Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed...

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Dynamic Mechanisms

Transcript of Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed...

Page 1: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Dynamic Mechanisms

Page 2: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

BASICS OF LOCI

Page 3: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A locus is the movement of a point as it follows certain conditions

• For example, a line is the locus of a point as it moves in a straight path

What is a Locus?

Page 4: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A circle is the locus of a point which moves so it remains a constant distance from a fixed point “p”

• The fixed point is called the centre and the distance the radius

The Circle as a Locus

p

Page 5: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• We use loci to find the midpoint of a line

• The locus of a point which moves so that it is equidistant from two fixed points is called the perpendicular bisector of the line

• The intersection of the perpendicular bisector and the line segment yields the midpoint

Constructions that use Loci

A B

Page 6: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• We can used loci to solve simple problems such as finding the bisector of an angle

• The bisector of an angle can be defined as:

• The locus of a point that moves so that it remains equidistant from 2 fixed lines

Constructions that use Loci

D

A

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Page 7: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

INVOLUTES

Page 8: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 9: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• An involute is the locus of a point on a line as the line rolls along a shape

• It can also be thought of as the locus of the end of a piece of string as the string is wound/unwoundaround the circumference of a plane figure

Involutes

Page 10: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Involutes are used to determine the length of belts used in pullies and other machines

• Involutes are also used to calculate the amount of material required to create tyres and wheels

Applications of Involutes

Page 11: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Involute of a Square

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DA

BC

ABA C

BA

Page 13: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Involute of a Triangle

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A

Page 15: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Involute of a Hexagon

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Page 17: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Involute of a Circle

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Page 19: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Making Involute models

• http://www.math.nmsu.edu/~breakingaway/Lessons/involute1/involute.html

Page 20: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

TANGENTS TO INVOLUTES

Page 21: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Involutes are curves, and as with all curves a tangent can be drawn to the involute

Tangents to Involutes

Page 22: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Tangent to an involute at point P

P

Page 23: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 24: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Tangent to an involute at point P

P

Page 25: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 26: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

THE HELIX

Page 27: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

The Helix

• A helix is the locus of a point as it moves on the surface of a cylinder so that it rotates at a constant rate around the surface of the cylinder, while also progressing in the direction of the axis at a constant rate

Page 28: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Helix Anatomy

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The development of a helix appears as a straight line development

Page 29: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A geodesic is the shortest distance between two points on a surface

• The geodesic of a cylinder may be:– A circle

– A linear element

– A helix

Helix as a Geodesic

Page 30: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• The helix is used for the thread of bolts, reamers and drill bits

• Springs are derived from the helix

• Helical gears are derived from the helix

• Winding staircases are also derived from the helix

Applications of the Helix

Page 31: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• The helix may be the most important shape in the universe as the human gene code is structured around a helix

Applications of the Helix

Page 32: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

30°

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Left and Right Hand Helix Rule

Place your thumb along the shape of the helix as shown, and you will notice that the shape of the thumb and the helix are similar. This is a left hand helix. The plan of the cylinder will be indexed clockwise

Place your thumb along the shape of the helix as shown, and you will notice that the shape of the thumb and the helix are similar. This is a right hand helix. The plan of the cylinder will be indexed anti-clockwise

Left Hand Helix Right Hand Helix

Page 33: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

A right hand helix of one revolution

Page 34: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

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A left hand helix of one revolution

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A right handed helix of 1 ½ revolutions

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Page 39: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Internal Diameter: Diameter of Shaft/ internal helical curve

• Outside Diameter: Outermost diameter of the thread/helical curve

• Lead: amount of axial advance during one complete revolution of the helix

• Pitch: is the distance from a point on the helix to a corresponding point on the next revolution measured parallel to the axis

Helical Screw Thread: Terminology

Outside Diameter

Lead

Pitch

Internal Diameter

Page 40: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Right handed and Left handed Screw Threads

Page 41: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Single Start Double Start

Variations of Helical Screw Threads•A helical screw thread can consist of more than two helices•A two start screw thread has four helices•A three start would have six helices, etc

Page 42: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Single Start ThreadPitch = Lead

Two Start ThreadPitch= ½ Lead

Helical Screw Thread

Lead

Pitch

Lead

Pitch

When large axial movement is required two or more threads may be cut on one screw

Page 43: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Draw one revolution ofa single start right-handed screw thread (½the pitch) given

• Inside Ø: 40mm

• Outside Ø: 82mm

• Lead: 60mm

• Square Thread: 30mm

Helical Screw Thread

Lead Pitch

Page 44: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

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Page 45: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Given the plan and elevation of a cylinder with two points on its surface, X and Y. Draw a helix starting from the base of the cylinder and finishing at the top of the cylinder and passing through X and Y

Helix Problems

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Page 47: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Given the plan and elevation of a cylinder, having the point P on its surface draw a helix of one revolution so as it passes through P

Helix Problems

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Parallel to typical helix through the point

Page 49: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

SPIRAL GEOMETRY

Page 50: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Spiral

• A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point.

• If a line rotate about one of its end points (the pole), and at the same time a point moves continuously in one direction along the line, the locus of the moving point is a spiral

Pole

Page 51: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Conical Helix/Conical Spiral

• A conical spiral is the locus of a point as it moves on the surface of a cone so that it rotates at a constant rate around the cone while also progressing in the direction of the axis at a constant rate

• The plan of a conical spiral is an Archimedean spiral

Page 52: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• The conical spiral is used for augers and other boring devices such as screw tips

• It is also used for the construction of Archimedean wells

Applications of the Conical Spiral

Page 53: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Construct a conical spiral

Page 54: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

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Page 55: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Conical Spiral

• Note: A conical spiral is not a geodesic, as the development of a conical spiral is a curve

Page 56: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Term Definition

Pole The point at the centre

Convolution One complete rotation of the point around the spiral

Vector Angle The angle between any two radius vectors

Radius Vector Any line from pole to a point on the spiral

Spiral Terminology

Radius Vector

Pole

One Convolution

Page 57: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• There are two main types of spirals:

• Archimedean Spirals

• Logarithmic Spirals

Spiral Types

Page 58: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• An Archimedean spiral is the locus of a point that moves around a circle at a constant speed while also moving away from/towards the pole at a constant speed

Archimedean Spirals

Page 59: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• The Archimedean spiral is functional as well as aesthetic

• Archimedean springs are used in watch making and door mechanisms

• Because of the link between the conical and Archimedean spiral many of the applications of the Archimedean spiral are exhibited through the conical spiral

Applications of the Archimedean Spiral

Page 60: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A logarithmic spiral is a spiral that increases/decreases proportionally according to a given rule.

• A logarithmic curve will never terminate at a pole

Logarithmic Spirals

Page 61: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Logarithmic Spirals are naturally occurring spirals in nature

• The sea shell on the right contains a logarithmic spiral

• The natural occurrence of manmade design in nature or visa versa is known as bio-mimicry

Applications of the Logarithmic Spiral

This Wikipedia and Wikimedia Commons image is from the user Chris 73 and is freely available at http://commons.wikimedia.org/wiki/Image:NautilusCutawayLogarithmicSpiral.jpg under the creative commons cc-by-sa 2.5 license

Page 62: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Some universes branch out in a logarithmic spiral

• An understanding of geometrical shapes may assist scientists and engineers in furthering their research and discoveries

Applications of the Logarithmic Spiral

Page 63: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Spiral Types

Archimedean Spiral Logarithmic Spiral

Page 64: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Draw an archimedean spiral of one convolution given the longest radius vector as 60mm and the shortest as 0mm

Archimedean Spirals

Page 65: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

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Page 66: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Archimedean Spirals

• Draw an archimedian spiral of 1 ¾ convolutions given the longest radius vector as 60mm and the shortest as 20mm

Page 67: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

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Page 68: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Archimedean Spirals

• Construct one convolution of an archimedean spiral given the shortest radius vector of 20mm and an increase in vector length of 5mm every 45°

Page 69: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Add 5mm onto the radius vector for every 45° increment

Page 70: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Logarithmic Spirals

A:B=Ratio of Spiral

B

Construction derived from similar traingles

Page 71: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Logarithmic Spirals

• Construct one convolution of an logarithmic spiral given a vector angle of 30° and the ratio of the vector lengths as 10:12 (Initial radius not specified)

Page 72: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

12

Logarithmic spiral derived from similar triangles

Page 73: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

TANGENTS TO SPIRALS

Page 74: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Tangent to an Archimedean spiral at a point P

P

Page 75: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

1 Radian = 57.3°

Page 76: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

P

Tangent to a Logarithmic spiral at a point P

Page 77: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

As this is an equiangular spiral it can be mathematically proven that the angle between any radius vector and a tangent will always be a constant 77°20’

Page 78: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Animation of a logarithmic spiral involute

• http://mathworld.wolfram.com/LogarithmicSpiralInvolute.html

Page 79: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

LOCI

Page 80: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A locus is the movement of a point as it follows certain conditions

• A locus may be used to ensure that moving parts in machinery do not collide

Applications of Loci

Page 81: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 82: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A cycloid is the locus of a point on the circumference of a circle which rolls without slipping along a straight line

• The valve on a car tyre generates a cycloid as the car moves

Cycloid

Page 83: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• http://www.edumedia-sciences.com/a325_l2-cycloid.html

Other cycloid animations

Page 84: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

P

Draw a cycloid given the circle, the base line and the point on the circumference

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Triangulation Method

The cycloid is the locus of a point on thecircumference of a circle which rolls without slippingalong a straight line

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Triangulation Method with lines omitted for clarity

Page 87: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• An inferior trochoid is the path of a point which lies inside a circle which rolls, without slipping, along a straight line

• The reflector on a bicycle generates an inferior trochoid as the bike moves along a flat surface

Inferior Trochoid

Page 88: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

P

Draw an inferior trochoid given the circle, the base line and the point P inside the circumference

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An inferior trochoid is the path of a pointwhich lies inside a circle, which rolls,without slipping along a straight line.

Page 90: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Superior Trochoid

• A superior trochoid is the path of a point which lies outside a circle which rolls, without slipping, along a straight line

• Timber moving against the cutter knife of a planer thicknessergenerates a superior trochoid

Page 91: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

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Draw a superior trochoid given the circle, the base line and the point P outside the circumference

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P1 2 3 4 5 6 7 8 9 10 11

A superior trochoid is the path of a point which lies inside a circle, which rolls, without slipping around the inside of a fixed circle

Page 93: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Epicycloid

• An epicycloid is the locus of a point on the circumference of a circle which rolls without slipping, around the outside of a fixed arc/ circle

• The applications and principles of a cycloid apply to the epicycloid

• Various types of cycloids are evident in amusement rides

Page 94: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

P

If a circle rolls without slipping round the outside of a fixed circle then a point P on the circumference of the the rolling

circle will produce an epicycloid

Page 95: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Segment lengths stepped off along base arc

An epicycloid is the locus of apoint on the circumference of acircle which rolls withoutslipping, around the outside ofa fixed arc/ circle

Page 96: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Inferior Epitrochoid

• An inferior epitrochoidis the path of a point which lies inside a circlewhich rolls, without slipping, around the outside of a fixed circle

• The applications and principles of the inferior trochoid apply to the inferior epitrochoid

Page 97: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

If a circle rolls without slipping round the inside of a fixed circle then a point P inside the circumference of the the

rolling circle will produce an inferior epitrochoid

Page 98: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Segment lengths stepped off along base arc

An inferior epitrochoid is thepath of a point which liesinside a circle, which rolls,without slipping around theoutside of a fixed circle

Page 99: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Superior Epitrochoid

• A superior epitrochoid is the path of a point which lies outside a circle which rolls, without slipping, around the outside of a fixed circle

• The applications and principles of the superior trochoid apply to the superior epitrochoid

Page 100: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

If a circle rolls without slipping round the inside of a fixed circle then a point P outside the circumference of the the

rolling circle will produce a superior epitrochoid

Page 101: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

A superior epitrochoid is thepath of a point which liesoutside a circle, which rolls,without slipping around theoutside of a fixed circle

Page 102: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Hypocycloid

• A hypocycloid is the locus of a point on the circumference of a circle which rolls along without slipping around the inside of a fixed arc/circle.

• The applications of the cycloid apply to the hypocycloid

Page 103: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

P

If a circle rolls without slipping round the inside of a fixed circle then a point P on the circumference of the the rolling

circle will produce a hypocycloid

Page 104: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

112

2

3

4

5

6

78

9

10

11

1

23

45 6

7 8 9 1011 12

Segment lengths stepped off along base arc

The hypocycloid is the locus of apoint on the circumference of acircle which rolls along withoutslipping around the inside of afixed arc/circle

Page 105: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Superior Hypotrochoid

• A superior hypotrochoidis the path of a point which lies outside a circlewhich rolls, without slipping, around the inside of a fixed circle

• The applications and principles of the superior trochoid apply to the superior hypotrochoid

Page 106: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

If a circle rolls without slipping round the inside of a fixed circle then a point P outside the circumference of the the

rolling circle will produce a superior hypotrochoid

Page 107: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

1 2

12 3

4

5

6

78

9

10

11

1

2

34

56 7 8 9

1011

12

A superior hypotrochoid is the path of apoint which lies outside a circle, whichrolls, without slipping around the inside of afixed circle

Page 108: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Inferior Hypotrochoid

• An inferior hypotrochoid is the path of a point which lies inside a circle which rolls, without slipping, around the inside of a fixed circle

• The applications and principles of the inferior trochoid apply to the inferior hypotrochoid

Page 109: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

If a circle rolls without slipping round the inside of a fixed circle then a point P inside the circumference of the the

rolling circle will produce an inferior hypotrochoid

Page 110: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

121 2

3

4

5

6

78

9

10

11

1

23

45 6 7 8 9 10

11 12

Segment lengths stepped off along base arc

An inferior hypotrochoid is the path of apoint which lies inside a circle, which rolls,without slipping around the inside of a fixedcircle

Page 111: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• The path the object follows can change as the object rolls

• The principle for solving these problems is similar ie. triangulation

• Treat each section of the path as a separate movement

• Any corner has two distinctive loci points

Loci of irregular paths

Page 112: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Loci of irregular paths

P

A

C

B

The circle C rolls along thepath AB without slipping forone full revolution.Find the locus of point P.

Page 113: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

65

4

3

2

1

7

8

9

10

11

0,124321

P

X

X

Point X remains stationary while the circle rolls around the bend

Page 114: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

TANGENTS TO LOCI

Page 115: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Tangent to a cycloid at a point P

P

Page 116: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Normal

Arc length =Radius of Circle

Page 117: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Tangent to an epicycloid at a point P

P

Page 118: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Normal

Arc length =Radius of Circle

Page 119: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Tangent to the hypocycloid at a point P

P

Page 120: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Normal

Arc length =Radius of Circle

Page 121: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Further Information on Loci

• http://curvebank.calstatela.edu/cycloidmaple/cycloid.htm

Page 122: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

COMBINED MOVEMENT

Page 123: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Combined Movement

Shown is a circle C, which rolls clockwise along the line AB for one full revolution. Also shown is the initial position of a point P on the circle. During the rolling of the circle, the point P moves along the radial line PO until it reaches O. Draw the locus of P for the combined movement.

PA

O

C

B

Page 124: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

65

4

3

2

1

7

8

9

10

110,12

654321 7 8 9 10 11 12

P

Page 125: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Combined MovementShown is a circle C, which rollsclockwise along the line AB forthree-quarters of a revolution.Also shown is the initial positionof a point P on the circle. Duringthe rolling of the circle, thepoint P moves along the semi-circle POA to A.

Draw the locus of P for thecombined movement.

A

PO

C

B

Page 126: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

20°

A

P

C

B1 2 3 4 5 6 7 8 9

1

2

3

4

56

7

8

9

Page 127: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Combined Movement

The profile PCDA rolls clockwise along theline AB until the point D reaches the line AB.During the rolling of the profile, the point Pmoves along the lines PA and AD to D.Draw the locus of P for the combinedmovement.

A

P

D

C

B

Page 128: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

P6P4

P3

7

A

6 5 4

P2

3 2

P5

P

4

1

32

7

56

1

D6

5

4

3

21

P1

Page 129: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

LINKAGES

Page 130: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Linkages are used to restrict the motion of objects so that they follow a regular path

• Linkages are commonly found in children's toys, windows, automotive parts, etc

Linkages

Page 131: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Linkages are used to redirect kinetic energy or other forces

• A scissors jack is a common example of a linkage

Linkages

Page 132: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Basic Linkages

Sliding Link Pivot

Crank Rocker

Page 133: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Sliding Link

• Sliding links are used to restrict the movement of a link to movement along an axis

• Sliding links have many applications and functions

• Sliding links restrict the opening in windows

Page 134: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Pivot

• A pivot joins two links together and allows 360° of freedom about the pivot

• A pivot acts like a hinge

• Pivots are found in many household items

Page 135: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Crank

• Cranks are used to receive motion or to transfer rotary motion

• Cranks are often used with bevel gears or other variations of gears

• Common examples are in wheel braces, hand mixers etc

Page 136: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A rocker mechanism restricts the swing of a linkage, to a known angle

• Rockers are very prominent in children's cradles, chairs and similar objects

• The locus of the rocker must be found to ensure the chair doesn't swing too far back

Rocker

Page 137: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Linkages

• Mechanisms like this are a common feature in machines

• In order for such mechansims to operate as desired it is necessary to plot the loci of the parts

Page 138: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Converting Mechanisms to Line Drawings

A

B

C

P

Page 139: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Converting Mechanisms to Line Drawings

A

B

C

P

Page 140: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

A

P

A ladder AB is leaning against awall, with one end against thewall and the other on the floor.Plot the locus of the midpoint ofthe ladder as it slides to the floor

B

Page 141: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 142: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

The figure below shows a crank AB whichrotates clockwise about point A. Link BC isrestricted to slide vertically at C.Plot the locus of point P for one revolution ofthe crank.

A

B

P

C

Page 143: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 144: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

The figure below shows a crank ABwhich rotates about the fixed pointB in a clockwise direction. Point C isa trunnion. Crank BC pivots aboutthe fixed point B and slides throughthe trunnion.Plot the locus of point P for onerevolution of the crank AB. A

P

C

B

Page 145: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 146: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

The figure below shows a crank OA which rotatesabout the fixed point O. A and B are pin joints. CrankBC pivots about the fixed point C. Plot the locus ofpoint P for one revolution of the crank OA.

A

P

C

B

O

Page 147: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 148: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

The crank OD rotates anticlockwise about a fixed point O. AB oscillates aboutthe fixed point A. D is fixed to a block, which slides along AB. Point C isconstrained to slide horizontally.Plot the locus of point P during one complete revolution of the crank OD

PCB

O

D

A

Page 149: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 150: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

E/P

C

DB

A

The figure below shows a crank Ab which rotates anti-clockwise aboutpivot C. Another crank CD rotates clockwise about Pivot C. Link BE pivotsat B and E. Link DEP pivots at D and E. Plot the locus of point P for onerevolution of the cranks. (Both cranks rotates at the same rate)

Page 151: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 152: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

The figure below shows a crank AB which pivotsabout A. B is a pivot and P is a sliding link. Plotthe displacement diagram for point P for onecomplete clockwise revolution of the crank.

P

B

A

Page 153: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 154: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

CAMS

Page 155: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A cam is a machine part for transferring rotary motion to linear motion

• In a radial plate cam, the cam is mounted on a rotating shaft

• The motion is recieved by a follower

• To see a cam in operation click on the link

Cams

Follower

Cam

Shaft

http://www.engr.colostate.edu/~dga/video_demos/mechanisms/IC_engine_cam_crank_animation.gif

Page 156: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Followers can be knife edged, rollers or flat footed

Follower Types

Knife Edged Roller Flat Footed

Page 157: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• The point of the follower can follow very complicated cam profiles

• Wears Rapidly

• Must be used at low speeds

Knife Edged Follower

Page 158: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line
Page 159: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

30 60 120 150 180 210 240 270 300 330 36090

30

60

120

150180

210

240

270

300

330

360

90

• In order to determine the shape of a cam, a displacement diagram is drawn first

• The height of the diagram (A) is equal to the total displacement of the follower ie. the difference between the highest and lowest points

• The width of the displacement diagram does not matter but it is divided into regular divisions representing angular increments (on the cam)

• 30° increments are generally used

Displacement Diagrams

Displacement Diagram

Cam Profile

A

Page 160: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A cam that imparts uniform velocity (UV) has the following displacement diagram

• The cam shown has a rise at uniform velocity, followed by a fall at uniform velocity• The follower rises and falls at a

constant speed• Shown over is the cam profile

with uniform velocity rise and uniform velocity fall

• The disadvantage of uniform velocity is abrupt changes of movement of the follower

Uniform Velocity (UV)

UV UV

Page 161: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A dwell is a period when there is no displacement of the follower– Cam radius remains

constant

• A cam will have a circular profile for periods of dwell

• Note the circular segment on the cam

Dwell

UV UVDwell

Page 162: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• Simple Harmonic Motion (SHM) is the gentle acceleration and deceleration of the end view of a point as it rotates at constant speed around the diameter of a circle

• Simple harmonic motion produces a sine curve

• Shown over is the outline of a cam with SHM rise and SHM fall

Simple Harmonic Motion (SHM)

Simple Harmonic Motion

Page 163: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• A follower with Uniform Acceleration and Retardation (UAR) will accelerate and decellerate at the same rate

• The path of UAR is parabolic and can be drawn using the rectangle method

• Shown over is the outline of a cam with UAR rise and UAR fall

Uniform Acceleration and Retardation (UAR)

UAR

Page 164: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Cams

• Draw the displacement diagram for a plate cam rotating in an anticlockwise direction imparting the following motion to the inline knife edge follower:– UV rise 0˚-90˚ of 40mm– Dwell 90˚-180˚– SHM fall 180˚-360˚ of 40mm

• The nearest approach of the follower to the cam shaft centre is 20mm

• The can shaft diameter is 15mm

Page 165: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

0 30 60 90 120 150 180 210 250 270 300 330 360

30˚

60˚

90˚

120˚

150˚

180˚

210˚

250˚

270˚

300˚

330˚

360˚

UV rise Dwell SHM

Fall 0˚30˚

60˚

90˚

120˚

150˚

Total rise 40Nearest approach of follower 20mmØ15 mm shaft

Page 166: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Cams

• Draw the displacement diagram for a plate cam rotating in a clockwise direction imparting the following motion to the inline knife edge follower:– SHM rise 0˚ -90˚ of 35mm– UV rise 90˚ -210˚ of 10mm– UAR fall 210˚ -360˚ of 45mm

• The nearest approach of the follower to the cam shaft centre is 20mm

• The cam shaft diameter is 15mm

Page 167: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

0 30 60 90 120 150 180 210 250 270 300 330 360

0

330

300

270

240

210

180

150

120

90

60

30

360

Nearest approach of follower 20mmØ15 mm shaft

Total rise 45

Page 168: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Plot the follower displacement diagram

for an in-line knife-edge follower in contact with the cam profile shown

below

Page 169: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

360°

30°

60°

90°

120°

150°

180°

210°

240°

270°

300

330°

30° 60° 90° 120° 150° 180° 210° 240° 270° 300° 330° 360°0°

Page 170: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Roller Followers

• Are used because they give a smoother movement and they wear more evenly

Page 171: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Cams

• Draw the displacement diagram for a plate cam rotating in an anticlockwise direction imparting the following motion to the roller follower:– UV rise 0˚ -90˚ of 40mm– Dwell 90˚ -180˚– SHM fall 180˚ -360˚ of 40mm

• The roller follower has a diameter of 12mm• The nearest approach of the roller centre to the

cam shaft centre is 20mm• The cam shaft diameter is 15mm

Page 172: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

0 30 60 90 120 150 180 210 250 270 300 330 360

30˚

60˚

90˚

120˚

150˚

180˚

210˚

250˚

270˚

300˚

330˚

360˚

UV rise Dwell SHM

Fall 0˚30˚

60˚

90˚

120˚

150˚

Total rise 40Nearest approach of follower 20mm

Ø15 mm shaftRoller Ø12

Page 173: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Flat Footed Follower

• Wears slower than a knife edge follower

• May bridge over hollows

Page 174: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Cams

• Draw the displacement diagram for a plate cam rotating in an anticlockwise direction imparting the following motion to the flat follower:– UV rise 0˚ -90˚ of 40mm– Dwell 90˚ -180˚– SHM fall 180˚ -360˚ of 40mm

• The follower extends 6mm to either side• The nearest approach of the follower to the cam

shaft centre is 20mm• The can shaft diameter is 15mm

Page 175: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

0 30 60 90 120 150 180 210 250 270 300 330 360

30˚

60˚

90˚

120˚

150˚

180˚

210˚

250˚

270˚

300˚

330˚

360˚

UV rise Dwell SHM

Fall 0˚30˚

60˚

90˚

120˚

150˚

Total rise 40Nearest approach of follower 20mm

Ø15 mm shaft

Flat footed follower extends 6mm to either side

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GEARS

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• Gears are toothed wheels• Gears are used to

transmit motion• Gears are also used to

convert rotary to linear motion or visa versa

• Gears can be used to reduce or increase the torque on an object

• Gears are found in watches, engines and toys

Gears

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Types of Gears• There are many different types

of gears, each of which are designed for their specific purpose

• Different types of gears are used in the following machines:

• Drills: Bevel Gears

• Car engines: Helical Gears

• Watches: Epicycloidal Gears

• Power transmission: Involute Spur Gears

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• http://www.mekanizmalar.com/involute1.shtml

Gear animations

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• Imagine two disks in contact at their circumference (friction wheels)

• These two disks meet at one point • If one disk rotates it imparts motion to the other disk• However these disks are prone to slipping• Large pressure must be exerted between the disks in

order to create a sufficient frictional force between them

• Friction wheels will only be used where low power is required

• Introducing teeth will eliminate slipping occurring

Why gears?

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Why gears?Two Friction Wheels

Two Toothed Wheels

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• A spur gear is a toothed wheel

• The shape of the teeth is derived from either an involute curve or an epicycloidal curve

• The involute is the most commonly used curve

Spur Gears

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Gear Terminology

Driver Gear

Pinion (Driven Gear)

Rack

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Gear Terms

Term Definition

DriverGear

When two gears are in mesh the gear withthe power (connected to the shaft) is calledthe driver

Pinion

When two gears are in mesh the smallergear is called the pinion, and the gear whichpower is transmitted to is called the drivengear

Rack It is a spur gear whose radius is at infinity)

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Gear ratio

• The gear ratio is the ratio at which one gear rotates relative to the other and it is directly proportional to the diameter of the gears

• Diameter of driver gear = D• Diameter of driven gear = d• Gear ratio= D:d• If the driver gear has a diameter of 200 and the

driven gear has a diameter of 100 then the gear ratio will be 2:1– The driven gear rotates twice as fast as the driver gear

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Page 187: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

Gear teeth

• The aim of designing gear teeth is that the faces of the teeth will roll across each other, minimalising the sliding friction

• Two types of curves are commonly used:– Involute

– Epicycloidal

Root Circle

Tip Circle

Base Circle

InvoluteCurves

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Involute Curves

Tip Circle

Pitch Circle

Involute Curves

Root Circle

The involute profile provides continuous contact between the teeth while also providing a smooth rolling motion

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Parts of a Gear Tooth

Flank

Bottom Land

Top Land

Pitch Surface

Tooth Trace

Pitch Circle

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• An imaginary circle which corresponds to the outside diameter of the friction rollers from which the spur gears are derived.

• Formula = – Module × Number of

teeth

Parts of a Gear ToothPitch Circle

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• Radial distance from the pitch circle to the top of the tooth

• Formula: – Addendum = module

Parts of a Gear Tooth

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Addendum

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• Radial distance from the pitch circle to the bottom of the tooth space

• Formula: – Dedendum = 1.25 ×

module

Parts of a Gear Tooth

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Dedendum

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• Distance between the top of a tooth and the bottom of the mating space

• Formula: – Dedendum - Addendum

Parts of a Gear Tooth

Clearance

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• The base circle is the imaginary circle from which the involute is created

• Formula: – Base Circle Diameter =

Pitch Circle Diameter ×cos (pressure angle)

Parts of a Gear Tooth

Base Circle

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• Distance measured along the pitch circle from a point on one tooth to a corresponding point on the next tooth. This includes one tooth and one space.

• Formula: – {πd(circumference)} ÷ n

Parts of a Gear Tooth

Circular Pitch

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Circular Pitch

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• Circular thickness: Thickness of one tooth measured along the pitch circle, equal to ½ the circular pitch.

• Formula: – Circular pitch ÷ 2

Parts of a Gear Tooth

Circular Thickness

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Circular Thickness

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• Outside Diameter: is the diameter of the circle that contains the top of the teeth =

• Formula: – Pitch Circle Diameter + 2

addendum

Parts of a Gear Tooth

Outside Diameter

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• Diameter of the root circle

• Formula: – Pitch Circle Diameter - 2

dedendum

Parts of a Gear Tooth

Root Circle

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• Full height of the tooth

• Formula: – Addendum + Dedendum

Parts of a Gear Tooth

Whole Depth

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Whole Depth

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• Distance a tooth projects into the mating space

• Formula: – 2 × Addendum

Parts of a Gear Tooth

Working Depth

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Working Depth

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• Angle created at the centre of the gear between a point on one tooth on the PCD, and the corresponding point on an adjacent tooth

• Formula: – 360 ÷ number of teeth

Parts of a Gear Tooth

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Angular Pitch

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• Common Tangent – A line tangential to the two base circles along which contact between the meshing teeth takes place, also known as the line of action

• Pitch Point – Point of contact between the pitch circles of meshing gears

More Terminology

Common tangent

Common Normal

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Parts of a Gear Tooth

Flank

Bottom Land

Top Land

Pitch Surface

Tooth Trace

Pitch Circle

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Parts of a Gear Tooth

Term Definition

Pitch SurfaceIs an imaginary cylindrical surface which contains the pitch circleof a gear

Addendum Is the part of the tooth outside the pitch

Dedendum Is the part of the tooth inside the pitch surface

FlankIs the part of the tooth that comes into contact with other gears

Tip Surface Is and imaginary surface at the top of the tooth

Root Surface Is an imaginary surface at the bottom of the tooth

Top Land Is the part of the tooth between opposite flanks

Bottom Land Is the part of the root surface between opposite flanks

Tooth TraceIs the intersection between the pitch surface and the flank of thetooth

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Gear Terminology

Tip Circle

Pitch Circle

Base Circle

Root Circle

Θ = pressure angle

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Pitch Circle Diameter

Tip circle

Root circle

Base circle

Addendum

Clearance

Tooth thickness measured on PCD

Dedendum

Working Depth

Circular Pitch

Whole Depth

Pitch Angle

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Gear Terms

Term Symbol Definition

Addendum a The part of the tooth that extends outside of the pitchcircle/pitchlineThe addendum is always equal to the modulea=m

Base Circle BCD An imaginary circle from which the tooth shape is generatedThe base circle = the pitch circle diameter × cos (pressureangle)

BCD=PCD × cos (pressure angle)

This circle can be constructed graphically

Circular Pitch p Is the distance from the point on one tooth to thecorresponding point on the next toothMeasured around the pitch circle

p= πm

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Gear Terms

Term Symbol Definition

Circular Tooth Thickness The thickness of a tooth measured along the pitch circle

Circular tooth thickness = p/2

Clearance c Is the space underneath the tooth when it is in meshClearance = ¼ of the addendum

c =d - a=0.25a=0.25m

Dedendum d Is the part of the tooth which is inside the pitch circle or the pitch line=1.25 × addendum

d=1.25 a

Line of Action Contact between the teeth of meshing gears takes place along a line tangential to the two base circlesThis line passes through the pitch point

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Gear Terms

Term Symbol Definition

Module m Is the pitch circle diameter divided by the number of teethThe module for gears in mesh must be the same or they will vibrate and wear badly

m= PCD/t

Pitch Circle Diameter PCD

Pinion When two gears are in mesh the smaller gear is called the pinion

Pitch Angle 360°÷ number of teeth

Pitch Circle PC Is the circle representing the original cylinder which transmitted motion by friction

Pitch Point When two gears are in mesh their pitch circles will be tangiental to each other. The pitch point is the point of contact betweeen the two circles

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Gear Terms

Term Symbol Definition

Pressure Angle Θ The angle between the line of action and the common tangent to the pitch circles at the pitch point

The pressure angle is normally 20° but may be 14.5°

Tip Circle A circle through the tips of the teeth

Wheel When two gears are in mesh the larger one is called the wheel

Whole depth Is the depth of the tooth from tip to rootWhole depth = addendum + dedendum

Working Depth The whole depth – the clearance

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Line of action

• To ensure the gear motion is smooth, quiet and free from vibration, a direct line of transmission must act between the gear teeth

• This line of action, or common normal determines the pressure angle of the teeth and passes through the pitch point.– i.e. Gears in mesh meet at only one point which is

the intersection of their Pitch Circle Diameters

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Page 220: Dynamic Mechanisms - t4...Spiral • A spiral can be the locus of a point as it moves around a fixed point (pole) while steadily increasing its distance from the point. • If a line

• http://science.howstuffworks.com/gear8.htm

Other line of action animations

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Line of Action

Line of Action

Common Normal

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• A rack is a straight toothed bar

• Technically it is a spur gear whose radius is at infinity

• Because of this all principles of circular spur gears hold true

Rack

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Rack

½ p ½ p

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Tip Circle

Pitch Circle

Base Circle

Root Circle

Tip Line

Root Line

Pitch Line

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• http://www.brockeng.com/mechanism/RackNPinion.htm

Line of action for a rack and pinion animation

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Gears

• Given a pitch circle diameter of 200mm and a module of 10, and a pressure angle of 20°construct the spur gear.

• Show at least four teeth on the gear• Teeth to be constructed by the involute

method.

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Gear Calculations Results

Module (m) 10

No. of teeth (t) 20

Pressure angle (Θ) 20°

Pitch circle diameter (PCD) m × t 200mm

Base circle diameter PCD × cosΘ 187.9mm

Addendum (a) a = m 10mm

Dedendum (d) 1.25 × m 12.5mm

Clearance d - a 2.5mm

Tip circle diameter PCD + 2a 220mm

Root circle diameter PCD - 2d 175mm

Circular pitch (p) π × m 31.4mm

Tooth thickness p ÷ 2 15.7mm

Pitch angle 360° ÷ t 18°

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PCD=200

Addendum/Tip circle

Dedendum/ Root circle

Base circle

Addendum=moduleTip Circle=Ø220

Dedendum=1.25 *moduleRoot circle=Ø175

Use graphical construction

Number of teeth=PCD=module(m)*number of teeth (t)PCD=m*t=20 teeth

Circular pitch distance=p=πmp=31.4

Tooth thickness= 31.4/2=15.7

Angular pitch= 360/t360/16=18°

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PCD=200

Addendum/Tip circle

Dedendum/ Root circle

Base circle

Tooth radiates into centre below base circle

Clearance = 0.25*module=2.5

Tooth thickness measured on PCD

Angular Pitch (18°)

Only Pitch circle and tip circle are required for left hand side.

Tracing paper may be used to replicate the tooth profile

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SOLUTION USING UNWINSMETHOD

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PCD=200

Addendum/Tip circle

Dedendum/ Root circle

Base circle

Addendum=moduleTip Circle=Ø220

Dedendum=1.25 *moduleRoot circle=Ø175

Base Circle Ø= PCD *cos (pressure angle)BCD=187.9mm

Number of teeth=PCD=module(m)*number of teeth (t)PCD=m*t=20 teeth

Circular pitch distance=p=πmp=31.4

Tooth thickness= 31.4/2=15.7

Angular pitch= 360/t360/16=18°

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4

3

2

1

A B C

Tangent to base circle

Radius 1A

Pitch Point (P)

Tooth Thickness

Bisector of tooth thickness (radiating to CP of PCD)

Axial Symmetry of Centre point 1

Radius 1P

Bottom of tooth profile radiates into centre point

Clearance Circle

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4

3

2

1

A B C

Tangent to base circle

Tooth thickness

Length 1 to A

Pitch Point

Axial symmetry

Clearance Circle

Pitch Angle

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Gears

• Draw two involute spur gears in mesh and show five teeth on each gear.

• The gear ratio is 4:3.• Driver gear details: Module=8, teeth=24,

pressure angle=20°

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Driver Gear Calculations Results

Module (m) 8

No. of teeth (t) 24

Pressure angle (Θ) 20

Pitch circle diameter (PCD) m × t 192

Base circle diameter PCD × cosΘ 180.4

Addendum (a) a = m 8

Dedendum (d) 1.25 × m 10

Clearance d - a 2

Tip circle diameter PCD + 2a 208

Root circle diameter PCD - 2d 172

Circular pitch (p) π × m 25.13274123

Tooth thickness p ÷ 2 12.56637061

Pitch angle 360° ÷ t 15

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Driven Gear Calculations Results

Module (m) 8

No. of teeth (t) 4:3=24:18 18

Pressure angle (Θ) 20

Pitch circle diameter (PCD) m × t 144

Base circle diameter PCD × cosΘ 135.3

Addendum (a) a = m 8

Dedendum (d) 1.25 × m 10

Clearance d - a 2

Tip circle diameter PCD + 2a 160

Root circle diameter PCD - 2d 124

Circular pitch (p) π × m 25.13274123

Tooth thickness p ÷ 2 12.56637061

Pitch angle 360° ÷ t 20

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PCD

Addendum/Tip circle

Root circle/Dedendum

Base circle

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PCD

Addendum/TipRootcircle/dedendum

Base circle

Pitch Angle 15°

Pitch Angle 20°

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Gears

• An involute gear is in mesh with a rack.• The involute gear has 20 teeth, a pressure

angle of 20° and module of 10.• Draw the gear and rack in mesh, showing four

teeth on the gear and an equivalent on the rack.

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Gear Wheel Calculations Result

Module (m) 10No. of teeth (t) 20Pressure angle (Θ) 20Pitch circle diameter (PCD) m × t 200Base circle diameter PCD × cosΘ 187.9Addendum (a) a = m 10Dedendum (d) 1.25 × m 12.5Clearance d - a 2.5Tip circle diameter PCD + 2a 220Root circle diameter PCD - 2d 175Circular pitch (p) π × m 31.4Tooth thickness p ÷ 2 15.7Pitch angle 360° ÷ t 18

Rack Result

Module 10

Pressure angle 20°

Addendum 10mm

Dedendum 12.5mm

Clearance 2.5mm

Pitch 31.4mm

Tooth thickness 15.7mm

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½ p ½ p

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Tip Circle

Pitch Circle

Base Circle

Root Circle

Tip Line

Root Line

Pitch Line

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PCD

Addendum/Tip circle

Dedendum/ Root circle

Base circle

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Pitch Angle 18°

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Links to Dynamic Mechanisms

• http://www.ul.ie/~nolk/maincontents.htm