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Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889.

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Page 1: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

DescribingMotion

DescribingMotion

PART I The Force-Motion Relationship

Photo reprinted from Marey, 1889.

Page 2: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

X velocity-Time

-0.300

-0.200

-0.100

0.000

0.100

0.200

0.300

0.400

0.500

0.600

-0.100 0.000 0.100 0.200 0.300 0.400 0.500

Page 3: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Movement is Motion – Motion is Movement

Page 4: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Laboratory Movement

Page 5: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Small Movement

Page 6: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Review of Math Review

Systeme Internationale = Metric System

Fundamental Units: mass in kg, linear distance in m, angular distance in rad, time in s

All other physical measurements are derived from these variables:

Force = N = kg*m / s2 Energy = J = kg*m2 / s2

Website for conversions http://catcode.com/trig/trig08.html

Page 7: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

More review of Math Review

Radian – the angle created by the arc on a circle with the length of the radius of the circle (~ 57.3 degrees)

Arc length = 1 radius

Page 8: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Math Review

Trigonometry – sine, cosine, tangent, and inverse functions

sin a = A/C, cos a= B/C, tan a= A/B

sin-1 A/C = a, cos-1 B/C = a,

tan-1 A/B = aA

a

B

C

Page 9: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Math Application: important in signal processing

Sine function – continuous wave over angular position

+1

0

-10 180 360 degrees

Page 10: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Cosine function – continuous wave over angular position

+1

0

-1

Math Application: important in signal processing

Page 11: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Math Review

Website for sine and cosine waves

http://catcode.com/trig/trig08.html

Page 12: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Describing Motion = Kinematics

Kinematics describes the

Time – Geometry of Motion

or the

Movement Pattern

during static or dynamic activity

Page 13: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Two Fundamental Movement Patterns

Translation – Linear Movement – displacement from one point to another in either:

Straight lines – rectilinear translation or

Curved lines – curvilinear translation

Animals can do both but curvilinear motion more common

Page 14: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Curvilinear Translation During Walking

Page 15: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Two Fundamental Movement Patterns

Rotation – Angular Movement – displacement around an axis

Principle means of

animal motion

Page 16: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Translation Through Rotation

A person stands up by rotating the hip, knee, and ankle joints

Animals rotate to translate

Animals are rotating machines

Animals translate by skillfully combining joint rotations

Page 17: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Translation Related to Rotation

Linear displacement and velocity related to the angular kinematics:

s = r

v = r

Calculate Arc Length when radius = 1 cm and = 90°

Page 18: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Four Kinematic Variables or Motion Descriptors

Position – location within the environment

Displacement – the change in position with movement

Velocity – rate of change of position

Acceleration – rate of change of velocity

(All variables are vectors)

Page 19: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Biomechanics Laboratories

Page 20: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Position in a Linear 2D Reference Frame

Heel Strike: Shoulder=1.01,1.34

Knee = 1.11, 0.47

Toe Off: Shoulder=1.87,1.35

Knee = 1.78, 0.44

Page 21: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Position in an Angular Reference Frame

Segment Angles – Angle between a body segment and the right horizontal from distal end of segment

Trunk = 85° or 1.48 rad

Arm = 95° or 1.66 rad

Page 22: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Position in an Angular Reference Frame

Joint Angles – Angle between two body segments

Shoulder = 20° or 0.35 rad

Knee = ???

Page 23: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Generate Angular Position Data

1) Identify location of skeletal joints

2) Define joint angles

3) Calculate segment angles

4) Combine segment angles to calculate joint angles

Page 24: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Position in an Angular Reference Frame

          

  Acromion

1.10, 1.34

Greater Trochanter

1.05, 0.8

Lateral Knee

1.18, 0.5

Lateral Malleolus

1.23, 0.1

Heel

1.20, 0.02

5th Met

1.35, 0.08

Page 25: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Position in an Angular Reference Frame

Joint angular position for obese and lean subjects while walking

Obese less flexed at hip and knee and less dorsiflexed at ankle

Obese walk in a more erect pattern

Page 26: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Displacement

Displacement = difference between final and initial positions

Linear displacement (d) = Pf – Pi (m)

Angular displacement () = f - i ( or rad)

Displacement does not necessarily equal distance (the length of the path traveled)

Page 27: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Displacement in a Linear Reference Frame

Horizontal displacement:

heel strike to toe off

Shoulder = 0.86 m

Met Head = 0.09 m

Total displ. Shoulder =

1.87,1.35

-1.01,1.34

0.86,0.01

Page 28: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Displacement in a Linear Reference Frame

Resultant displacement between heel strike and toe off for:

Shoulder = 0.87 m

Met head = 0.10 m

Magnitude Result. Displ. = (Hor disp2 + Vert disp2)1/2

Page 29: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Linear Displacement During Walking

Step length – forward displacement of one foot during swing phase

Stride length – combined forward displacement of both feet during left and right swing phases

Page 30: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Linear Displacement During Walking

Step length – mean value ~ 0.75 m for healthy adults, less for shorter, older, ill, or injured people

Left and right step length symmetry

Stride length – mean value ~1.5 m for healthy adults, less for shorter, older, ill, or injured people

Page 31: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Velocity

Velocity = rate of change of position

= amount of displacement per unit time

“rate of change” = calculus concept of the derivative or slope

Linear velocity (v) = (Pf – Pi) / time (m/s)

Angular velocity () = (f - i) / time (/s or rad/s)

Page 32: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Johnson vs Lewis100m, Seoul 1988

More information with shorter measurement intervalsNewsweek, 7-29-96

Gross body movement

Page 33: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Average vs. Instantaneous Velocity

Page 34: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Velocity

Velocity = rate of change of position

= amount of displacement per unit time

“rate of change” = calculus concept of the derivative or slope

Linear velocity (v) = (Pf – Pi) / time (m/s)

Angular velocity () = (f - i) / time (/s or rad/s)

Simple Finite Difference TechniqueSimple Finite Difference Technique

Page 35: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Velocity: displacement / timeVelocity: displacement / time

vectorvector•magnitude: how fastmagnitude: how fast•direction: specification of “which way”direction: specification of “which way”

•This is motionThis is motion

Page 36: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Cyclic Movement – Angular Kinematics

Positive & negative slopes on position curve have positive and negative phases on the velocity curve

0.00

2.00

An

gu

lar

Po

sitio

n

Time

Page 37: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Cyclic Movement – Angular Kinematics

Positive & negative slopes on position curve have positive and negative phases on the velocity curve

0.00

2.00

An

gu

lar

Po

sitio

n

Time

Increasing +

Page 38: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Cyclic Movement – Angular Kinematics

Positive & negative slopes on position curve have positive and negative phases on the velocity curve

0.00

2.00

An

gu

lar

Po

sitio

n

Time

Increasing +

Decreasing +

Page 39: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Cyclic Movement – Angular Kinematics

Positive & negative slopes on position curve have positive and negative phases on the velocity curve

0.00

2.00

An

gu

lar

Po

sitio

n

Time

Increasing +

Decreasing +

Increasing -

Page 40: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Cyclic Movement – Angular Kinematics

Positive & negative slopes on position curve have positive and negative phases on the velocity curve

0.00

2.00

An

gu

lar

Po

sitio

n

Time

Increasing +

Decreasing +

Increasing -

Decreasing -

Page 41: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Cyclic Movement – Angular Kinematics

Positive & negative slopes on position curve have positive and negative phases on the velocity curve

0.00

2.00

An

gu

lar

Po

sitio

n

Time

-2.00

0.00

2.00

Angula

r V

elo

city

Time

Page 42: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Relationship Between Position and Velocity

Knee angular position & velocity curves during the stance phase of running

Page 43: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Knee Position/Velocity in Walking

Knee Angular Position

-70.0

-60.0

-50.0

-40.0

-30.0

-20.0

-10.0

0.0

10.0

0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80

Time (s)

Po

sit

ion

(d

eg

rees)

Fle

xio

n i

s N

eg

ati

ve

Knee Position

contact Toe off

Page 44: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Knee Position/Velocity in Walking

Knee Angular Position and Velocity

-70.0

-60.0

-50.0

-40.0

-30.0

-20.0

-10.0

0.0

10.0

0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80

Time (s)

Po

sit

ion

(d

eg

rees)

Fle

xio

n i

s N

eg

ati

ve

Knee Position

Identify local minima and maxima: velocity = ??

Page 45: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Knee Position/Velocity in Walking

Knee Angular Position and Velocity

-70.0

-60.0

-50.0

-40.0

-30.0

-20.0

-10.0

0.0

10.0

0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80

Time (s)

Po

sit

ion

(d

eg

rees)

Fle

xio

n i

s N

eg

ati

ve

Knee Position

What is the sign of the velocity between local min & max?

Page 46: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Knee Position/Velocity in Walking

Knee Angular Position and Velocity

-70.0

-60.0

-50.0

-40.0

-30.0

-20.0

-10.0

0.0

10.0

0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80

Time (s)

Po

sit

ion

(d

eg

rees)

Fle

xio

n i

s N

eg

ati

ve

Knee Position

Identify inflection points : ?

Page 47: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Knee Position/Velocity in Walking

Knee Angular Position and Velocity

-70.0

-60.0

-50.0

-40.0

-30.0

-20.0

-10.0

0.0

10.0

0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80

Time (s)

Po

sit

ion

(d

eg

rees)

Fle

xio

n i

s N

eg

ati

ve

Knee Position

Identify inflection : local minima & maxima on velocity

Page 48: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Knee Position/Velocity in Walking

Knee Angular Position and Velocity

-70.0

-60.0

-50.0

-40.0

-30.0

-20.0

-10.0

0.0

10.0

0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80

Time (s)

Po

sit

ion

(d

eg

rees)

Fle

xio

n i

s N

eg

ati

ve

-400

-300

-200

-100

0

100

200

300

400

500

600

Velo

cit

y (

deg

rees/s

)

Knee Position

Knee Velocity

Identify local minima and maxima

Page 49: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Knee Position/Velocity in Walking

Knee Angular Position and Velocity

-70.0

-60.0

-50.0

-40.0

-30.0

-20.0

-10.0

0.0

10.0

0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80

Time (s)

Po

sit

ion

(d

eg

rees)

Fle

xio

n i

s N

eg

ati

ve

-400

-300

-200

-100

0

100

200

300

400

500

600

Velo

cit

y (

deg

rees/s

)

Knee Position

Knee Velocity

Identify inflection points

Page 50: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Second Order Finite Differences

• Use Project to demonstrate need.

Page 51: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Acceleration

Acceleration = rate of change of velocity

= change in velocity per unit time

change in velocity = change in motionchange in velocity = change in motion

Page 52: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Acceleration

Acceleration = rate of change of velocity

= change in velocity per unit time

“rate of change” = calculus concept of the derivative or slope

Linear acceleration (a) = (Vf – Vi) / time (m/s2)

Angular acceleration () = (f - i) / time

(/s2 or rad/s2)

Page 53: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Acceleration

Acceleration due to gravity = g = 9.81 m /s2

-140-120-100-80-60-40-20

00 1 2 3 4 5

Time (s)

Po

s (m

) o

r V

el (

m/s

)

Position

Velocity

Describe shape of:Position curveVelocity curveAcceleration?

Page 54: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Acceleration

Acceleration due to gravity = g = 9.81 m /s2

-140-120-100-80-60-40-20

00 1 2 3 4 5

Time (s)

Po

s (m

) o

r V

el (

m/s

)

Position

Velocity

Describe shape of:Position curveVelocity curveAcceleration

Page 55: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Velocity – Acceleration Relation

Based on definition of acceleration, sketch the angular acceleration curve for this velocity curve

-2.00

0.00

2.00

Angula

r V

elo

city

Time

Page 56: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Velocity – Acceleration Relation

Acceleration curve shows the slope of the velocity curve, including positive and negative directions

-2.00

0.00

2.00

Angula

r V

elo

city

Time

-2.00

0.00

2.00

An

gu

lar

Acc

ele

ratio

n

Time

Page 57: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Acceleration is our link to kinetics

• Important to understand the concept of positive and negative acceleration

Page 58: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Acceleration is our link to kinetics

• Important to understand the concept of positive and negative acceleration

• Parabolic motion: horizontal & vertical components

• release velocity• Peak velocity• contact velocity

Page 59: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Wayne WrightHuman Cannonball

Page 60: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Acceleration is our link to kinetics

• Important to understand the concept of positive and negative acceleration

• Parabolic motion: horizontal & vertical components

• release velocity• Peak velocity• contact velocity

Gymnast leaves ground at v v = 3m/s and v h = 4.2 m/s. Calculate velocities 0.25 seconds later.

Gymnast is at peak height (v v = 0 m/s). How fast is she traveling 0.25 m (vertical) later? What is vh?

Gymnast is falling at –1.5 m/s. How fast is she traveling 0.25s later? What about v h?

Page 61: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Constant Linear Velocity

• Acceleration = 0• what is force?

• Calculating final position of body

• Rearrange equation of velocity• Sprinter is 70 from start. Horizontal velocity of

11.5 m/s. Maintains for 1.7s. How far from start line?

Page 62: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

So let’s imagine the force. 09/02/07: Labor Day occasion to commemorate lost railroad workers By Bill Kemp Archivist/Librarian, McLean County Museum of History Advertisement  BLOOMINGTON -- On Feb. 25, 1921, "death came fantastic with horror" when a storage tank explosion tossed Harold Downey’s whirling, lifeless body 200 feet into the air. A Chicago & Alton Railroad boilermaker, Downey’s fatal accident reminds us of the untold number of railroad workers who lost their lives toiling in one of the more vital and dangerous industries in U.S. history. On that Friday afternoon, Downey, who worked at the C&A shops on Bloomington’s west side, was sent to repair a leaking gasoline storage tank. When he entered through a manhole at the top, his lighted torch ignited the escaping fumes."His body was propelled upwards with a force, the intensity of which can only be imagined," the Pantagraph reported.

Page 63: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Forensic Biomechanics

Complete the project available from the website.

Page 64: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

General Kinematic Procedures

Linear data:

use position of body segments for descriptive stride characteristics (how far, high, etc)

use position, velocity, and acceleration for complex inverse dynamics (F = ma)

Angular data:

use joint angular position for direct comparisons

use joint angular velocity for joint power (P= T * )

Page 65: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

General Kinematic Procedures

Other places: You name it, people use it.

Pelvic tilt

Hand displacement in reaching

Trunk vibrations in driving

Tibia accelerations in running (shock)

etc etc etc

Page 66: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889
Page 67: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Orthotic Effects on Kinematics

Page 68: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Kinematic Coordination in Running

Coordination between knee and subtalar motions

Page 69: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Kinematic Coordination in Running

Page 70: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

AnklePosition: Soft vsStiffLandings

Page 71: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Use angular velocity to compare technique

Page 72: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Use angular velocity to compare technique

Page 73: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Use angular velocity to compare technique

Page 74: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Relation Between Kinematics & Kinetics

Kinetics causes kinematics

Force produces acceleration which ultimately causes a change in position

Kinematics causes kinetics ?

Position causes force??

Is this possible???

Page 75: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

482 Advanced Biomechanics

• How many plan to enroll in this class for Spring 2008?

• Early registration is next week, do it at that time.

• Warning: if low enrollment, class will be cancelled, so sign up for an alternative class too.

Page 76: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Error in Kinematic Data

Calculations of derivatives introduces noise into the signal

Velocity has some error

Acceleration has more error

Page 77: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Error From Data Acquisition

Digitizing process introduces error in position data –

Markers move or vibrate relative to the joint center

System misses the marker

Markers are covered

Page 78: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Time vs Frequency

Human movement – low frequency

Digitizing error – high frequency

Derivatives increase high frequency error

Pos = sin 2 Vel = 2 cos 2

Page 79: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Fourier Analysis – Frequency Content

Single frequency

Two frequencies

Many frequencies

Page 80: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Digital Filters to Remove Error

Low pass filter allows low frequency signal to pass but filters out high frequency error

Cut off frequency ~ 5-15 Hz

Optimal filter techniques

Fourier Analysis

Page 81: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Optimal Filter

Finds point beyond which filtering does not change result

Page 82: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Digital Filter Demonstration

(Show digital filter program application)

Bench Press: filter the angular velocity and acceleration curves

Page 83: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889
Page 84: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889
Page 85: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889
Page 86: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889
Page 87: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889
Page 88: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

80% 1RM BP, Narrow vs Wide Grip

Page 89: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Filtered Position – Good Acceleration

Filter position data to produce accurate velocity and acceleration data

We filter the linear horizontal & vertical position vs time data

Page 90: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Signal Processing

Data Filtering or smoothing vs. Curve fitting

y = 106.02x - 108.53

R2 = 0.9502

40

50

60

70

80

90

1.50 1.60 1.70 1.80 1.90

Height

Ma

ss

Force by Contraction Velocity

y = 991.57x2 - 545.25x + 101.45

R2 = 0.9871

020406080

100120

0 0.1 0.2 0.3 0.4

Velocity (mm/s)

Fo

rce

(N)

Page 91: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Signal Processing

Complex and detailed mathematical topic

We provided only the slightest introduction

Page 92: Describing Motion Describing Motion PART I The Force-Motion Relationship Photo reprinted from Marey, 1889

Summary – Kinematics

Kinematics describes the movement pattern in linear and angular reference frames

Kinematics is the outcome of Kinetics (the result not the cause)