# Velocity and Acceleration

The analysis of velocity and acceleration in a range of mechanisms including Klein's Construction for piston acceleration.

**Contents**

## Introduction

The Theory of Machines is concerned with the Motion of parts of machines and the forces which act on those parts. In most cases these forces are not constant and their calculation demands that we know the velocities and accelerations which occur in the various components.

The concept of **Instantaneous Centres of Velocity**was covered in the section on Mechanisms. In this section the Analysis of Velocity and Acceleration are considered with particular reference to Cranks and Pistons.

**Klien**'

**s Construction for Piston Acceleration**is introduced and a description of the

**Coriolis Component**is given.

### Velocity

- In the diagram the point moves in the plane . The length and the .

**Velocity**is the measurement of the rate and direction of change in the position of an object. It is a vector physical quantity; both magnitude and direction are required to define it.

Then:
And,
Differentiating with respect to time :
The radial component of Velocity ( i.e. in the direction of ) is given by:
And using equations (1) and (2)
Which is the rate of increase of
The tangential component of velocity (i.e. Perpendicular to in the direction of increasing)
Where = angular velocity of

### Acceleration

**Acceleration**is the time rate of change of velocity with respect to magnitude or direction; the derivative of velocity with respect to time.

Differentiating (1) and (2)
The Radial components of acceleration
And from equation (3)
The Tangential component of acceleration
By substitution:
(Note = Angular acceleration of )

Of these four terms in equations (4) and (5)
- is the rate of change of radial velocity
- is the centripetal acceleration due to the rotation of
- is due to the change in angular velocity.
- is called the compound supplementary acceleration or
**Coriolis Component**. Notice that the direction of this is the same as when is radially outwards.

## The Velocity And Acceleration Of A Piston By Analysis

In the following analysis is the uniform angular velocity of the crank. The positive direction of velocity and acceleration is away from the crankshaft.## The Vector Method For Velocity And Acceleration

The Law of addition of velocities states that: Velocity of = Velocity of + Velocity of relative to i.e.**Absolute velocities**(or accelerations) are given from to the corresponding point on the diagram.

**For Velocities**

- The relative velocity between two points and on the same link of a mechanism must be perpendicular to the line joining the points and is equal to (Equation (2))since is constant and is zero.
- The relative velocity for two points sliding over one another is along the common tangents of their paths and represents the component , is zero since

**For Acceleration**The relationships for acceleration are similar to those given for velocity:

- Acceleration of = Acceleration of + Acceleration of relative to
- Equations (4) and (5) are the general expressions for the radial and tangential components of relative acceleration.
- For two points on the same link leaving centripetal component (which can be calculated when the velocities are determined) and the tangential component
- For a uniformly rotating Crank leaving the centripetal as the only term.
- The
**Coriolis**component arises when a point on one link is sliding along another link which is itself rotating.

**Velocity (or acceleration) image**of the link.

## Klein's Construction For Piston Acceleration

The above is a diagramatic sketch of a piston, connecting rod, and crank assembly where,- is the connecting rod with the Crank Pin.
- is the crank.
- is the line of stroke.
- is the gudgeon pin

- Extend to meet the line through perpendicular to the line of stroke. Let the point of intersection be .
- Draw a circle centre and radius .
- Draw a circle with as diameter.
- Let the common cord cut the line at and the line of stroke at .

**acceleration diagram**for . It can be shown that this scale is .

- The Centripetal acceleration of the crank pin is
- The piston acceleration is
- is the Centripetal component and the Tangential component of the acceleration of relative to , so that is the acceleration image of .
- For any point on draw a line parallel to cutting in . The acceleration of is in magnitude and direction.

Example:

[imperial]

##### Example - Example 1

Problem

An aeroplane flying at 180 m.p.h. in a direction North of West sights another due North of . After 30 seconds flying is seen to be in a North-Easterly direction from and after a further 45 seconds is directly astern of . If is flying at a constant speed in a direction due South, find:

- a) The
**speed**of - b) For
**how long**is within 2 miles of

Workings

In the following diagram the Paths of and are shown. Their three particular positions are and respectively.
(30 seconds flying)
By scaling or by calculation and occupies 45 seconds of flying time.
Hence, Speed of =
Relative displacement of to = displacement of - displacement of
i.e.
In the first 30 seconds
Assuming that A is at rest at , the relative path of is produced and a circle centre and of radius 2 miles cuts this path at 1 and . Between 1 and , lies within 2 miles of .
But
This represents 30 seconds of relative displacement
But, Time corresponding to 1 mile =

Solution

- a) The
**speed**of is - b)