ocr a level physical education a 7875 next previous module 2565 b1.2.1 ocr examinations a level...
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Module 2565 B1.2.1
OCR A Level Physical Education A 7875
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OCR ExaminationsA Level Physical Education
A 7875
Module 2565 : Option B1part 2
Biomechanical Analysis of Human Movement
Module 2565 B1.2.2
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INDEX27 - LEVERS28 - CLASSIFICATION OF LEVERS29 - EFFICIENCY OF LEVERS30 - MOMENT OF FORCE - TORQUE - PRINCIPLE of
MOMENTS31 - CALCULATION OF EFFORT IN MUSCLE FORCE IN TRICEPS MUSCLE a worked example32 - PRINCIPAL AXES OF ROTATION - BODY PLANES &
AXES 33 - BODY PLANES FOR MOVEMENT34 - ANGULAR MOTION - TORQUE MOMENT OF FORCE / TORQUE / COUPLE35 - ANGULAR MOTION - ANALOGUES OF NEWTON’s
LAWS36 - ANGLE - ANGULAR DISPLACEMENT37 - ANGULAR VELOCITY38 - ANGULAR ACCELERATION39 - MOMENT OF INERTIA40 - MOMENT OF INERTIA41 - MOMENT OF INERTIA - The SPRINTER’S LEG42 - CONSERVATION OF ANGULAR MOMENTUM ANGULAR MOMENTUM CONSERVATION of ANGULAR MOMENTUM43 - CONSERVATION OF ANGULAR MOMENTUM -
EXAMPLES THE SPINNING SKATER / THE TUMBLING
GYMNAST44 - CONSERVATION OF ANGULAR MOMENTUM -
EXAMPLES DANCER - SPIN JUMP / THE SLALOM 45 - CONSERVATION OF ANGULAR MOMENTUM -
EXAMPLES THE LONG JUMPER - BEFORE TAKE-OFF
Index
3 - IMPULSE4 - IMPULSE - FOLLOW THROUGH5 - IMPULSE - FORCE TIME GRAPHS6 - IMPULSE - CALCULATION OF VELOCITY OF STRUCK BALL7 - WORK AND ENERGY - WORK8 - WORK AND ENERGY - ENERGY9 - APPLICATIONS OF WORK FORMULA
WORK FORMULA APPLIED TO THROWS10 - APPLICATIONS OF WORK FORMULA11 - APPLICATIONS OF WORK FORMULA
BOB SLEIGH START12 - POWER13 - PROJECTILES - PROJECTILES AND YOUR PPP14 - RELEASE15 - FLIGHT16 - FLIGHT - WEIGHT17 - FLIGHT - RELATIVE SIZE OF FORCES18 - FLIGHT - LARGE AIR RESISTANCE19 - FLIGHT - THE BERNOULLI EFFECT20 - FLIGHT AND LIFT - LIFT FORCES21 - SPIN - THE MAGNUS EFFECT22 - BOUNCING BALLS WITH SPIN23 - CENTRE OF MASS - WHERE IS THE CENTRE OF MASS?24 - BALANCE and TOPPLING25 - CENTRE OF MASS - GENERATION OF ROTATION
FORCE ACTING AT TAKE-OFF THROUGH CoM26 - CENTRE OF MASS - GENERATION OF ROTATION
FORCE ACTING AT TAKE-OFF NOT THROUGH CoM
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IMPULSE
IMPULSE • another concept derived from Newton's second
law
• impulse = total change of momentum• = force x time• useful when large forces are applied for short
times
• examples of use of impulse :– fielder catching a hard cricket ball– bat, racquet, stick, golf club striking a ball– footballer kicking a ball
Impulse
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IMPULSE
IMPULSE• = force x time
• when a bat strikes a ball, a large force is applied to the ball for a short time
• follow through when striking a ball :– increases time of contact– therefore increases impulse– therefore increases final momentum (and hence the
speed) of struck ball
• the turn in the discus throw– increases the time over which force is applied– therefore increases the impulse– and increases the final momentum of the discus– hence increases the speed of release and the distance
thrown
Impulse
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IMPULSE
FORCE TIME GRAPHS• the area under this graph is the impulse
• the graph below represents the force time graph for the force between foot and ground during a foot strike when sprinting
• the bigger the area – the bigger the impulse– and the greater the change of
momentum of the runner– the greater the acceleration
Impulse
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IMPULSE
CALCULATION OF VELOCITY OF STRUCK BALL
• estimate the area under the force time graph• this is the impulse, I = Ft• and I = change of momentum of the ball, =
mv
• divide by the mass of the ball gives you the change in velocity of the ball, = v
• subtract incoming velocity (= - u) (remember to make it negative if ball travels towards the bat)
• final velocity v = v - (- u)
Impulse
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WORK AND ENERGY
WORK• is the scientific form of mechanical energy• work = force x distance moved in direction of force• unit the joule J
• example :– work done on a cycle ergometer– work = force x distance moved– force = weight hung from wheel in Newtons (the
weight will be 10 N per kg mass)– distance = circumference of wheel x number of
revolutions of wheel– answer in joules
Work and Power
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WORK AND ENERGY
ENERGY• work is the same thing as energy• work is the energy used for exerting forces (i.e.
mechanical energy)
• energy for physical activity comes from chemical fuel foods
• the chemical reaction which converts this energy into work is a complex biochemical / physiological process involving ATP, glucose, and oxygen
• kinetic energy (KE) is energy due to movement
Work and Power
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APPLICATIONS OF WORK FORMULA
WORK FORMULA APPLIED TO THROWS• work = force x distance• this work is provided by energy converted from food
fuel in the body
• the throwing action converts this work into kinetic energy (KE = energy of movement) of the thrown object
• therefore to maximise this KE, the thrower must maximise :– the force applied to the implement throughout the
throw– by doing strength training– and the distance over which the force is applied– by learning the technique of the throw– and doing flexibility training
Work and Power
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APPLICATIONS OF WORK FORMULA
Work and Power
FORCE DISTANCE GRAPH• work = force x distance• the area under the force time graph is equal to the work
done by the force over the distance
• in the case of the thrower this work is converted into kinetic energy (KE)
• the formula for KE = 1 m v2 2
• this formula enables you to work out the release velocity of the thrown implement
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APPLICATIONS OF WORK FORMULA
BOB SLEIGH START• the work formula is relevant• because force is applied over a
distance
• the work done by the pushers is converted into kinetic energy of the sleigh + bobsleighmen
• work = force x distance
• therefore maximum possible force has to be exerted over the maximum possible distance during the shove
Work and Power
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POWER
POWER• = rate of doing work
= rate of using energy= work done or energy used
time taken • unit the watt W
• power = force x speed (another definition)• a powerful sportsperson can apply force at
speed
• example : to find a person's power running upstairs– he exerts a force = weight of
person– through a distance = height
moved– work = weight (N) x height (m) (ans J)
= potential energy gained by person
– power = work (ans W) time taken to run upstairs
Work and Power
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PROJECTILES
PROJECTILES• the motion of objects in flight
– human bodies– shot / discus / javelin /
hammer– soccer / rugby / cricket
tennis / golf balls
• is governed by the forces acting– weight– air resistance– Magnus effect– aerodynamic lift
• and the direction of motion
PROJECTILES AND YOUR PPP• you should include an analysis
of any relevant projectile motion in your chosen sports in your PPP
• include analysis of– release conditions– forces likely to be acting– spin– flight pattern or path
Projectile Motion
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RELEASE
Projectile Motion
DI STAN CETR AVELLED BY
PR OJ ECTI LE
angle ofrelease
height ofrelease
speed ofrelease
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FLIGHT
Projectile Motion
FOR CES ACTI NG
w eight airresistance
aerodynam iclift
M agnuseff ect
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FLIGHTWEIGHT• weight will always act on a body in flight• the amount to which weight is a predominant force acting
governs the shape of the flight path• if weight were the only force acting then the shape of the flight
path would be a parabola• some flight paths are similar to this
– shot / hammer– human body in jumps / tumbles / dives
Projectile Motion
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FLIGHT
RELATIVE SIZE OF FORCES• the faster the projectile travels the
greater will be air resistance
• aerodynamic lift applies to– thrown objects with a wing shape
profile– javelin / discus / rugby ball /
American football / frisbee
• the Magnus effect applies to spinning balls
• if the shapes of the flight path differ from a parabola then some combination of these forces must be relatively large compared with the weight
Projectile Motion
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FLIGHTLARGE AIR RESISTANCE• example :
– badminton shuttle struck hard
– the air resistance is very large compared with the weight
– the resultant force is very close to the air resistance
Projectile Motion
• the shuttle would slow down rapidly over the first part of the flight
• later in the flight of a badminton shuttle :– now the air resistance is much
less– and comparable with the weight
• This pattern of the resultant force changing markedly during the flight
• predicts a markedly asymmetric path
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FLIGHT - THE BERNOULLI EFFECT
BERNOULLI EFFECT • is the effect that enables
aerofoils to fly
• caused by reduction in pressure on a surface across which a fluid moves
• the greater the speed, the bigger the pressure difference, the greater the force
• this effect is used in sport :– inverted wings on racing
cars– create down-force– which then increases
friction for cornering
• as layers of air flow past the wing
• the layers under the wing flow further and faster than those over the top of the wing
Projectile Motion
• this causes reduced pressure under the wing
• and hence a downward force
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FLIGHT AND LIFT
LIFT FORCES• these forces are caused by bulk
displacement of fluid and are similar to air resistance
• a wing shaped object moves through the air– discus– ski jumper
Projectile Motion
• as it moves forward and falls through the air, it pushes aside the air
• creating a higher pressure underneath the object
• and a lower pressure over the top of the object
• and creates a lift force
• this force is similar to the force which enables a stone to skip over the surface of water
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SPIN
THE MAGNUS EFFECT• this is the Bernoulli effect applied
to spinning (swerving) balls• the spin takes more layers of air
the long way round the ball• this means that the air travels
faster round this part of the ball
Projectile Motion
• therefore there is a reduction in pressure on this side of the ball
• this causes the Magnus effect force as shown
• the direction of swerve of spinning ball is therefore in the same sense as the direction of spin
• back spin - soar• top spin - dip• side spin - slice and hook• soccer free-kicks - swerving
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BOUNCING BALLS WITH SPIN
BOUNCING BALLS• as a ball bounces there is friction
between the lowest point of the ball and the ground
• if the ball is spinning, this friction can be increased or reduced
• a ball with back spin will have increased backwards friction with the ground which will cause the ball to bounce backwards form its normal path
Projectile Motion
• a ball with top spin will have friction driving forwards on the ball - making the ball travel forward of its normal path
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CENTRE OF MASS
CENTRE of MASS (CoM)• this is the single point in a body which represents all
the spread out mass of a body
WHERE IS THE CENTRE OF MASS?
• position of centre of mass depends on shape of body
• this is how the high jumper can have his CoM pass under the bar
• but he could still clear the bar
Centre of Mass
• the weight acts at the CoM since gravity acts on mass to produce weight
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BALANCE and TOPPLING
BALANCE• to keep on balance the CoM must
be over the base of support
TOPPLING• the CoM must be over the base of
support if a person is to be on balance
• toppling would be caused by the weight acting at the CoM creating a moment about the near edge of the base of support
• this can be used by divers or gymnasts to initiate a controlled spinning (twisting) fall and lead into somersaults or twists
Centre of Mass
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CENTRE OF MASS - GENERATION OF ROTATION
Centre of Mass
FORCE ACTING AT TAKE-OFF THROUGH CoM
• the line of action of a force on a jumper before take-off determines whether or not he rotates in the air after take off
• if a force acts directly through the centre of mass of an object, then linear acceleration will occur (Newton's second law), no turning or rotating
• example : – basketballer : force acts through CoM
therefore jumper does not rotate in air
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CENTRE OF MASS - GENERATION OF ROTATION
FORCE ACTING AT TAKE-OFF NOT THROUGH CoM
• a force which acts eccentrically to the centre of mass of a body will cause the body to begin to rotate (will initiate angular acceleration)
• this is because the force will have a moment about the CoM and will cause turning
• example : – high jumper : force acts to one side
of CoM therefore jumper turns in air
Centre of Mass
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LEVERS
LEVERS • levers have an pivot (fulcrum),
effort and load
Body Levers
J O I NTS ASLEVER S
eff ort inm uscle
load is forceapplied
pivot atjoint
class 1E-P-L
class 3L-E-P
class 2E-L-P
• and are a means of applying forces at a distance from the source of the force
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CLASSIFICATION OF LEVERS
Body Levers
CLASSIFICATION OF LEVERS
• class 1 lever : pivot between effort and load• see-saw lever found rarely in the body• example : triceps / elbow
• class 2 lever : load between pivot and effort• wheelbarrow lever, load bigger than effort• example : calf muscle / ankle
• class 3 lever : effort between pivot and load• mechanical disadvantage, effort bigger than
load, most common system found in body• example : quads / knee and biceps / elbow
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EFFICIENCY OF LEVERS
Body Levers
EFFI C I ENCY OFLEVER S
angle betw eeneffort and lever
arm
length oflever arm
distance betw eeneffort andfulcrum
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MOMENT OF FORCE - TORQUE
MOMENT of a FORCE (TORQUE) PRINCIPLE of MOMENTS
• this law applies when a lever is balanced
• (When the arms of the lever are not accelerating)
• moments tend to turn a lever arm :– clockwise (CW) – or anticlockwise (ACW)
• anticlockwise moment = clockwise
moment
Moment of Force
• moment = force x distance from pivot to line of action of force
• unit newton metre Nm• example :
– moment = F x d– d measured at right angles to
F
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CALCULATION OF EFFORT IN MUSCLE
FORCE IN TRICEPS MUSCLE a worked example
Moment of Force
• load (weight in hand is 20 kg) = 20 x 10 (each kg weighs 10 N) = 200 N
• distance of load to pivot (hand to elbow joint) = 0.3 m• anticlockwise moment (of load) = 200 x 0.3
= 60 Nm• distance of effort from pivot (triceps muscle insertion to elbow
joint) = 0.02 m• clockwise moment (of effort) = effort x 0.02• ACW moment = CW moment• 60 Nm = effort x 0.02• therefore effort = 60
0.02 • effort = force in triceps muscle = 3000 N
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PRINCIPAL AXES OF ROTATION
BODY PLANES & AXES • plane - an imaginary flat surface through the body
• axis of rotation- an imaginary line about which the body rotates or spins, at right angles to the plane
• vertical / longitudinal axis (V)- whole body movements - twisting /
turning, spinning skater / discus / hammer / ski turns
Principal Axes of Rotation
• frontal axis (F)- whole body movements include somersaults, pole vault take off, sprinting
• sagittal / transverse axis (S) - whole body movements include cartwheel
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BODY PLANES FOR MOVEMENT
Principal Axes of Rotation
PLANES :• frontal - divides body into front and back sections :
abduction, adduction, lateral flexion• - whole body movements include cartwheel
• sagittal - divides the body into left and right sections : flexion, extension, dorsiflexion plantarflexion
• - whole body movements include somersaults, pole vault take off, sprinting
• transverse - divides the body into upper and lower sections : medial / lateral rotation,
supination, pronation • - whole body movements - twisting /
turning, spinning skater / discus / hammer / ski turns
• as a student you will have to identify the major planes and axes in physical activity
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ANGULAR MOTION - TORQUE
MOMENT OF FORCETORQUECOUPLE• these are all terms which describe
the turning effect produced by a force
• when it acts eccentrically (to one side of) to an axis of rotation
• moment = F x d
Angular Motion
• such a moment would cause rotation / turning
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ANGULAR MOTIONANALOGUES OF NEWTON’s LAWS
NEWTON’s 1ST LAW• rate of spinning will remain the same provided
no torque acts• strictly - angular momentum remains the same
(is conserved)• see later for explanation of angular momentum
NEWTON’s 2ND LAW• if a torque acts on a spinning system then this
will change the angular velocity of the system• the rate of spinning will speed up or slow
down
NEWTON’s 3RD LAW• if a torque acts from one body onto another• then the first experiences an equal and
opposite torque in the opposite direction
Angular Motion
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ANGLE - ANGULAR DISPLACEMENT
ANGLE (ANGULAR DISPLACEMENT)• to be scientifically correct angle should not be
measured in degrees, but in RADIANS (r)
• angle = arc length = l radius of arc
r
Angular Motion - Measurements
• 360 degrees = 2 x radians = 6.28 radians– 180o = r = 3.14 r– 90o = 1/2 r = 1.57 r– 30o = 1/6 r = 0.52 r
• and so on (see maths text book for more)
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ANGULAR VELOCITY
ANGULAR VELOCITY• = angle turned through per second = angle turned through =
time taken t
= Greek letter omega
Angular Motion - Measurements
• this is rate of spin, most easily understood as revolutions per second (revs per sec)
• revs per sec would have to be converted to the unit radians per second (rs-1) for calculations
• 1 rev per second = 2 x = 6.28 rs-1
• rates of spin apply to :– tumbling gymnasts– trampolinists (piked straight and tucked
somersaults) – discus and hammer throwers– spinning skaters– skiers turning and twisting between slalom gates
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ANGULAR ACCELERATION
ANGULAR ACCELERATION• rate of change of angular velocity
• angular acceleration = change of angular
velocity time taken
• A =2 - 1 t
• note similarity of formula with linear motion
• used when rates of spin increase or decrease
• example :– hammer thrower
Angular Motion - Measurements
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MOMENT OF INERTIA
MOMENT OF INERTIA (MI)• the equivalent of mass for rotating systems• rotational inertia
• objects rotating with large MI require large moments of forces / torque to change their angular velocity
• objects with small MI require small moments of force / torque to change their angular velocity or
• MI depends on the spread of mass away from the axis of spin, hence body shape
• the more spread out the mass, the bigger the MI
• unit kilogramme metre squared kgm2
Angular Motion - Moment of Inertia
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MOMENT OF INERTIAMOMENT OF INERTIA (MI)• MI = Mr2
• MI depends on the spread of mass away from the axis of spin, hence body shape
• the more spread out the mass, the bigger the MI
• bodies with arms held out wide have large MI• the further the mass is away from the axis of
rotation increases the MI dramatically
Angular Motion - Moment of Inertia
• sportspeople use this to control all spinning or turning movements• pikes and tucks are good examples of use of MI, both reduce MI• in the diagram, I is the MI for the left most pin man, and I has a
value of about 1 kgm2 for an average person
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MOMENT OF INERTIA
The SPRINTER’S LEG• when the leg is straight, the leg
has high MI about hip as axis• therefore requires large force /
torque in groin muscle to swing leg
Angular Motion - Moment of Inertia
• on the other hand when fully bent the leg has low MI
• therefore requires low force / torque in groin muscle to swing leg
• so a sprinter tends to bring the leg through as bent as possible (heel as close to backside as possible)
• this is easier and faster the more bent the leg
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CONSERVATION OF ANGULAR MOMENTUM
ANGULAR MOMENTUM (H)• angular momentum = moment of inertia x angular
velocity = rotational inertia x rate of spin• H = I x
CONSERVATION of ANGULAR MOMENTUM• this is a law of the universe which says that angular momentum of a
spinning body remains the same (provided no external forces act)• a body which is spinning / twisting / tumbling will keep its value of H
once the movement has started
• therefore if MI (I) changes by changing body shape• then must also change to keep angular momentum (H) the same• if MI (I) increases (body spread out more) then must decrease (rate
of spin gets less)
Conservation of Angular Momentum
• strictly, this is only exactly true if the body has no contact with its surroundings, as for example a high diver doing piked or tucked somersaults in the air
• but it is almost true for the spinning skater !
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CONSERVATION OF ANGULAR MOMENTUM - EXAMPLES
THE SPINNING SKATER• arms wide - MI large - spin slowly• arms narrow - MI small - spin
quickly
Conservation of Angular Momentum
THE TUMBLING GYMNAST• body position open - MI large -
spin slowly• body position tucked - MI small -
spin quickly
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CONSERVATION OF ANGULAR MOMENTUM - EXAMPLES
DANCER - SPIN JUMP• the movement is initiated with arms
held wide - highest possible MI• once she has taken off, angular
momentum is conserved• flight shape has arms tucked across
chest - lowest possible MI• therefore highest possible rate of
spin
Conservation of Angular Momentum
THE SLALOM SKIER• slalom skier crouches on approach
to gate therefore with large turning MI
• as he / she passes the gate he / she stands straight up (reducing MI)
• so turns rapidly past the gate, then crouches again (increasing MI)
• to resume slow turn between gates
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CONSERVATION OF ANGULAR MOMENTUM - EXAMPLES
THE LONG JUMPER
BEFORE TAKE-OFF• the jumper has an upward reaction
force acting on his / her take-off foot• which acts eccentrically to the CoM• and therefore causes clockwise
rotation of the jumper’s body after take-off
Conservation of Angular Momentum
AFTER TAKE-OFF• the jumper would rotate forwards
and land on his / her face• unless he / she could minimise the
rate of rotation
• this is done by making the MI as big as possible
• as in the hang or sail technique