biomechanics lab, univ. of ottawa1 measurement of internal work by absolute work method d. gordon e....

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Biomechanics Lab, Univ. of Ottawa 1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School of Human Kinetics, University of Ottawa, Ottawa, CANADA

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Page 1: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 1

Measurement of Internal Workby Absolute Work Method

D. Gordon E. Robertson, PhD, FSCB

Biomechanics Laboratory,

School of Human Kinetics,

University of Ottawa, Ottawa, CANADA

Page 2: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 2

Mechanical Energy

Four forms– Gravitational potential (Egp)m g y

– Elastic potential (Eep) ½ k s2

– Translational kinetic (Etk) ½ m v2

– Rotational kinetic (Erk) ½ I 2

• Total mechanical energy is sum of all four

• Elastic potential energy is usually omitted because it cannot be measured accurately

Page 3: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 3

Total Body Mechanical Energy

• Sum of all segmental total mechanical energies (Es)

• Segmental total energy

Es = ms g ys + ½ ms vs2 + ½ Is s

2

• Total body energy (Etotal, sum over all segments)

Etotal = Es

Page 4: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 4

External Work

• External work = change () in total body mechanical energy

Wexternal = Etotal)• or simplified

Wexternal = Etotal (tfinal) – Etotal (tinitial)

Page 5: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 5

Zero-work Paradox

• If a body moves at constant velocity along a horizontal path no “external” mechanical work is done (work = 0)!

• Mechanical cost of moving body parts cancel out if motion is cyclic.

• Problem exists with all locomotor tasks but if body speeds up or rises (e.g., treadmill), some external work is done BUT additional costs of “cycling” the body parts are not included.

Page 6: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 6

Work Allowing No Transforms or Transfers of Energy

Work done that prevents both transfers and transforms of energy, i.e., from potential to kinetic and from segment to segment.

Wn = |ms g ys | + | ½ ms vs2 | +

| ½ Is s2|

• First summation is over all time intervals• Second summation is over all segments• Norman et al. (1976)

Page 7: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 7

Work Allowing within Segment Transforms

Work done that permits changes of forms of energy within a segment (kinetic to potential and vice versa) but no transfers from segment to segment.

Ww = |Es |• First summation is over all time intervals

• Second summation is over all segments

• Winter (1979)

Page 8: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 8

Energy Conservation by Transforming Energy within a Segment

• simple pendulum

pendulum

potential energy

potential energy

total energytotal

energy

kinetic energykinetic energy

Page 9: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 9

Internal Work

Internal work measures the mechanical costs of moving the limbs during a cyclic motion. The equation permits transfers of energy from segment to segment and transforms from one form (Egp, Etk) to another.

Winternal = |Etotal | − Wexternal

• Absolute values prevent decreases in mechanical energy from cancelling increases

Page 10: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 10

Energy Conservation by Transferring Energy between Segments

• compound pendulum

proximal segment proximal segment

total energytotal

energy

distal segment

distal segment

Page 11: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 11

Energy Saved by Transfers and Transforms

• Energy saved by permitting transfers of energy from segment to segment

Etransfers = Ww − Winternal

• Energy saved by permitting transforms of energy from one form to another (potential ot kinetic)

Etransforms = Wn − Ww

Page 12: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 12

Segment Energies during Walking

no conservation

in the leg (shank)

no conservation

in the leg (shank)

some conservation in the thigh

some conservation in the thigh

some conservation in the trunk

some conservation in the trunk

some transfer between left

and right sides

some transfer between left

and right sides

Page 13: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Biomechanics Lab, Univ. of Ottawa 13

Equation Summary

Etotal = ms g ys + ½ ms vs2 + ½ Is s

2

Wn = |ms g ys | + | ½ ms vs2 | + | ½ Is s

2|

Ww = |Es |

Wtotal = |Es | = Wwb

Wexternal = Etotal = Efinal − Einitial

Winternal = Wtotal − Wexternal

Page 14: Biomechanics Lab, Univ. of Ottawa1 Measurement of Internal Work by Absolute Work Method D. Gordon E. Robertson, PhD, FSCB Biomechanics Laboratory, School

Problems & Errors

• assumes a loss of energy in one part of the body can be cancelled by a gain in another part

• therefore underestimates internal work

• some researchers (Williams & Cavanagh, 1983) have tried to remove this limitation by blocking such compensations but this also prevents energy being transferred from joint to joint (e.g., plantiflexing while standing upright does transfer energy from the ankle to the head and all parts in between).

Biomechanics Lab, Univ. of Ottawa 14