced examples

Main advantage of this framework is interoperabilty with different brunches of science and engineering. These examples show this advantage of the framework. These examples are rather popular than realistic ones. Realistic pictures are much more complicated.

5.1 Controlled spacecraft

Let us consider following example. We have a spacecraft.

Controlled flight

Currents of its equipment interacts with Earth's magnetic field. Spacecraft has a photovoltaic that is an elastic vibrations body. It is used a flywheel for angular stabilzation of the spacecraft. Now let us construct this situation:

Control scenario

Now I'll explain it. First of all I setup Coordinates of Spacecraft. We need it for definition of gravitational acceleration and magnetic field. Then I construct Magnetic Field by formulas. Earth's magnetic field is very complicated and it is not easy to construct it by formulas. Usage of external library is more appropriate. But now I've no such library and I set formulas from my mind. It is convenient to have a vector of magnetic field. Therefore I've used Field Vector:

Vector i

I've named this operation as assembly. Using vector I've defined mechanical moment of field spacecraft interaction as vector product of magnetic induction and magnetic moment of spacecraft:

Vector

This product is contained in Magnetic force. Then we disassembly result vector using the Force components. Unlike magnetic field I have got a library of gravity field (square Gravity). I've used it for definition of gravity accelerations. Now we've defined all forces and we can put Spacecraft and define its properties. They are exhibited on the following form:

Aliases of spacecraft

Using aliases we've linked Coordinates and Spacecraft. The tab page of forces and moments is presented below:

Spacecraft forces and moments

We've defined inertial accelerations and mechanical moments. Then we connect a Flywheel and a Photovoltaic to Spacecraft and define those properties. Now the mechanical system is ready. Let us construct its control system. First its element is a sensor. We will use a sensor of local vertical. To do this we define Spacecraft frame and Earth's center frame. Relative position (6D) enables us simulate the sensor of local vertical. The Control law uses it. And at last Flywheel moment of Flywheel is a Formula_1 of Control law:

Spacecraft forces and moments

This system is unstable. If you have 5 minutes only then it is not easy to construct the control system of spacecraft. It is my first experience. Maybe it is the last one. To say true, I can do nothing. My mission is to explain to specialists the most nontrivial aspects of their occupation.

5.2 Virtual vibrostand

At part 3 I had had performed a lot of work. I had made a frequency difference detector and a phase discriminator. This work should be used for mechanics. Now I'll use this work for definition of frequency response. To do this I'll construct virtual vibrostand. I'd never seen real vibrostand. However I think that it looks like:

Real vibrostand

Mechanical device acts to spacecraft by momentum and then computer compares input and output signals. Now I'll construct this vibrostand using the framework, spacraft of 5.1 and schemes of part 3 :

Virtual vibrostand

The Chirp acts by momentum on spacecraft. The Chirp rate is small. Another parts of this scenario are parts of frequency difference detector and phase discriminator. Amplitude and Phase are components of frequency response. However it is not worth to try it since this spacecraft is unstable

6. Points of interests

OMG I've got this idea off my brain. Now I can devote myself to more interesting things.

License

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About the Author

Petr Ivankov
Architect
Russian Federation Russian Federation
Ph. D. Petr Ivankov worked as scientific researcher at Russian Mission Control Centre since 1978 up to 2000. Now he is engaged by Aviation training simulators http://dinamika-avia.com/ . His additional interests are:
 
1) Noncommutative geometry
 
http://front.math.ucdavis.edu/author/P.Ivankov
 
2) Literary work (Russian only)
 
http://zhurnal.lib.ru/editors/3/3d_m/
 
3) Scientific articles
http://arxiv.org/find/all/1/au:+Ivankov_Petr/0/1/0/all/0/1

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