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Moment of inertia
From Wikipedia, the free encyclopedia
This article is about the moment of inertia of a rotating object, also termed the mass moment of inertia. For the moment of
inertia dealing with the bending of a beam, also termed the area moment of inertia, see second moment of area.

In classical mechanics, moment of inertia, also called mass moment of inertia, rotational inertia, polar moment of
inertia of mass, or the angular mass, (SI units kg·m²) is a measure of an object's resistance to changes to its rotation. It is
the inertia of a rotating body with respect to its rotation. The moment of inertia plays much the same role in rotational
dynamics as mass does in linear dynamics, describing the relationship between angular momentum and angular
velocity, torque and angular acceleration, and several other quantities. The symbolsI and sometimes J are usually used to
refer to the moment of inertia or polar moment of inertia.

While a simple scalar treatment of the moment of inertia suffices for many situations, a more advanced tensor treatment
allows the analysis of such complicated systems as spinning tops and gyroscopic motion.

The concept was introduced by Leonhard Euler in his book Theoria motus corporum solidorum seu rigidorum in 1765.[1] In
this book, he discussed the moment of inertia and many related concepts, such as the principal axis of inertia.

                    Contents

                        [hide]



1 Overview

2 Scalar moment of inertia for single body

3 Scalar moment of inertia for many bodies

 o     3.1 Moment of inertia about a point

 o     3.2 Moment of inertia theorems

 o     3.3 Properties

 o     3.4 Energy, angular momentum, torque

 o     3.5 Examples

4 Moment of inertia tensor

 o     4.1 Definition

 o     4.2 Derivation of the tensor components

 o     4.3 Reduction to scalar

5 Principal axes of inertia

 o     5.1 Parallel axis theorem

 o     5.2 Rotational symmetry

 o     5.3 Comparison with covariance matrix

6 See also

7 Notes

8 References
9 External links

[edit]Overview

The moment of inertia of an object about a given axis describes how difficult it is to change its angular motion about that
axis. Therefore, it encompasses not just how much mass the object has overall, but how far each bit of mass is from the
axis. The further out the object's mass is, the more rotational inertia the object has, and the more torque (force* distance
from axis of rotation) is required to change its rotation rate. For example, consider two hoops, A and B, made of the same
material and of equal mass. Hoop A is larger in diameter but thinner than B. It requires more effort to accelerate hoop A
(change its angular velocity) because its mass is distributed farther from its axis of rotation: mass that is farther out from that
axis must, for a given angular velocity, move more quickly than mass closer in. So in this case, hoop A has a larger moment
of inertia than hoop B.




Divers reducing their moments of inertia to increase their rates of rotation


The moment of inertia of an object can change if its shape changes. Figure skaters who begin a spin with arms outstretched
provide a striking example. By pulling in their arms, they reduce their moment of inertia, causing them to spin faster (by the
conservation of angular momentum).

The moment of inertia has two forms, a scalar form, I, (used when the axis of rotation is specified) and a more
general tensor form that does not require the axis of rotation to be specified. The scalar moment of inertia, I, (often called
simply the "moment of inertia") allows a succinct analysis of many simple problems in rotational dynamics, such as objects
rolling down inclines and the behavior of pulleys. For instance, while a block of any shape will slide down a frictionless
decline at the same rate, rolling objects may descend at different rates, depending on their moments of inertia. A hoop will
descend more slowly than a solid disk of equal mass and radius because more of its mass is located far from the axis of
rotation. However, for (more complicated) problems in which the axis of rotation can change, the scalar treatment is
inadequate, and the tensor treatment must be used (although shortcuts are possible in special situations). Examples
requiring such a treatment include gyroscopes, tops, and even satellites, all objects whose alignment can change.

The moment of inertia is also called the mass moment of inertia (especially by mechanical engineers) to avoid confusion
with the second moment of area, which is sometimes called the area moment of inertia (especially by structural engineers).
The easiest way to differentiate these quantities is through their units (kg·m² as opposed to m4). In addition, moment of
inertia should not be confused with polar moment of inertia (more specifically, polar moment of inertia of area), which is
a measure of an object's ability to resist torsion(twisting) only, although, mathematically, they are similar: if the solid for
which the moment of inertia is being calculated has uniform thickness in the direction of the rotating axis, and also has
uniform mass density, the difference between the two types of moments of inertia is a factor of mass per unit area.
Inertia
Inertia is the resistance of any physical object to a change in its state of motion or rest, or the tendency of an object to resist
any change in its motion. The principle of inertia is one of the fundamental principles of classical physics which are used to
describe the motion of matter and how it is affected by applied forces. Inertia comes from the Latin word, iners, meaning
idle, or lazy. Isaac Newton defined inertia as his first law in his Philosophiæ Naturalis Principia Mathematica, which states:[1]

The vis insita, or innate force of matter, is a power of resisting by which every body, as much as in it lies, endeavours to
preserve its present state, whether it be of rest or of moving uniformly forward in a straight line.

In common usage the term "inertia" may refer to an object's "amount of resistance to change in velocity" (which is quantified
by its mass), or sometimes to its momentum, depending on the context. The term "inertia" is more properly understood as
shorthand for "the principle of inertia" as described by Newton in his First Law of Motion; that an object not subject to any net
external force moves at a constant velocity. Thus an object will continue moving at its current velocityuntil some force
causes its speed or direction to change.

On the surface of the Earth inertia is often masked by the effects of friction and gravity, both of which tend to decrease the
speed of moving objects (commonly to the point of rest). This misled classical theorists such as Aristotle, who believed that
objects would move only as long as force was applied to them.
2A/2B BIOMECHANICS 2

nd

ed.

www.flickr.com/photos/keithallison/4062960920/

1

©PE STUDIES REVISION SEMINARSCONTENT

Introduction to Biomechanics

•What is it?

•Benefits of Biomechanics

Types of motion in Physical Activity

•Linear

•Angular

•General

Coordination of linear motion

•Types of forces

•Kinematic Chain

•Simultaneous force summation

•Sequential force summation

Stability and Balance

•Balance

•Stability

•Centre of Gravity (COG)

•Base of Support

•Factors affecting balance and stability

2CONTENT

Newton’s laws of motion

•Force production

•Newton’s 1

st

Law of motion

•Inertia

•Newton’s 2

nd

Law of motion

•Momentum
•Conservation of momentum

•Impulse

•Flattening the arc

•Newton’s 3

rd

Law of motion

Projectile motion

•Trajectory of a projectile

•Factors affecting flight of a projectile

•Angle of release

•Height of release

•Velocity at take off

•Gravity

•Air resistance

•Spin 32. SEQUENTIALLY

• Where body parts are moved in sequence to produce a force.

• Generally used to produce maximal force in whole body actions such

as throwing, kicking and striking

• E.g. A baseball pitcher, striking in golf, kicking in rugby

CO ORDINATION CONTINUUM.FORCE SUMMATION

FOR MAXIMAL OR SUBMAXIMAL FORCE

www.flickr.com/photos/flash716/2579185404/ www.flickr.com/photos/martindo/3040647348/

4

©PE STUDIES REVISION SEMINARS

HomeSUCCESSFUL SUMMATION OF FORCE/MOMENTUM

•Body parts move in a sequence to generate the largest force or

acceleration possible.

•To sequentially produce maximal force effectively, the following

principles need to be applied:

1. The stronger and larger muscles of the thighs and trunk are moved first

followed by the smaller and faster muscles

2. Sequentially accelerate each body part so that optimum momentum passes

from one body part to the next.

3. Each body part should be stable so that the next body part accelerates

around a stable base to transfer momentum
4. Use as many body parts as possible, so force can be applied over the

maximum possible time

5. Follow through is important to prevent deceleration of last segment and

safe dissipation of force.

6. Ensure all forces are directed towards the target

©PE STUDIES REVISION SEMINARS 5

HomeSEQUENTIAL SUMMATION OF FORCES - THROWING

Big body parts of legs and

trunk initiate movement

Wide base provides stable base

for acceleration of each

segment

Maximise number of segments

used

Follow through towards the

target to prevent deceleration

of final segment and maximise

momentum towards the target

©PE STUDIES REVISION SEMINARS 6

HomeDETERMINING THE CENTRE OF GRAVITY

• To determine ones COG, simply draw a box around the objects

outer extremities

• Then draw diagonal lines through the box, with the point of

intersection determining the objects approximate COG.

www.flickr.com/photos/dearlydeparted/3834132754/

7

©PE STUDIES REVISION SEMINARS

Home

Approximate

COGFACTORS AFFECTING BALANCE & STABILITY

Low COG =

↑ stability

High COG =

↓ stability

8
©PE STUDIES REVISION SEMINARS

Home

3. THE HEIGHT OF THE COG ABOVE THE BASE OF SUPPORT

• The line of gravity or pull of gravity will always pass vertically through the

centre of an object’s mass.

• The higher the centre of gravity above the base of support, the less stable

the object is. Athletes often lower their centre of gravity by bending the

knees in order to increase their stabilityMore stable                                                        Less stable

Low COG                                  Higher COG

Wide base of support – 4 point contact                         Small base of support – 2 point contact

Line of gravity in middle of support                                               Similar line of gravity

STABILITY VARIES WITH BODY POSITION

©PE STUDIES REVISION SEMINARS 9

HomeNEWTON’S 1

ST

LAW OF MOTION

Newton’s First Law of Motion - Inertia

The size of the force required to change the state of motion of an object

depends on the mass of the object. The greater the mass of the object,

the greater the force needed to move it.

The 8kg medicine ball has a

greater inertia because of its

greater mass and therefore

requires a greater force to move it

The golf ball on the left will

remain stationary on the tee until

a force (applied by the club) is

applied to it

10

©PE STUDIES REVISION SEMINARS

Home

“A body continues in its state of rest or state of motion unless acted upon by

a force”. Newton’s Second Law of Motion – acceleration / momentum

The greater the force applied to an object, the faster the acceleration will be.

Acceleration is directly proportional to the force applied.
A small force applied to a ball using

a putter results in slow acceleration

A large force applied to a ball using a

driver results in faster acceleration

NEWTON’S 2

ND

LAW OF MOTION

www.flickr.com/photos/mandj98/2567621739 www.flickr.com/photos/jae_yong/679089763/

11

©PE STUDIES REVISION SEMINARS

Home

“The rate of change of acceleration to a body is proportional to the force

applied to it”.• If all other factors are constant (i.e. Speed of release, height of release,

spin, air resistance);

©PE STUDIES REVISION SEMINARS 12

1. ANGLE OF RELEASE

Home

•An angle of less than 45⁰ results in shorter horizontal distances,

shorter vertical distances and shorter flight times

•This might be useful in the following sports;

•Throwing in softball, cricket etc, stab pass in AFL

•An angle of greater than 45⁰ results in shorter horizontal

distances , greater vertical distances and longer flight times.

•This might be useful in the following sports;

•High Jump, Pole Vault, punting in American Football

www.flickr.com/photos/stuseeger/434121246/

www.flickr.com/photos/thatpicturetakr/2461107564/sizes/l/©PE STUDIES REVISION SEMINARS 13

VERTICAL MOTION

HORIZONTAL MOTION

1. ANGLE OF RELEASE

Home

Angle of release = 45⁰

•Vertical and horizontal

velocity is equal

•Max horizontal distance
attained

Angle of release > 45⁰

•Vertical velocity is greater

than horizontal

•↑ height and flight time

•↓horizontal distance

Angle of release < 45⁰

•Horizontal velocity is

greater than vertical

•↓ height and flight time

•↓horizontal distance
Q4E Case Study 10 - Cricket Batting 1
                                           Batting is a side-on game – or at least it used t

                                                           Proposed Subject usage:

                                                Sports Science A level & 1st/2nd yr Degre
                                                     ECB Cricket Coaches Level 1 - 4

                                                GCSE / A-level Sports Science 2008 - Crick


                                                National Curriculum 2008-2009 (Key Stage

                     3. Evaluating and improving performance. Judge how good a performance
                     it
                                                      AQA GCSE PE 2009 Specification

                     6.2 Analysis of performance

                     The specification will assess a candidate‟s ability to analyse performance s

                              Determine its strengths and weaknesses
                              Improve its quality and effectiveness

                                                      AQA A Level PE 2009 Specification

                     At AS, candidates are required to observe, analyse and evaluate performan

                     21.2 Observe the chosen performer in relation to the competent performa
                     techniques for a chosen activity




Cricket Batting 1:

The demands for International cricket batsmen have changed considerably over the past ten y
matches and one day internationals is testament to this. There is no doubt in my mind that 20
increasing the range of flamboyant strokes we see today, the reverse sweep or flick over fine l
bowler. Nobody seems to play with a straight bat anymore? Batsmen are intent on working the
pick up a quick single with a bat path that only coincides with the ball for a split second… effec
justify the risks taken?

Given that batting is such an important part of the game, it is surprising that little biomechanic
the sport. The biomechanics of the off-drive and on-drive have been found to be very similar, w
execution. Grip force patterns of top & bottom hands along with kinematic analysis of selected
however, the underlying theme from the biomechanics literature is that batting has many diffe
compare the flowing and rhythmical drives of Sachin Tendulkar, Brian Lara & Sunil Gavaskar, t
Hayden & Adam Gilchrist, or the skill and determination of an Aravinda de Silva, Ricky Ponting
becoming more apparent from the research is the degree of variation the same individual has w
look at players when they first arrive at the crease and then after scoring 50+ runs, why is this
A question which I have been asked on many occasions, most notably by the late Bob Woolme
very much of the opinion that, apart from teaching a few basic fundamentals, ones batting abi
primarily by the players natural flare, athletic instinct and desire to succeed. In Bob‟s opinion,
be related back to one or more of his key fundamentals. After numerous debates with Bob on t
fundamentals must be consistent throughout all batsmen: and in coaching terminology, we mu
cricket ball. So, what are these key fundamentals? Well put simply, they are made up of Dynam
the Bat and most importantly the Path of the Bat during the stroke…

Some aspects of batting cannot be supported biomechanically, however many elite players are
techniques. The objective of this article is for all coaches to ask themselves „How do you optim
the act of striking a cricket ball as simple as possible for the player?‟. I strongly believe that bio
of every batsmen, it is the responsibility of coaches to ensure that the biomechanical informati
within an appropriate time frame... The key fundamentals are discussed below;

‘Path of the Bat & Angular Momentum’ : Many of today‟s players utilize their bottom hand
during the backswing. This is a minor modification on the traditional method when batsmen wi
the top of the backlift, the face being slightly open towards second slip.

By utilizing the bottom hand as a lever, the wrists will remain close to the centre of mass, thus
the base of support (effectively making the bat lighter). If the centre of mass of the bat can be
generated is minimal, therefore, the force required by the muscles in the forearms is reduced a
action will also decrease the rotational inertia of the system. As a result the bat will travel in a
dynamic and executed faster.

The definition for ‘Rotational Inertia’ is as follows:

A rotating rigid body (for example the bat) maintains its state of uniform rotation -
unless an external TORQUE is applied or otherwise the conservation of angular mom
momentum that an object has depends on two physical quantities:

the MASS and the VELOCITY of the moving object...

Consequently, when translated into coaching terminology, this means that the cricket bat will b
cricketer‟s centre of mass. The path of the bat on the backswing and position at the top of the
action has a chain reaction in kinematics, if the arms leave the body on the backswing, this wil
counteract this action. The correct position of the hands and bat at the top of the backswing w
movement to be produced with a greater angular acceleration, it will also enable the path to be
straight bat!

Many batsmen have a distinct loop in their backswing & downswing. As a result the bat must u
from the forearms) in order to set it onto the required plane to make contact with a straight ba
compensations may go unnoticed on a good wicket, what happens if the ball nips back off the
bat are at complete odds with each other, with only a small „contact zone‟ where the two can c
path, have to wait until after the commencement of their downswing to begin to try and redire
looking to increase stroke accuracy the longer the path of the bat is in line with the ball, the m

Figure 1 is a six-image photo sequence of Michael Vaughan (MV), Mark Ramprakash (MR), Mat
match footage is taken from the Second test, West Indies vs. England – Headingley, Leeds 25t
National Cricket Academy at Loughbrough, March 06. The red line highlights the path of the to
approximately 80mph in release speed.

Each of the six-image sequences is made up of the following events:

         Frame 1: The bowler is in the pre-delivery position. Note: All four of the players‟ hand
         Frame 2: Trigger Movement, un-weighting of the front foot - Back foot landing of the
         Frame 3: Bowler – Front Foot Contact
Frame 4: Point of Release (POR)
         Frame 5: Ball – approximately half way down the wicket - Top of Backswing
         Frame 6: Ball Impact.




                                   Figure 1: Six-image photo sequence – Quintic v14 video ana

Traditional coaching principles generally suggest that the bat should not be taken back outside
second slip. The first 2 players in the sequence (MV & MR) illustrate during frames 1-5, how th
throughout the stroke. The position of the hands directly under their shoulders enables their w
the mass of the bat remains close to the base of support. This will decrease the „ROTATIONAL
bat also remains close to the body, allowing the mass of the bat to remain close to the base of
lighter.
It can be seen from the trace of the toe of the bat, that the backswing & downswing are very s
of the backswing, thus no need to re-align the bath at the start of the downswing. This also ha
swing is based on the most current ball flight information available. A controlled bat path at the
velocity alone.

The image sequences of MP & AF also highlight in frames 1-5, their wrists remaining close to t
Although the positions of their hands are directly under their shoulders, the position and path o
out towards second slip. As a result the mass of the bat goes towards the OFF-side (Frames 2
will increase the „Rotational Inertia‟ of the system. This will have the effect of making the bat fe
toe of the bat, that the backswing & downswing are two distinct traces. Both players have a lo
align the bat & shoulders at the start of the downswing. In each case their shoulders re-align t
in a continuous rhythmical manner, as in the example of Matthew Prior, demonstrates a very li
commonly described as hitting „in to out‟… The additional forces required in the forearms, uppe
inertia and re-align the bat with the path of the ball are significant, especially with today‟s heav
align early in the downswing and bring the bat down on a good plane; however, there still is an
complicate matters on a seaming wicket.

Golf is another sport where similar mechanics applies; think of the path of the club on the back
can only think of two exceptions, Jim Furyk and Eamonn Darcy, that have a considerable loop
transition. At least with golf, the ball is stationary and the path of the club through impact area
however (as with Andrew Flower & Matthew Prior) unnecessary movements of the clubhead du
pressure and as a result be inconsistent... Figure 2 highlights the trajectory of the clubhead dri
note the backswing & downswing are on a very similar path. The slight changes at the top of t
during the swing.




                                              Figure 2: Padraig Harrington x6 image photo sequ
                                                        Quintic v14 video analysis software

Dynamic Balance – Position of Readiness? : For every action there is a reaction. If the fu
the required chaining effects of movement will not occur efficiently and effectively. The stance
about to face a delivery. It is the base to play all your shots, as the majority of coaching mater
relaxed at stance”. What is the correct stance & optimal width?

Coaching textbooks would recommend the feet approximately a foot length apart either side o
A wider base may indicate a desire to optimise stability by increasing the base of support. The
potential decline in mobility so a trade-off situation exists. In my opinion, the centre of mass of
midpoint between the feet indicating that the weight is evenly distributed on both the left & rig
evenly distributed on their heels & toes. The weight should be through your instep, or arches i
wiggle your toes, without having to change your balance. Batting is an athletic, explosive move
the best possible starting position – that of dynamic balance...

Where should the weight be positioned?

This is a great question to ask every batsman – they should be able to answer. However what
they do! Technology is needed here to give you the correct answer, force or pressure platform
accurate measurements. Traditional coaching literature would suggest the weight on the balls
reason being, that you can transfer quickly to either front or back foot depending on the length
the toes, this does in fact limit movement to the leg side; a classic example is people falling ov
deliveries…

As long as the batsmen is comfortable in their preferred starting position and any pre delivery
The most critical point during batting in terms of stability & balance is the position at which the
the ‘Position of Readiness’.

The batsmen does not know where the ball is going at POR, short, full, off side, straight or dow
bowlers‟ delivery action and even previous deliveries may influence the final outcome, yet until
With this in mind the batsmen needs to be in the optimal position to move and react to where
be still & eyes level at this point, but their posture needs to be alive and athletic. The easiest w
equal, both: 50% Right & 50% Left, and equally distributed by heels & toes - 50% Balls & 50%
POR, it is easy for the player to come forward, but you would require a double movement to go
weight is predominately on the front foot at POR – it‟s hard to come further forward, a double

A simple yet extremely affective way of ascertaining where a player‟s weight is at POR is to do
get comfortable by playing a number of different shots at various line & length, then simply on
watch carefully where is their body weight, are they moving forward, backwards, or falling to t
dynamically balanced at the point you fake to release the ball, they must be ready to react to w
putting themselves at a distinct disadvantage.

A recent football study undertaken by Quintic involved analysing English Premiership goalkeepe
The outcome has very similar connotations with batting. The goalkeepers, when saving a pena
the ball is struck, as they don‟t know where the ball will be targeted… If, for example, the goal
right-handed people do!) then, they were fine when diving to the right, but if they needed to d
right leg, move their centre of gravity over to the left before finally pushing off the left leg… by
effectively the distance they could cover on the left in the same time frame was significantly re

 Figure 3 highlights the position of the four batsmen at the point of release. (Andrew Flower is
Where do you think the weight is distributed for each of them? Are they balanced at the point
right with the same amount of effort, or do they favour one particular movement? Are they in




                                                             Figure 3: Point of Release

In two of the above examples (MP & MV) the weight distribution is predominately on the back
the opposite having the majority of weight on the front foot, only Andrew Flower has an even
MV the next frame on the video has the left foot airborne. From looking at the above example,
the heels at POR, a reaction to the toe of the bat going away from the body? Chicken or egg, w

If a player has a pre delivery trigger movement there is an opportunity to move into a more dy
releases the ball. This increase in momentum can be later utilised during the stroke. You are m
start in a balanced position. However, the movement must enable the batsmen to arrive at a b
the trigger movements. Too many players are in a poor position at POR as a result of poor tim
trigger movements (they do differ during the stages of an innings), different movements to dif
inconsistency. Have a pre-delivery movement by all means, but ensure it is consistent and you

A stable base or a position of dynamic balance at POR would ensure:

         Increased resistance to work the body levers against other body parts – summation o
         momentum to the lighter, faster moving body parts…
         Body energy transferred efficiently to the bat
         Full force generation

Finally food for thought, if you increase your stability during the position of readiness, what eff
consistency?

In summary, some aspects of elite player‟s technique can not be supported biomechanically. T
coaches to ask themselves „How do you optimise the art and science of batting whilst keeping
possible for the player?‟

Biomechanical analysis is the „why‟ something happens, it is down to the skill of the coach and
the „cause and effect‟ of the any movement they observe...

Dr Paul Hurrion
(Ph.D Sports Biomechanics)
Quintic Consultancy Ltd

ECB Level IV – Biomechanics Tutor
ICC Bowling Review Group – Biomechanics Advisor

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Principles of biomechanics

  • 1. Moment of inertia From Wikipedia, the free encyclopedia This article is about the moment of inertia of a rotating object, also termed the mass moment of inertia. For the moment of inertia dealing with the bending of a beam, also termed the area moment of inertia, see second moment of area. In classical mechanics, moment of inertia, also called mass moment of inertia, rotational inertia, polar moment of inertia of mass, or the angular mass, (SI units kg·m²) is a measure of an object's resistance to changes to its rotation. It is the inertia of a rotating body with respect to its rotation. The moment of inertia plays much the same role in rotational dynamics as mass does in linear dynamics, describing the relationship between angular momentum and angular velocity, torque and angular acceleration, and several other quantities. The symbolsI and sometimes J are usually used to refer to the moment of inertia or polar moment of inertia. While a simple scalar treatment of the moment of inertia suffices for many situations, a more advanced tensor treatment allows the analysis of such complicated systems as spinning tops and gyroscopic motion. The concept was introduced by Leonhard Euler in his book Theoria motus corporum solidorum seu rigidorum in 1765.[1] In this book, he discussed the moment of inertia and many related concepts, such as the principal axis of inertia. Contents [hide] 1 Overview 2 Scalar moment of inertia for single body 3 Scalar moment of inertia for many bodies o 3.1 Moment of inertia about a point o 3.2 Moment of inertia theorems o 3.3 Properties o 3.4 Energy, angular momentum, torque o 3.5 Examples 4 Moment of inertia tensor o 4.1 Definition o 4.2 Derivation of the tensor components o 4.3 Reduction to scalar 5 Principal axes of inertia o 5.1 Parallel axis theorem o 5.2 Rotational symmetry o 5.3 Comparison with covariance matrix 6 See also 7 Notes 8 References
  • 2. 9 External links [edit]Overview The moment of inertia of an object about a given axis describes how difficult it is to change its angular motion about that axis. Therefore, it encompasses not just how much mass the object has overall, but how far each bit of mass is from the axis. The further out the object's mass is, the more rotational inertia the object has, and the more torque (force* distance from axis of rotation) is required to change its rotation rate. For example, consider two hoops, A and B, made of the same material and of equal mass. Hoop A is larger in diameter but thinner than B. It requires more effort to accelerate hoop A (change its angular velocity) because its mass is distributed farther from its axis of rotation: mass that is farther out from that axis must, for a given angular velocity, move more quickly than mass closer in. So in this case, hoop A has a larger moment of inertia than hoop B. Divers reducing their moments of inertia to increase their rates of rotation The moment of inertia of an object can change if its shape changes. Figure skaters who begin a spin with arms outstretched provide a striking example. By pulling in their arms, they reduce their moment of inertia, causing them to spin faster (by the conservation of angular momentum). The moment of inertia has two forms, a scalar form, I, (used when the axis of rotation is specified) and a more general tensor form that does not require the axis of rotation to be specified. The scalar moment of inertia, I, (often called simply the "moment of inertia") allows a succinct analysis of many simple problems in rotational dynamics, such as objects rolling down inclines and the behavior of pulleys. For instance, while a block of any shape will slide down a frictionless decline at the same rate, rolling objects may descend at different rates, depending on their moments of inertia. A hoop will descend more slowly than a solid disk of equal mass and radius because more of its mass is located far from the axis of rotation. However, for (more complicated) problems in which the axis of rotation can change, the scalar treatment is inadequate, and the tensor treatment must be used (although shortcuts are possible in special situations). Examples requiring such a treatment include gyroscopes, tops, and even satellites, all objects whose alignment can change. The moment of inertia is also called the mass moment of inertia (especially by mechanical engineers) to avoid confusion with the second moment of area, which is sometimes called the area moment of inertia (especially by structural engineers). The easiest way to differentiate these quantities is through their units (kg·m² as opposed to m4). In addition, moment of inertia should not be confused with polar moment of inertia (more specifically, polar moment of inertia of area), which is a measure of an object's ability to resist torsion(twisting) only, although, mathematically, they are similar: if the solid for which the moment of inertia is being calculated has uniform thickness in the direction of the rotating axis, and also has uniform mass density, the difference between the two types of moments of inertia is a factor of mass per unit area.
  • 3. Inertia Inertia is the resistance of any physical object to a change in its state of motion or rest, or the tendency of an object to resist any change in its motion. The principle of inertia is one of the fundamental principles of classical physics which are used to describe the motion of matter and how it is affected by applied forces. Inertia comes from the Latin word, iners, meaning idle, or lazy. Isaac Newton defined inertia as his first law in his Philosophiæ Naturalis Principia Mathematica, which states:[1] The vis insita, or innate force of matter, is a power of resisting by which every body, as much as in it lies, endeavours to preserve its present state, whether it be of rest or of moving uniformly forward in a straight line. In common usage the term "inertia" may refer to an object's "amount of resistance to change in velocity" (which is quantified by its mass), or sometimes to its momentum, depending on the context. The term "inertia" is more properly understood as shorthand for "the principle of inertia" as described by Newton in his First Law of Motion; that an object not subject to any net external force moves at a constant velocity. Thus an object will continue moving at its current velocityuntil some force causes its speed or direction to change. On the surface of the Earth inertia is often masked by the effects of friction and gravity, both of which tend to decrease the speed of moving objects (commonly to the point of rest). This misled classical theorists such as Aristotle, who believed that objects would move only as long as force was applied to them.
  • 4. 2A/2B BIOMECHANICS 2 nd ed. www.flickr.com/photos/keithallison/4062960920/ 1 ©PE STUDIES REVISION SEMINARSCONTENT Introduction to Biomechanics •What is it? •Benefits of Biomechanics Types of motion in Physical Activity •Linear •Angular •General Coordination of linear motion •Types of forces •Kinematic Chain •Simultaneous force summation •Sequential force summation Stability and Balance •Balance •Stability •Centre of Gravity (COG) •Base of Support •Factors affecting balance and stability 2CONTENT Newton’s laws of motion •Force production •Newton’s 1 st Law of motion •Inertia •Newton’s 2 nd Law of motion •Momentum
  • 5. •Conservation of momentum •Impulse •Flattening the arc •Newton’s 3 rd Law of motion Projectile motion •Trajectory of a projectile •Factors affecting flight of a projectile •Angle of release •Height of release •Velocity at take off •Gravity •Air resistance •Spin 32. SEQUENTIALLY • Where body parts are moved in sequence to produce a force. • Generally used to produce maximal force in whole body actions such as throwing, kicking and striking • E.g. A baseball pitcher, striking in golf, kicking in rugby CO ORDINATION CONTINUUM.FORCE SUMMATION FOR MAXIMAL OR SUBMAXIMAL FORCE www.flickr.com/photos/flash716/2579185404/ www.flickr.com/photos/martindo/3040647348/ 4 ©PE STUDIES REVISION SEMINARS HomeSUCCESSFUL SUMMATION OF FORCE/MOMENTUM •Body parts move in a sequence to generate the largest force or acceleration possible. •To sequentially produce maximal force effectively, the following principles need to be applied: 1. The stronger and larger muscles of the thighs and trunk are moved first followed by the smaller and faster muscles 2. Sequentially accelerate each body part so that optimum momentum passes from one body part to the next. 3. Each body part should be stable so that the next body part accelerates around a stable base to transfer momentum
  • 6. 4. Use as many body parts as possible, so force can be applied over the maximum possible time 5. Follow through is important to prevent deceleration of last segment and safe dissipation of force. 6. Ensure all forces are directed towards the target ©PE STUDIES REVISION SEMINARS 5 HomeSEQUENTIAL SUMMATION OF FORCES - THROWING Big body parts of legs and trunk initiate movement Wide base provides stable base for acceleration of each segment Maximise number of segments used Follow through towards the target to prevent deceleration of final segment and maximise momentum towards the target ©PE STUDIES REVISION SEMINARS 6 HomeDETERMINING THE CENTRE OF GRAVITY • To determine ones COG, simply draw a box around the objects outer extremities • Then draw diagonal lines through the box, with the point of intersection determining the objects approximate COG. www.flickr.com/photos/dearlydeparted/3834132754/ 7 ©PE STUDIES REVISION SEMINARS Home Approximate COGFACTORS AFFECTING BALANCE & STABILITY Low COG = ↑ stability High COG = ↓ stability 8
  • 7. ©PE STUDIES REVISION SEMINARS Home 3. THE HEIGHT OF THE COG ABOVE THE BASE OF SUPPORT • The line of gravity or pull of gravity will always pass vertically through the centre of an object’s mass. • The higher the centre of gravity above the base of support, the less stable the object is. Athletes often lower their centre of gravity by bending the knees in order to increase their stabilityMore stable Less stable Low COG Higher COG Wide base of support – 4 point contact Small base of support – 2 point contact Line of gravity in middle of support Similar line of gravity STABILITY VARIES WITH BODY POSITION ©PE STUDIES REVISION SEMINARS 9 HomeNEWTON’S 1 ST LAW OF MOTION Newton’s First Law of Motion - Inertia The size of the force required to change the state of motion of an object depends on the mass of the object. The greater the mass of the object, the greater the force needed to move it. The 8kg medicine ball has a greater inertia because of its greater mass and therefore requires a greater force to move it The golf ball on the left will remain stationary on the tee until a force (applied by the club) is applied to it 10 ©PE STUDIES REVISION SEMINARS Home “A body continues in its state of rest or state of motion unless acted upon by a force”. Newton’s Second Law of Motion – acceleration / momentum The greater the force applied to an object, the faster the acceleration will be. Acceleration is directly proportional to the force applied.
  • 8. A small force applied to a ball using a putter results in slow acceleration A large force applied to a ball using a driver results in faster acceleration NEWTON’S 2 ND LAW OF MOTION www.flickr.com/photos/mandj98/2567621739 www.flickr.com/photos/jae_yong/679089763/ 11 ©PE STUDIES REVISION SEMINARS Home “The rate of change of acceleration to a body is proportional to the force applied to it”.• If all other factors are constant (i.e. Speed of release, height of release, spin, air resistance); ©PE STUDIES REVISION SEMINARS 12 1. ANGLE OF RELEASE Home •An angle of less than 45⁰ results in shorter horizontal distances, shorter vertical distances and shorter flight times •This might be useful in the following sports; •Throwing in softball, cricket etc, stab pass in AFL •An angle of greater than 45⁰ results in shorter horizontal distances , greater vertical distances and longer flight times. •This might be useful in the following sports; •High Jump, Pole Vault, punting in American Football www.flickr.com/photos/stuseeger/434121246/ www.flickr.com/photos/thatpicturetakr/2461107564/sizes/l/©PE STUDIES REVISION SEMINARS 13 VERTICAL MOTION HORIZONTAL MOTION 1. ANGLE OF RELEASE Home Angle of release = 45⁰ •Vertical and horizontal velocity is equal •Max horizontal distance
  • 9. attained Angle of release > 45⁰ •Vertical velocity is greater than horizontal •↑ height and flight time •↓horizontal distance Angle of release < 45⁰ •Horizontal velocity is greater than vertical •↓ height and flight time •↓horizontal distance
  • 10.
  • 11. Q4E Case Study 10 - Cricket Batting 1 Batting is a side-on game – or at least it used t Proposed Subject usage: Sports Science A level & 1st/2nd yr Degre ECB Cricket Coaches Level 1 - 4 GCSE / A-level Sports Science 2008 - Crick National Curriculum 2008-2009 (Key Stage 3. Evaluating and improving performance. Judge how good a performance it AQA GCSE PE 2009 Specification 6.2 Analysis of performance The specification will assess a candidate‟s ability to analyse performance s Determine its strengths and weaknesses Improve its quality and effectiveness AQA A Level PE 2009 Specification At AS, candidates are required to observe, analyse and evaluate performan 21.2 Observe the chosen performer in relation to the competent performa techniques for a chosen activity Cricket Batting 1: The demands for International cricket batsmen have changed considerably over the past ten y matches and one day internationals is testament to this. There is no doubt in my mind that 20 increasing the range of flamboyant strokes we see today, the reverse sweep or flick over fine l bowler. Nobody seems to play with a straight bat anymore? Batsmen are intent on working the pick up a quick single with a bat path that only coincides with the ball for a split second… effec justify the risks taken? Given that batting is such an important part of the game, it is surprising that little biomechanic the sport. The biomechanics of the off-drive and on-drive have been found to be very similar, w execution. Grip force patterns of top & bottom hands along with kinematic analysis of selected however, the underlying theme from the biomechanics literature is that batting has many diffe compare the flowing and rhythmical drives of Sachin Tendulkar, Brian Lara & Sunil Gavaskar, t Hayden & Adam Gilchrist, or the skill and determination of an Aravinda de Silva, Ricky Ponting becoming more apparent from the research is the degree of variation the same individual has w look at players when they first arrive at the crease and then after scoring 50+ runs, why is this
  • 12. A question which I have been asked on many occasions, most notably by the late Bob Woolme very much of the opinion that, apart from teaching a few basic fundamentals, ones batting abi primarily by the players natural flare, athletic instinct and desire to succeed. In Bob‟s opinion, be related back to one or more of his key fundamentals. After numerous debates with Bob on t fundamentals must be consistent throughout all batsmen: and in coaching terminology, we mu cricket ball. So, what are these key fundamentals? Well put simply, they are made up of Dynam the Bat and most importantly the Path of the Bat during the stroke… Some aspects of batting cannot be supported biomechanically, however many elite players are techniques. The objective of this article is for all coaches to ask themselves „How do you optim the act of striking a cricket ball as simple as possible for the player?‟. I strongly believe that bio of every batsmen, it is the responsibility of coaches to ensure that the biomechanical informati within an appropriate time frame... The key fundamentals are discussed below; ‘Path of the Bat & Angular Momentum’ : Many of today‟s players utilize their bottom hand during the backswing. This is a minor modification on the traditional method when batsmen wi the top of the backlift, the face being slightly open towards second slip. By utilizing the bottom hand as a lever, the wrists will remain close to the centre of mass, thus the base of support (effectively making the bat lighter). If the centre of mass of the bat can be generated is minimal, therefore, the force required by the muscles in the forearms is reduced a action will also decrease the rotational inertia of the system. As a result the bat will travel in a dynamic and executed faster. The definition for ‘Rotational Inertia’ is as follows: A rotating rigid body (for example the bat) maintains its state of uniform rotation - unless an external TORQUE is applied or otherwise the conservation of angular mom momentum that an object has depends on two physical quantities: the MASS and the VELOCITY of the moving object... Consequently, when translated into coaching terminology, this means that the cricket bat will b cricketer‟s centre of mass. The path of the bat on the backswing and position at the top of the action has a chain reaction in kinematics, if the arms leave the body on the backswing, this wil counteract this action. The correct position of the hands and bat at the top of the backswing w movement to be produced with a greater angular acceleration, it will also enable the path to be straight bat! Many batsmen have a distinct loop in their backswing & downswing. As a result the bat must u from the forearms) in order to set it onto the required plane to make contact with a straight ba compensations may go unnoticed on a good wicket, what happens if the ball nips back off the bat are at complete odds with each other, with only a small „contact zone‟ where the two can c path, have to wait until after the commencement of their downswing to begin to try and redire looking to increase stroke accuracy the longer the path of the bat is in line with the ball, the m Figure 1 is a six-image photo sequence of Michael Vaughan (MV), Mark Ramprakash (MR), Mat match footage is taken from the Second test, West Indies vs. England – Headingley, Leeds 25t National Cricket Academy at Loughbrough, March 06. The red line highlights the path of the to approximately 80mph in release speed. Each of the six-image sequences is made up of the following events: Frame 1: The bowler is in the pre-delivery position. Note: All four of the players‟ hand Frame 2: Trigger Movement, un-weighting of the front foot - Back foot landing of the Frame 3: Bowler – Front Foot Contact
  • 13. Frame 4: Point of Release (POR) Frame 5: Ball – approximately half way down the wicket - Top of Backswing Frame 6: Ball Impact. Figure 1: Six-image photo sequence – Quintic v14 video ana Traditional coaching principles generally suggest that the bat should not be taken back outside second slip. The first 2 players in the sequence (MV & MR) illustrate during frames 1-5, how th throughout the stroke. The position of the hands directly under their shoulders enables their w the mass of the bat remains close to the base of support. This will decrease the „ROTATIONAL bat also remains close to the body, allowing the mass of the bat to remain close to the base of lighter.
  • 14. It can be seen from the trace of the toe of the bat, that the backswing & downswing are very s of the backswing, thus no need to re-align the bath at the start of the downswing. This also ha swing is based on the most current ball flight information available. A controlled bat path at the velocity alone. The image sequences of MP & AF also highlight in frames 1-5, their wrists remaining close to t Although the positions of their hands are directly under their shoulders, the position and path o out towards second slip. As a result the mass of the bat goes towards the OFF-side (Frames 2 will increase the „Rotational Inertia‟ of the system. This will have the effect of making the bat fe toe of the bat, that the backswing & downswing are two distinct traces. Both players have a lo align the bat & shoulders at the start of the downswing. In each case their shoulders re-align t in a continuous rhythmical manner, as in the example of Matthew Prior, demonstrates a very li commonly described as hitting „in to out‟… The additional forces required in the forearms, uppe inertia and re-align the bat with the path of the ball are significant, especially with today‟s heav align early in the downswing and bring the bat down on a good plane; however, there still is an complicate matters on a seaming wicket. Golf is another sport where similar mechanics applies; think of the path of the club on the back can only think of two exceptions, Jim Furyk and Eamonn Darcy, that have a considerable loop transition. At least with golf, the ball is stationary and the path of the club through impact area however (as with Andrew Flower & Matthew Prior) unnecessary movements of the clubhead du pressure and as a result be inconsistent... Figure 2 highlights the trajectory of the clubhead dri note the backswing & downswing are on a very similar path. The slight changes at the top of t during the swing. Figure 2: Padraig Harrington x6 image photo sequ Quintic v14 video analysis software Dynamic Balance – Position of Readiness? : For every action there is a reaction. If the fu the required chaining effects of movement will not occur efficiently and effectively. The stance about to face a delivery. It is the base to play all your shots, as the majority of coaching mater relaxed at stance”. What is the correct stance & optimal width? Coaching textbooks would recommend the feet approximately a foot length apart either side o A wider base may indicate a desire to optimise stability by increasing the base of support. The potential decline in mobility so a trade-off situation exists. In my opinion, the centre of mass of midpoint between the feet indicating that the weight is evenly distributed on both the left & rig evenly distributed on their heels & toes. The weight should be through your instep, or arches i wiggle your toes, without having to change your balance. Batting is an athletic, explosive move the best possible starting position – that of dynamic balance... Where should the weight be positioned? This is a great question to ask every batsman – they should be able to answer. However what they do! Technology is needed here to give you the correct answer, force or pressure platform accurate measurements. Traditional coaching literature would suggest the weight on the balls
  • 15. reason being, that you can transfer quickly to either front or back foot depending on the length the toes, this does in fact limit movement to the leg side; a classic example is people falling ov deliveries… As long as the batsmen is comfortable in their preferred starting position and any pre delivery The most critical point during batting in terms of stability & balance is the position at which the the ‘Position of Readiness’. The batsmen does not know where the ball is going at POR, short, full, off side, straight or dow bowlers‟ delivery action and even previous deliveries may influence the final outcome, yet until With this in mind the batsmen needs to be in the optimal position to move and react to where be still & eyes level at this point, but their posture needs to be alive and athletic. The easiest w equal, both: 50% Right & 50% Left, and equally distributed by heels & toes - 50% Balls & 50% POR, it is easy for the player to come forward, but you would require a double movement to go weight is predominately on the front foot at POR – it‟s hard to come further forward, a double A simple yet extremely affective way of ascertaining where a player‟s weight is at POR is to do get comfortable by playing a number of different shots at various line & length, then simply on watch carefully where is their body weight, are they moving forward, backwards, or falling to t dynamically balanced at the point you fake to release the ball, they must be ready to react to w putting themselves at a distinct disadvantage. A recent football study undertaken by Quintic involved analysing English Premiership goalkeepe The outcome has very similar connotations with batting. The goalkeepers, when saving a pena the ball is struck, as they don‟t know where the ball will be targeted… If, for example, the goal right-handed people do!) then, they were fine when diving to the right, but if they needed to d right leg, move their centre of gravity over to the left before finally pushing off the left leg… by effectively the distance they could cover on the left in the same time frame was significantly re Figure 3 highlights the position of the four batsmen at the point of release. (Andrew Flower is Where do you think the weight is distributed for each of them? Are they balanced at the point right with the same amount of effort, or do they favour one particular movement? Are they in Figure 3: Point of Release In two of the above examples (MP & MV) the weight distribution is predominately on the back the opposite having the majority of weight on the front foot, only Andrew Flower has an even MV the next frame on the video has the left foot airborne. From looking at the above example,
  • 16. the heels at POR, a reaction to the toe of the bat going away from the body? Chicken or egg, w If a player has a pre delivery trigger movement there is an opportunity to move into a more dy releases the ball. This increase in momentum can be later utilised during the stroke. You are m start in a balanced position. However, the movement must enable the batsmen to arrive at a b the trigger movements. Too many players are in a poor position at POR as a result of poor tim trigger movements (they do differ during the stages of an innings), different movements to dif inconsistency. Have a pre-delivery movement by all means, but ensure it is consistent and you A stable base or a position of dynamic balance at POR would ensure: Increased resistance to work the body levers against other body parts – summation o momentum to the lighter, faster moving body parts… Body energy transferred efficiently to the bat Full force generation Finally food for thought, if you increase your stability during the position of readiness, what eff consistency? In summary, some aspects of elite player‟s technique can not be supported biomechanically. T coaches to ask themselves „How do you optimise the art and science of batting whilst keeping possible for the player?‟ Biomechanical analysis is the „why‟ something happens, it is down to the skill of the coach and the „cause and effect‟ of the any movement they observe... Dr Paul Hurrion (Ph.D Sports Biomechanics) Quintic Consultancy Ltd ECB Level IV – Biomechanics Tutor ICC Bowling Review Group – Biomechanics Advisor Downloads Written Case Study ~0.8 MB