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Kinesiology

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Kinesiology. Chapter Outline.  The musculoskeletal system.  Human strength and power.  Sources of resistance to muscle contraction.  Joint biomechanics: concerns in lifting.  Movement analysis and exercise prescription. Muscle Pulling Force Manifested As a Pushing Force. - PowerPoint PPT Presentation
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Page 1: Kinesiology

Kinesiology

Page 2: Kinesiology

Chapter Outline

The musculoskeletal system

Human strength and power

Sources of resistance to muscle contraction

Joint biomechanics: concerns in lifting

Movement analysis and exercise prescription

Page 3: Kinesiology

Muscle Pulling Force Manifested As a Pushing Force

Page 4: Kinesiology

Muscle Pulling Force Manifested As a Pulling Force

Page 5: Kinesiology

Front View of Adult Male Human Skeleton

Page 6: Kinesiology

Rear View of Adult Male Human Skeleton

Page 7: Kinesiology

The Vertebral Column

Page 8: Kinesiology

Front View of Adult Male Human Skeletal Musculature

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Rear View of Adult Male Human Skeletal Musculature

Page 10: Kinesiology

A Lever

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A First-Class Lever (The Forearm)

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A Second-Class Lever (The Foot)

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A Third-Class Lever (The Forearm)

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Lever Systems

• Classified systems of torque• Relative positions of force, resistance, and axis

of rotation vary in the different types or classes of levers

Page 15: Kinesiology

Classes of Levers

1. First Class – The applied force and the resistance are on opposite sides of the fulcrum.

2. Second Class – The resistance is between the applied force and the fulcrum.

3. Third Class – The applied force is between the resistance and the fulcrum.

Page 16: Kinesiology

First Class Lever

fulcrum

applied force

resistance armresistance

force arm

Page 17: Kinesiology

Second Class Lever

fulcrum

resistanceapplied

force

resistance arm

force arm

Page 18: Kinesiology

Third Class Lever

fulcrum

resistance

applied force

resistance arm

force arm

Page 19: Kinesiology

Levers In The Musculo-Skeletal System

• Most are third class levers• This system produces a disadvantage for force

but an advantage for speed of movement

Page 20: Kinesiology

DFA

DRA

FM

R

FRO

Levers In The Musculo-Skeletal System

Most of the musculo-skeletal system consists of third class levers.

The resistance arm is longer than the force arm.

Page 21: Kinesiology

Levers In The Musculo-Skeletal System

A

B

The musculo-skeletal lever systems generally favor speed over strength.

In the time that the muscle insertion moves a given distance (red arrow), the resistance moves a much greater distance (blue arrow).

Page 22: Kinesiology

Levers In The Musculo-Skeletal System

A

B

In other words, the end of a limb is moving at a greater velocity than the attachments of the muscles that produce that movement.

Page 23: Kinesiology

Strength vs. Speed in Skeletal Muscle

• In a muscle contraction acting on a limb the resistance moves through the same angular displacement as the muscle insertion.

• The angular velocity of the muscle insertion (A) is equal to the angular velocity of the load (B)

q

AB

Page 24: Kinesiology

Strength vs. Speed in Skeletal Muscle

DFADRA

FM

R

FRO

If DFA = 3 cm and DRA = 30 cm• The relative speed of the resistance to the muscle insertion = DRA/DFA = (30 cm)/(3 cm)

= 10• This means that the resistance is moving at 10 times the velocity of the muscle

insertion

Page 25: Kinesiology

Levers in the Musculo-Skeletal System

• Not all levers in the musculo-skeletal system are third class.

• When performing toe rises the ankle becomes a second class lever system.

fulcrum

DRA

DFA

R

FM

Page 26: Kinesiology

Most of the skeletal muscles operate at a

considerable mechanical disadvantage. Thus, during

sports and other physical activities, forces in the muscles

and tendons are much higher than those exerted by the

hands or feet on external objects or the ground.

Page 27: Kinesiology

Types of Muscle Contractions

• Isometric– Tension is developed– No movement of the joint

• Isotonic– Constant resistance– Variable speed

• Isokinetic– Constant speed of contraction– Variable resistance

Page 28: Kinesiology

Speed vs. Force Movements

• Speed movements– Joints move in sequence– Walking, running

• Force movements– Joints move simultaneously– Squat, bench press

Page 29: Kinesiology

Linear vs. Angular Velocity

r

qA

A

B

B

Page 30: Kinesiology
Page 31: Kinesiology

If you think you're No. 1, you're never going to reach potential. So each day, we

battle. And each day, it changes.

Lelan Rogers – Syracuse University Lacrosse

Assistant Coach

Page 32: Kinesiology

Mechanical Principles

• Mass• Weight• Inertia• Speed • Velocity• Acceleration

Page 33: Kinesiology
Page 34: Kinesiology

Linear Acceleration (in velocity direction)

• This is the familiar stoplight acceleration along a straight line

• Zero to Sixty-Seven (30 m/s) in 5 seconds:– 30 m/s in 5 seconds means 6 m/s2 (~0.6g)

• Typical car acceleration, normal driving ~0.2g

Page 35: Kinesiology

Curves & Centripetal Forces• Going around a curve smushes you against

window– Understand this as inertia: you want to go

straight your body wants tokeep going straight

but the car is acceleratingtowards the center of the curve

Page 36: Kinesiology

Centripetal Forces

• The car is accelerated toward the center of the curve by a centripetal (center seeking) force

Centripetal Forceon car velocity of car

(and the way you’d rather go)

Page 37: Kinesiology

Introduction• Projectile Motion: Motion through the air without a propulsion

Page 38: Kinesiology
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Part 1.Motion of Objects Projected Horizontally

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v0

x

y

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x

y

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x

y

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x

y

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x

y

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x

y

•Motion is accelerated•Acceleration is constant, and downward• a = g = -10 m/s2 •The horizontal (x) component of velocity is constant•The horizontal and vertical motions are independent of each other, but they have a common timeg = -10 m/s2

Page 46: Kinesiology

Trajectory

x = v0 ty = h + ½ g t2

Eliminate time, t

t = x/v0

y = h + ½ g (x/v0)2

y = h + ½ (g/v02) x2

y = ½ (g/v02) x2 + h

y

x

h

Parabola, open down

v01v02 > v01

Page 47: Kinesiology

Changes in Vx

y

x

h

Page 48: Kinesiology

Part 2.Motion of objects projected at an angle

Page 49: Kinesiology

x

y

• Motion is accelerated• Acceleration is constant, and

downward• a = g = -9.81m/s2 • The horizontal (x) component of

velocity is constant• The horizontal and vertical

motions are independent of each other, but they have a common time

a = g =

- 9.81m/s2

Page 50: Kinesiology

Trajectory and Horizontal Range

0

5

10

15

20

25

30

35

0 20 40 60 80

15 deg

30 deg

45 deg

60 deg

75 deg

vi = 25 m/s

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Velocity

•Final speed = initial speed (conservation of energy)•Impact angle = - launch angle (symmetry of parabola)

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PROJECTILE MOTION - SUMMARY• Projectile motion is motion with a constant

horizontal velocity combined with a constant vertical acceleration

• The projectile moves along a parabola

Page 53: Kinesiology

• When a weight is held in a static position or when it is

moved at a constant velocity, it exerts constant

resistance, only in the downward direction.

Equilibrium

• However, upward or lateral acceleration of the weight

requires additional force.

Overcoming the effect of gravity

Page 54: Kinesiology

Stability• Center of gravity• Line of gravity• Base of support

Page 55: Kinesiology

Center of Gravity

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Anatomical Planes of the Human Body

Page 62: Kinesiology

Muscle Fiber Arrangements

Page 63: Kinesiology

Resistance training is quite safe compared with

other sports and fitness activities. Prudence can keep

injuries to a minimum. Basic safety principles include

good lifting form, appropriate resistance,

accommodation to injuries, balance, and variety.

Page 64: Kinesiology

Specificity is a major consideration when designing

an exercise program to improve performance in a

particular sport activity. The sport movement must be

analyzed qualitatively or quantitatively to determine the

specific joint movements that contribute to the whole-

body movement. Exercises that use similar joint

movements are then emphasized in the resistance

training program.

Page 65: Kinesiology
Page 66: Kinesiology

Stability

• Base of support (bos)• Center of gravity

(cog)/center of mass • Line of gravity (log)

Page 67: Kinesiology

Equilibrium and Movement

• Body segments moved independently– Mass is redistributed– Changes body’s cog

• As long as the cog is located over the bos the body will remain in equilibrium

Page 68: Kinesiology

Stability• Resistance to movement

– mass– log– bos– Move weight in the direction of the oncoming force

Page 69: Kinesiology

Dynamic Balance

• Constant interaction of forces–Move body in a given direction at a

given speed–Smooth transition of cog from one bos

to the next

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Dynamic Balance

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Force

• F = m(a)• Any influence that can change the state of

motion of an object• The objective of movement must be

considered

Page 72: Kinesiology

Magnitude of Force• Inertia of object and other resisting forces must be

overcome by enough force for movement to occur• Force must have adequate magnitude to overcome

inertia• Liner movement the closer the force is applied to

the cog the less force needed• Rotational movement the farther the force is

applied to the cog the less force is needed• Objects with a fixed point unless the force is

applied through the point of fixation, the object will rotate

Page 73: Kinesiology

MOM and DADMOM• Maximize• Optimize• Minimize

Page 74: Kinesiology

Muscle Pulling Force Manifested As a Pushing Force

Page 75: Kinesiology

Muscle Pulling Force Manifested As a Pulling Force

Page 76: Kinesiology

Angular motion

• Object rotates around an axis• Types

– Turn– Spin – Swing

Page 77: Kinesiology

Athlete’s body

• Predominantly rotational

1. Muscles pull on bones2. Bones rotate at joints

Page 78: Kinesiology

Levers• Simple machines that transmit mechanical

energy• Components of a lever

– Rigid object that rotates around an axis– Applied force– Resistance (opposes force)

• Produce torque – Turning effect– Increased by magnifying force and/or distance

from axis of rotation

Page 79: Kinesiology

2 functions of a lever system

1. Magnify speed and distance2. Magnify force

Can not occur at the same time

Page 80: Kinesiology

Short Lever Arm

Page 81: Kinesiology

Long Lever Arm

Page 82: Kinesiology

Optimize

Page 83: Kinesiology

a. First Class. In a first class lever, the weight to be moved is at one end of the lever, the applied force is at the other end, and the fulcrum (the pivot or turning point) is between the two.

b. Second Class. In a second class lever, the weight to be moved is between the applied force and the fulcrum. This type of lever enables a weight to be moved with less force than would be required without a lever. (Many feel that there are no second class levers in the human body.)

c. Third Class. In a third class lever, the weight to be moved is at one end of the lever, the fulcrum is at the other end, and the applied force is between the weight and the fulcrum. This type of lever provides speed, but a greater amount of force is required for a given weight. This is the most common type of lever in the human body.

Page 84: Kinesiology

First Class LeverThe Forearm

Magnify either force or speed and distance

Page 85: Kinesiology

Second Class LeverThe Foot

Magnify force at the expense of speed and distance

Page 86: Kinesiology

Third Class LeverThe Forearm

Magnify speed and distance at the expense of force.

Predominate the body – most muscles apply great force in order to move light resistances over large distances at great speed.

Page 87: Kinesiology

Human Body LeversMost are long• Distal ends capable of moving rapidly

Body movements• Swift, wide movements• Low force • Tasks involving rapid movement with light objects are easily

performed• Very forceful movements may require an anchoring to secure

a mechanical advantage

Page 88: Kinesiology

Bats, sticks, clubs and racquets

• Increase lever arm length• May increase force applied• Demands more force generated by muscles

Page 89: Kinesiology

Movement of the Body

• Outcome of a system of levers that operate together

• Speed– levers function is sequence– Swinging a bat

• Great force– levers function simultaneously– Squat or bench press

Page 90: Kinesiology

Speed

Page 91: Kinesiology

Force

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Inertia

A body in motion will stay in motion a body at rest will stay at rest unless acted on by an outside force

Outside forces include• Gravity• Air resistance• Tuff guys

Page 93: Kinesiology

Acceleration

• Movement response• Depends on

– External force applied– Resistance to movement (inertia)

Page 94: Kinesiology

Formulas• Distance (d)

D=Vt• Force (F)

F=ma• Work (W)

W=Fd or W=mad• Power (P)

P=W/t or P=mad/t or P=FV

Abbreviations• Distance (d)• Velocity (V)• Force (F)• Mass (m)• Acceleration (a)• Time (t)

Page 95: Kinesiology

Linear Acceleration

• Change in velocity• As V and t, a• Only experienced when force is applied

– When force stops, a new speed is achieved• The direction of acceleration is in the same

direction as the force applied• Acceleration is proportional to force applied

Page 96: Kinesiology

Angular Acceleration

• Rate of change of angular speed or direction• Large change in angular velocity + small amount

of time = large angular acceleration• A lever arm only experiences angular

acceleration when an external torque is applied– Torque stops angular acceleration stops

• Angular acceleration is in the direction of the torque and is proportional to the amount of torque

Page 97: Kinesiology

Constant Velocity• Zero acceleration• Equal and opposing forces are encountered• Forces cancel out no acceleration or

deceleration

Acceleration Caused by Gravity• 9.8m/s2

• A falling object accelerates at the rate of 9.8m/s each second it falls

Page 98: Kinesiology

Acceleration Due to Gravity

Page 99: Kinesiology

Radial Acceleration

• Direction change caused by centripetal force• Mass of object + curve radius + speed +

centripetal force• Aimed along the circular path at any instant• The force responsible for change of direction

– mass, centripetal force needed• Instantaneous direction change as turn

radius

Page 100: Kinesiology

Hammer Throw

Page 101: Kinesiology

Action/Reaction

Every action has an equal and opposite reaction

Page 102: Kinesiology

Linear Motion

mass, resistance to change

Page 103: Kinesiology

Movement of the Human Body

Caused by a body segment exerting force when in contact with a surface

• The reaction of the surface moves the body– sand vs. concrete

• Runner – propelled forward with an equal and opposite force pushed backward against the ground– Surface has sufficient friction (resistance to slipping)

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Torque and Action/Reaction

• Every torque exerted had an equal an opposite torque

• Change in angular momentum must be caused by a force that is equal and opposite

Page 106: Kinesiology

When Action/Reaction is not desired• Controlled• Undesired action must be absorbed

– Energy can not be created or destroyed– Purpose of pads

Page 107: Kinesiology

Performing Actions in a Standing Position

• Counter pressure of the ground

• accuracy of movement• Base of support

Page 108: Kinesiology

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