# Dynamics of Geared Systems

Acceleration of geared systems, and analysing combined angular and linear motions.

**Contents**

## Introduction

When a geared system accelerates or decelerates there is a change in the total inertia of the system. Clearly, the value of this increase or decrease depends upon the speed ratios of the various parts of the system.In this section we use the moments of inertia of geared shafts to identify the total torque and the Equivalent moment of Inertia for any given shaft in a state of acceleration.

## The Acceleration Of Geared Systems

**Acceleration**is the rate of change of velocity as a function of time and it is vector. Acceleration is the second derivative of position with respect to time or, alternately, the first derivative of the velocity with respect to time.

- Suppose that two shafts and are geared together and the speed ratio is
- The total moments of inertia on the shafts are and

- The torque on shaft required to accelerate is

- This will produce an acceleration of shaft of
- The torque required on shaft to achieve the above acceleration on is
- This would require a torque on shaft of
- The
**Total torque**on is thus given by: - is called the
**Equivalent moment of Inertia**referred to shaft .

### The Total Kinetic Energy Of A And B

The

**kinetic energy**of an object is the energy which it possesses due to its motion. It is defined as the work needed to accelerate a body of a given mass from rest to its stated velocity.
The Total Kinetic Energy of and
But since ,

## Combined Angular And Linear Motion

There are many cases where masses moving with linear motion are connected by a fixed speed ratio to inertias in angular motion. Instead of dealing with the two motions separately, it is possible to reduce the system to one of the following:### An Equivalent Angular Motion

The

**angular motion**is one type of motion in which a body acts as a radius and all parts of the moving body rotate in the same angular direction and follow a circular path about a pivot point.To find the torque required to give an angular acceleration of to the winding drum of moment of inertia and radius , which is being used to raise a load on a cable wrapped round the drum.

This method is used in worked examples 2, 7, and 8.### An Equivalent Linear Motion

**Linear motion**is motion along a straight line, and can therefore be described mathematically using only one spatial dimension.

The linear acceleration on the level of a car of weight and engine torque , whose wheels have an inertia of and radius , and an engine with an inertia and a gear ration , is found from:
The equivalent tractive effort =
= Acceleration Equivalent mass + Losses Losses

See Example 9.
Example:

[imperial]

##### Example - Example 1

Problem

Two gear wheels and are mounted on parallel shafts so that they may revolve separately or may be meshed together externally.
The wheels were originally turning freely in the same direction.
Find:

- a) The
**speed**and**direction of rotation**of wheel , if the gears are suddenly meshed, assuming that there is no back-lash of the teeth. - b) The
**loss of energy**in ft. lb. due to impact.

Workings

- a) Let r.p.m. be the final speed of so that the final speed of is in the opposite direction.

- b) The loss of Kinetic Energy

=\left [\frac{1}{2}\times \frac{10}{32.2}\times \left ( \frac{12}{12} \right )^2\left ( 300^2-30.75^2 \right )+

+\frac{1}{2}\times \frac{12}{32.2}\times \left ( \frac{10}{12} \right )^2\left ( 100^2-61.5^2 \right ) \right ]\times\left ( \frac{2\pi}{60} \right )^2=

Solution

- The
**speed**is - The
**loss of Kinetic Energy**is