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Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa, Ottawa, CANADA
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Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Dec 14, 2015

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Page 1: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Biomechanics of Walking and Stair Ascent and Descent

D. Gordon E. Robertson, Ph.D.

Biomechanics, Laboratory,

School of Human Kinetics,

University of Ottawa, Ottawa, CANADA

Page 2: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Quantitative Domains

• Temporal–Phases (stance/swing) and events

(foot-strike, toe-off), stride rate

• Kinematic (motion description)– stride length, velocity, ranges of

motion, acceleration

• Kinetic (causes of motion)– ground reaction forces, joint forces,

moments of force, work, energy and power

Page 3: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Temporal Analysis

• Stride time

• Stride rate = 1/rate

• Stride cadence = 120 x rate (b/min)

• Instrumentation–Photocells and timers

–Videography (1 frame = 1/30 second)

–Metronome

Page 4: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Motion Analysis Tools

EMG

Force platform

Cine or Video camera

Page 5: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Electromyography

Delsys system

Mega system

Noraxon system Bortec system

Page 6: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Kinematic Analysis

• Study of motion without consideration of its causes

• Motion description

• Based on Calculus developed by Newton and Leibnitz

Isaac Newton, 1642-1727

Page 7: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Kinematic Analysis

• Linear position– Ruler, tape measure, optical

• Angular position– Protractor, inclinometer,

goniometer

• Linear acceleration– Accelerometry, videography

• Angular acceleration– Videography

Miniature accelerometers

Manual goniometer

Page 8: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Motion Analysis

• Cinefilm, video or infrared video

• Subject is filmed and locations of joint centres are digitized

High-speed cinecamera

Videocamera

Infrared camera

Page 9: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Computerized Digitizing (APAS)

Page 10: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Computerized Digitizing (Simi)

Page 11: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Stick Figure Animation

Walking

Page 12: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Kinetic Analysis

Causes of motion

• Forces and moments of force

• Work, energy and power

• Impulse and momentum

• Inverse Dynamics derives forces and moments from kinematics and body segment parameters (mass, centre of gravity, and moment of inertia)

Page 13: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Force Platforms

2 Kistler force platforms

Ground reaction force

Page 14: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Steps for Inverse Dynamics

• Space diagram of the lower extremity

Page 15: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Divide Body into Segments and Make Free-Body Diagrams

• Make free-body diagrams of each segment

Page 16: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Add all Known Forces to FBD

• Weight (W)

• Ground reaction force (Fg)

Page 17: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Apply Newton’s Laws of Motion to Terminal Segment

• Start analysis with terminal segment(s), e.g., foot or hand

Page 18: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Apply Reactions of Terminal Segment to Distal End of Next Segment in Kinematic Chain

• Continue to next link in the kinematic chain, e.g., leg or forearm

Page 19: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Repeat with Next segment in Chain or Begin with Another Limb

• Repeat until all segments have been considered, e.g., thigh or arm

Page 20: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Joint Power Analysis

0.0 0.1 0.2 0.3 0.4Time (s)

-4000.

-2000.

0.

2000.

-300.

0.

300.

-20.

0.

20.

Pow

er

(W)

Mom

en

t (N

.m)

A

ng

ula

r vel.

(/s

)

SR11BJ

ITO CFS CTO IFS

Extending

Flexing

Extensor

Flexor

Concentric

Eccentric

• compute the net moment of force at the joint

• multiply angular velocity and moment of force to obtain the “moment power”

• this is the power produced by the net moment of force acting across the joint

• it is mainly caused by muscle forces

• compute the angular velocity of the joint

Page 21: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Normal Walking Example

• Female subject

• Laboratory walkway

• Speed was 1.77 m/s

• IFS = ipsilateral foot-strike

• ITO = ipsilateral toe-off

• CFS = contralateral foot-strike

• CTO = contralateral toe-off

Page 22: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Ankle angular velocity, moment of force and power

• Dorsiflexors produce dorsiflexion during swing

• Plantar flexors control dorsiflexion

• Large burst of power by plantar flexors for push-off 0.0 0.2 0.4 0.6 0.8 1.0 1.2

Time (s)

-200

-100

0

100

-100

0

100

-10

0

10

P

ow

er

(W)

Mo

me

nt

(N.m

)

A

ng

. V

el.

(ra

d/s

)

Trial: 2SFN3Ang. velocityMomentPower

CFS ITO IFS CTO CFS ITO

Dorsiflexion

Plantar flexion

Dorsiflexors

Plantar flexors

Concentric

Eccentric

Page 23: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Knee angular velocity, moment of force and power

• Negative work by extensors to control flexion at push-off

• Burst of power to cushion landing

• Negative work by flexors to control extension prior to foot-strike

0.0 0.2 0.4 0.6 0.8 1.0 1.2Time (s)

-200

-100

0

100

-100

0

100

-10

0

10

P

ow

er

(W)

M

om

en

t (N

.m)

A

ng

. V

el.

(ra

d/s

)

Trial: 2SFN3Ang. velocityMomentPower

CFS ITO IFS CTO CFS ITO

Extension

Flexion

Extensors

Flexors

Concentric

Eccentric

Page 24: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Hip angular velocity, moment of force and power

0.0 0.2 0.4 0.6 0.8 1.0 1.2Time (s)

-200

-100

0

100

-100

0

100

-10

0

10

P

ow

er

(W)

Mo

me

nt

(N.m

)

A

ng

. V

el.

(ra

d/s

)

Trial: 2SFN3Ang. velocityMomentPower

CFS ITO IFS CTO CFS ITO

Flexion

Extension

Flexors

Extensors

Concentric

Eccentric

• Positive work by flexors to swing leg

• Positive work by extensors to extend thigh

• Negative work by flexors to control extension

Page 25: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Solid-Ankle, Cushioned Heel (SACH) Prostheses

Page 26: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Stick Figure Animation

Walking with SACH foot

Page 27: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4

Time (s)

-200.

-100.

0.

100.

-100.

0.

100.

-10.

0.

10.

Po

we

r (W

)

Mo

me

nt

(N.m

)

An

gu

lar

ve

l. (

/s)

Ankle angular velocity, moment of force and power of SACH foot prosthesis

• No power produced during push-off

Trial: WB24MH-SAng. velocityNet momentPower

ITO IFS CTO CFS ITO

Dorsiflexing

Plantar flexing

Dorsiflexor

Plantar flexor

Concentric

Eccentric

• Power dissipation during weight acceptance and push-off

Page 28: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

FlexFoot Prostheses(Energy Storing)

Recent models

Original model

Page 29: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Stick Figure Animation

Walking with FlexFoot prosthesis

Page 30: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Ankle angular velocity, moment of force and power of FlexFoot prosthesis

• Power returned during push-off

0.0 0.2 0.4 0.6 0.8 1.0 1.2

Time (s)

-500.

-250.

0.

250.

-100.

0.

100.

-10.

0.

10.

Po

we

r (W

)

M

om

en

t (N

.m)

A

ng

ula

r v

el.

(/s

)

Trial: WB13MH-FAng. velocityNet momentPower

ITO IFS CTO CFS ITO

Dorsiflexing

Plantar flexing

Dorsiflexor

Plantar flexor

Concentric

Eccentric

Page 31: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Ankle angular velocity, moment of force and power of person with hemiplegia (stroke side)

• No power during push-off

0.0 0.2 0.4 0.6 0.8

Time (s)

-2000.

-1000.

0.

1000.

-200.

0.

200.

-15.

0.

15.

Po

we

r (W

)

M

om

en

t (N

.m)

A

ng

ula

r ve

l. (

/s)

Trial: WPP14EGAng. vel.Net momentPower

IFS CTO CFS ITO IFS

Dorsiflexing

Plantar flexing

Dorsiflexor

Plantar flexor

Concentric

Eccentric

Page 32: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Ankle angular velocity, moment of force and power of person with hemiplegia (normal side)

• Power at push-off is reduced due to slower gait

0.0 0.2 0.4 0.6 0.8

Time (s)

-2000.

-1000.

0.

1000.

-200.

0.

200.

-15.

0.

15.

P

ow

er

(W)

Mo

me

nt

(N.m

)

An

gu

lar

ve

l. (

/s)

Trial: WPN03EGAng. vel.Net momentPower

IFS CTO CFS ITO IFS

Dorsiflexing

Plantar flexing

Dorsiflexor

Plantar flexor

Concentric

Eccentric

• Negative power is also reduced

Page 33: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Other Gait Patterns

Above-knee Prostheses

Page 34: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Stick Figure Animation

Walking with Terry Fox prosthesis

Page 35: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Support Moment

• Used to quantify stability during stance of gait

• Sum of ankle, knee and hip moments

• Extensors moments are made positive

Msupport = Mankle + Mknee + Mhip

• Should remain positive throughout stance despite loss of function at one or more joints

• Studies have shown that even people with artificial joints produce a positive support moment throughout stance

(Winter, J. Biomech, 13, 923-927, 1980)

Page 36: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Support Moment during Walking

• Support moment is positive throughout stance

• Typically has two peaks one after IFS and one before ITO

0.0 0.2 0.4 0.6 0.8 1.0 1.2Time (seconds)

-200.

-100.

0.

100.

-100.

0.

100.

-100.

0.

100.

-100.

0.

100.

200.

Net

mo

men

ts o

f fo

rce

(N.m

)

Trial: CJWK

IFS CTO CFS ITO

Support moment

Hip extensor

Knee extensor

Ankle extensor• Ankle plantar

flexors are the most important from midstance to toe-off

Page 37: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Laboratory Stairs

• Step height = 24 cm

• Step tread = 30 cm

• Railings = 36 in.

• Height and tread are adjustable

Force platformsForce platforms

Page 38: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Stick Figure Animation

Up One Step from Landing

Page 39: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Up One Step from Landing

• Smaller ankle plantar flexor moment

• Larger than normal knee extensor moment

0.7 0.9 1.1 1.3 1.5 1.7 1.9 2.1 2.3Time (seconds)

-200.

-100.

0.

100.

-100.

0.

100.

-100.

0.

100.

-100.

0.

100.

200.

Net

mo

men

ts o

f fo

rce

(N.m

)

Trial: STLUP7RH

ITO IFS ITO

Support moment

Hip extensor

Knee extensor

Ankle extensor

• Support moment similar to walking

Page 40: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Similarities to Walking

• Double support periods

• Ground reaction forces have double peak

• Cadence similar

• Support moment is similar (always positive with two peaks)

Page 41: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Differences with Walking

• Peak forces slightly higher• Centre of pressure is concentrated under

metatarsals, rarely near heel• Several types of steps

– ascent versus descent– single step up and down– double step up and down– start from or end at a landing

• Step height and tread vary from stairway to stairway

• Railings may be present

Page 42: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Ascent versus Descent

• Descent is more dangerous because if tripping occurs person will fall farther

• Descent is more likely to cause fall since centre of pressure and centre of gravity is closer to edge of stair

Page 43: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Factors Influencing Stability

• Weight

• Size of base of support (hand rails)

• Friction

• Distance from tipping edge

• Height of centre of gravity

• Visual field

• Vestibular system

• Inebriation/drugs

Page 44: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Stick Figure Animation

Down Two Stairs to Landing

Page 45: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Down Two Stairs Forwards

• Larger than normal negative power by ankle plantar flexors after foot-strike (IFS)

0.7 0.9 1.1 1.3 1.5 1.7 1.9 2.1Time (seconds)

-500.

-250.

0.

250.

500.

-250.

0.

250.

-250.

0.

250.

500.

Po

wer

(w

atts

)

Trial: CJRFD

ITO IFS ITO

Hip powers

Knee powers

Ankle powers

• Positive work done after IFS by knee flexors

Page 46: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Possibly Safer Descent

• Descend backwards

• Centre of pressure and centre of gravity are farther from edge of stairs

• If tripping occurs person falls into stairs not down stairs

• Person will be “forced” to use railing

• Problem with seeing next step

• Some people may have problem with neck

Page 47: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Stick Figure Animation

Down Two Steps Backwards

Page 48: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Down Two Stairs Backwards

• No concentric knee power required after IFS

0.5 0.7 0.9 1.1 1.3 1.5 1.7 1.9 2.1Time (seconds)

-500.

-250.

0.

250.

500.

-250.

0.

250.

-250.

0.

250.

500.

Po

wer

(w

atts

)

Trial: CJLBD

ITO IFS ITO

Hip powers

Knee powers

Ankle powers

• Larger than normal negative power by ankle plantar flexors after foot-strike (IFS)

• No push-off power needed from ankle

Page 49: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

What’s Next

• Modify rise and tread• At-risk subjects

– Elderly– Infants– Disabled– Distracted– Prostheses– Robots

• Ramps versus stairs– Angle of ramp– Surface friction

• Cambered surfaces

Page 50: Biomechanics of Walking and Stair Ascent and Descent D. Gordon E. Robertson, Ph.D. Biomechanics, Laboratory, School of Human Kinetics, University of Ottawa,

Questions?

Answers?

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