an optimal design for a foot activated a thesis

76
AN OPTIMAL DESIGN FOR A FOOT ACTIVATED LEVER MECHANISM by JOHl^ ENSDORPF, B.S. A THESIS IN INDUSTRIAL ENGINEERING Submitted to the Graduate Faculty of Texas Technological College In Partial Pulfillraent of the Requirements for the Degree of MASTER OP SCIENCE IN INDUSTRIAL ENGINEERING Approved Accepted May, 1 9 ^

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Page 1: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

AN OPTIMAL DESIGN FOR A FOOT ACTIVATED

LEVER MECHANISM

by

JOHl ENSDORPF, B.S.

A THESIS

IN

INDUSTRIAL ENGINEERING

Submitted to the Graduate Faculty of Texas Technological College

In Partial Pulfillraent of the Requirements for

the Degree of

MASTER OP SCIENCE IN

INDUSTRIAL ENGINEERING

Approved

Accepted

May, 1 9 ^

Page 2: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

75

l\Eh^73H

ACKN0WLEDGr4ENTS

I am deeply indebted to Professor Morris Schneider

for his over-all guidance in this thesis work and to Dr«

Richard A. Dudek, Dr. Robert Keller White, and Mr. Richard

Carmon for their advice and helpful comments. In addi­

tion, I wish to express appreciation to the subjects

utilized in this research project for their willingness

and enthusiasm in cooperating with me throughout the study.

ii

Page 3: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

TABLE OP CONTENTS

Page

ACKNOWLEDGMENTS ii

LIST OP TABLES v

LIST OP ILLUSTRATIONS vi

Chapter

I. INTRODUCTION . 1

Purpose and Scope . . • • • 1

History • • . . . • • • • . • • 2

I I . EQUIPMENT 8

Description of Equipment . 8

Use of Equipment 12

III. DESIGN OP THE EXPERIMENT l4

Discussion of Variable Factors . . . . . . 14

Schedule of Subjects 20

Experimental Procedure . . . . . . . . . . 23

Recording Data 24

IV. ANALYSIS OP DATA AND CONCLUSIONS 25

Computer Processing • • . . . • 27

Analysis and Interpretation 27

Conclusions • • . • . . . . . . • 35

Recommendations for Further Study . . . . . 37

BIBLIOGRAPHY ^2

iii

Page 4: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

APPENDIX 63

A. Sketches of Important Components of the Experimental Device 64

B. Preliminary Study of Foot-Ratio Correlation 67

iv

Page 5: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

LI3T OF tkBlMS

T^f^^U Pag«

1« 3ett«ioii Se^di iU ri»r 3iiSiJ««t« with

ChNlttr 0t fll»i« A t t i t u d e t « * * « * * * « 21

2 , Ideatif leAtion Teiile » « » • » • • 26

3« 3«irea«l*ftetor AaftVA Antlirfie « « * • • • » • « 28

Page 6: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

LIST OP ILLUSTRATIONS

Figure Page

1. Barnes's Experimental Pedals . . 39

2. Lauru*s Experimental Pedals 40

3» Force-Load Relationships • . • • • 41

4. Pedal Assembly . • • . . . . • . . 42

5* Side View of Frame Assembly 43

6. Front of Frame Assembly 44

7* Pedal Linkage • • . • . 45

8. Electrical Equipment . . . . . . . 46

9. Electrical Schematic 47

10. Foot Dimension Ratio Study 48

11. Sample Data Sheet . 49

12. Fulcrum - Composite Score Main Effect . . . . 50

13. Resistance - Composite Score Main Effect . . 51

14. Ratio - Composite Score Main Effect . . . . . 52

15. Fulcrum - Resistance - Composite Score Interaction . • • . • • . . . 53

16. Resistance - Ratio - Composite Score

Interaction 54

17. Fulcrum - Type Score Main Effect . . . . . . 55

18. Resistance - Type Score Main Effect 56

19. Fulcrum - Resistance - Type Score Interaction • • . . 57

vi

Page 7: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

20. Ratio - Type Score Interaction 58

21. Resistance - Ratio - Type Score Interaction , , 59

22. Fulcrum - Resistance - Ratio Type Score Interaction 60

23. Optimal Pedal Arrangements . . . . . . . . . 61

vii

Page 8: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

CHAPTER I

INTRODUCTION

Purpose and Scope

Ralph M. Barnes (1) states that

although the foot pedal is one of the most common de­vices for freeing the hands for productive work^ most pedals are poorly designed.

Pedals might be classified as those requiring con­siderable effort for manipulation and those requiring little effort. The first class is well illustrated by the garment press and by certain foot-operated punch presses and shears. The second class is illus­trated by the trip on a power punch press or the con­trol on an electrical sewing machine.

This research study had as its purpose the investi­

gation of the leg and the foot and their functional per­

formance with a foot pedal under multivariant environmental

conditions.

For optimal design of a foot pedal mechanism a

number of factors must be considered which directly affect

output of energy and over-all performance. These factors

aret

!• Fulcrum position in relation to the foot.

2. Resistance or load imposed against pedal

movement.

3* Foot dimension.

/

Page 9: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

4. Relation of application points of force exerted

by foot and linkage point of attachment on pedal.

5. Angular attitude of operator's tibia to plane

of the floor.

These factors are considered independent to over-all

performance of a foot pedal mechanism. The dependent

output can be measured in terms of operator's reaction

time to some stimulus, time to accomplish a specific task,

and by a measure of accuracy. For this research these

factors were measured in terms of2

1. Reaction time.

2. Travel time.

3* Accuracy.

All of the variables were considered significant

areas for study in the attempt to determine significant

design characteristics of a foot pedal mechanism.

History

Research of available publications concerning design

of foot pedal mechanisms indicates that comparatively

little work has been done in the area.

In 1941, Ralph M. Barnes, Henry Hardaway and Odif

Podolsky (2) of the College of Engineering at the State

University of Iowa conducted an experiment involving five

different types of pedals. The object of their study was

Page 10: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

to determine the relative effectiveness of the five diffe3>-

ent pedals. Each pedal had a different arrangement of the

fulcrum, which brought into use different muscles of the

body and required different body movements. The five

pedal arrangements used are shown in Figure 1.

Each pedal was depressed against a tension spring

requiring twenty inch-pounds for one complete stroke. For

example, one of the pedals had the fulcrum point installed

under the heel, the ball of the foot moving through a

distance of two inches against a resistance of ten pounds.

Copper contacts connected in series to solenoid-

operated pencils on a kymograph were used to time all

movements. Time to accomplish task was the only depend­

ent variable analysed.

In this study, fifteen experimental operators were

used, twelve male and three female. The operators were

all given similar instructions in the manipulation of the

pedals. The subjects came to the laboratory twice during

the experimental period. The first time they ran the

series of pedals in one order, i.e., 1-2-3-4-5. Then on

the second day the subjects operated the pedals in the

reverse order, 5-4-3-2-1. Before an operator was tested,

he was told to adjust his position and his chair so that

he would be comfortable. Each pedal was operated by the

right foot for a period of three minutes, and the opera­

tors were told to work as fast as they could. After

Page 11: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

one and one-half minutes of work, the kymograph was set

into operation for approximately seventy-five cycles.

After approximately a three-minute work period, the opera­

tor had a three-minute rest which was followed by a prac­

tice period of one-half minute on the next pedal and

another rest period of one-half minute. At the end of

this half-minute rest the operator began another three-

minute work period* This procedure was carried through

for all operators and on all pedals.

Data were taken from the paper tape which passed

under the solenoid pencils of the kymograph. The average

values of both orderlngs (from 1 to 5 and 5 to 1) of the

pedals were taken. The data for the fifteen operators

were averaged and analysed.

Considering the five pedals studied and the condi­

tions under which the study was made, the following con­

clusions were made:

1. Pedal 1 required the least amount of time per

stroke.

2. Pedal 2 required 5% more time per stroke than

Pedal 1.

3. Pedal 3 required 6% more time per stroke than

Pedal 1. ,

4. Pedal 4 required 3^% nore time per stroke than

Pedal 1.

Page 12: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

5* Pedal 5 required 9% more time per stroke than

Pedal 1*

Lueien Lauru (4) analyzed various foot pedal ful­

crum arrangements utilizing the force platform to collect

the dependent variable data. The pedals tested in his

experimental procedure activated a cutting and stamping

press. Both the standing and sitting positions were

analyzed in his experimental work, but only a detailed

analysis was made of the sitting position. Again, as in

the Barnes experiment, five pedal arrangements were used.

The arrangements are shown in Figure 2.

Force measurement with Lauru's force platform indi­

cated that Pedal 5 fulcrum arrangement was by far the

best model.

Two related experimental works concerning levers

were performed in 1952 and 1953 by A. A. A. Caminada (3)

and R. E. Peale (5), respectively, at Purdue University.

These levers, however, were hand-operated. The 1952

project investigated the effect of size of a lever upon

the time required to operate it. The 1953 study was a

follow-up project in which the physical elements of the

experimental equipment duplicated the equipment of the

previous year.

The latter study attempted to determine an optional

value of a lever length at a given torque.

Page 13: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

General conclusions reached in the 1952 experiment

were:

1. When the torque increases and the lever size

is kept constant, the time required to operate it in­

creases proportionately to the torque.

2. The time required to operate a lever is nearly

proportional to the distance the hand has to travel.

3* The path that the hand has to travel is, proba­

bly, the predominant factor in determining the time for

operation.

Conclusions reached in the 1953 experiment, using

the same torque values of the previous year, were:

1. For a given torque the cycle time to operate a

lever decreases as the length is decreased up to an opti­

mal point. As the lever length decreases beyond this

optimal length, the cycle time increases. Optimal lever

length was found to be nine inches.

2. In general, as the torque was increased the

curve of lever length vs. cycle time tended to "flatten

out" and approach a straight line; therefore, the optimal

lever length became less definite.

Historically, experimental designs concerning the

foot pedal were confined to a single-factor design or, at

most, to a two-factor design.

Page 14: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

The importance of the present study lies in the

fact that nearly all of the variables incorporated in

previous research, as well as a nuB^er of other important

variables, were incorporated into one single study.

A description of the equipment and its use will

be discussed in Chapter II. Chapter III will discuss in

detail the experimental design and the control of various

factors during experimentation. Chapter IV will be de­

voted to an analysis of interrelationship of all the

variables introduced and their apparent effect, one upon

the other. Appendix A will be devoted to drawings of

specific components of the experimental device, and Appen-

dix B will reflect the results of a preliminary study.

Page 15: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

CHAPTER II

EQUIPMENT

The discussion of the experimental device used in

this study will be divided into two sections. The first

section will provide a description of the equipment in

general terms. The second section will relate to the use

of the device during experimentation.

Description of the Equipment

The experimental device used in this study was

electrical and mechcuiical in nature with the structural

portion built of wood.

For definitive purposes a few terms are described

in order to differentiate terminology used throughout the

remainder of the text.

1. Task is the amount of deflection (tensile) of

a helical spring upon depression of the pedal. The task

distance remained constant throughout all experimental

sessions. The task deflection was 7*5 centimeters.

2. Load will be defined as the force in inch-

pounds necessary to deflect a specific spring the distance

of 7.5 centimeters.

8

Page 16: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

3« Force is defined as the amount of pressure

exerted by the subject on the pedal.

With the experimental conditions a basic static re­

lationship Qb«Wa was adhered to where:

Q « effort expended in inch-pounds;

W « spring arm load in inch-pounds

for a 7.5 centimeter deflection;

a » perpendicular distance from the pivot

or lever arm fulcrum to the line of

force in the spring arm;

b " distance from the lever fulcrum point

to point of force application by sub­

ject's foot (ball).

Figure 3 portrays these relationships.

The foot pedal assembly. Figure 4, was constructed

entirely of wood and was adjustable to the appropriate

fulcrum point and allowed linkage adjustment for control

of mechanical advantage. The pedal component of the

assembly was eig hteen inches long and five inches wide

with a formed heel stop attached to the rear of the unit.

The dimensions of the pedal unit allowed positive contact

with the pedal for the entire surface of shoe sole and

heel for all subjects. Pedal action was accomplished by

use of a hinge attached to the underside of the pedal and

Page 17: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

10

a base pedestal. The entire pedal assembly was mounted

on a plywood base for the purpose of positioning and

rigid support of the pedal unit itself.

The entire frame. Figure 5, supporting some instru­

mentation, wiring terminal strips and linkage, took the

shape of an inverted "U." The frame was forty-eight

Inches in height and thirty inches in width. The front

of the frame. Figure 6, served as the subject's indica­

tor panel. This panel was cut to a height twenty inches

from the floor and two feet in width to allow for pedal

positioning and freedom of leg movement during experimenta­

tion.

Paz*t of the linkage between the pedal and the re­

sistance. Figure 7» was accomplished by use of a non-

stretching Dacz*on cord. This portion of the linkage made

contact with the pulley system. For stability in indi­

cator movement the portion of the linkage attached

directly to the spring resistance was one-fourth inch brass

tubing. The indicator assembly was attached directly to

this portion of the linkage. The tubing also offered a

rigid surface for braking pedal movement. This linkage

design functioned smoothly and with negligible friction.

The electrical portion of the equipment. Figure 8,

was designed to measure output of pedal movement auto­

matically. In a single depression of the pedal, accuracy

or control, reaction time, and travel time were measured.

Page 18: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

11

Figure 9 offers a schematic diagram of the electrical

circuity designed to achieve automatic measuring of the

dependent variables and automatic braking of the pedal.

The electrical timing devices used, measured time

in units of 1/100 of a second. Two were used: one to

measure reaction time, the other travel time. Reaction

time is defined as the time taken by subject from receipt

of visual stimulus to start of pedal depression. Travel

time is defined as the time taken from first movement of

the pedal until movement was braked.

A light stimulus was utilised to initiate action

by the subject. This light was mounted on the indicator

panel.

The sequence of events for the subject to perform

a single pedal depression was as follows:

1. Light switched on.

2. Pedal depressed by subject €md upward motion

of indicator with goal being task line (7*5 centimeter

task deflection of spring).

3. Braking occurred when the subject made his

Initial decision to stop pedal movement.

The proper electrical sequencing of these actions

by the subject was controlled by four relays and two micro-

switches. The microswltches were attached to either side

of the pedal, and the relays were mounted on the frame

and table. The release of a simple contact on the pedal

Page 19: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

12

assembly stopped the reaction timer after switching of

visual stimulus. The travel timer started measurement

when reaction timer stopped. The travel timer stopped

when pedal movement stopped.

Pedal movement was detected by an astatic cartridge

arm attached to the linkage. The cartridge movement on a

thin aluminum surface generated sound which, in turn, was

amplified to detect the slightest pedal activation. When

movement stopped, sound detection ceased and braking action

occurred.

The braking component of the electrical system was

a solenoid unit which, with extensions of metal strapping

material, enclosed the rigid tubing portion of the link­

age. Rubber-surfaced wooden blocks mounted within the

solenoid extensions clamped on the tubing when motion

stopped. This action offered positive braking action.

Proper electrical balance for the entire electri­

cal circuit was accomplished before each experimental

session by adjusting voltage.

Attitude of each subject's tibia in relation to the

plane of the floor was indexed by simple angular devices

constructed of wood.

Use of the Equipment

All sessions were accomplished with the subject in

a seated position. The chair used offered a formed

Page 20: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

13

back rest, «md all subjects were required to sit in a pos­

ture position so that the subject's back contacted the

chair back. The subject was then strapped to the chair

with a seat belt.

Tibia angle was indexed and chair raised or lowered

to minimize visual parallax with the panel. The upper leg

was checked for horizontal attitude, and proper axis align­

ment of the right leg and pedal were assured.

Each pedal depression and subsequent braking action

dictated that the accuracy measurement be read first on

the scale attached adjacent to the indicator track. Then

the travel time and reaction time were read and recorded.

Since four tibia attitudes were assigned to each experi­

mental session, the subject was required to move to a new

position after the prescribed number of trials at a par­

ticular tibia attitude.

Chapter III will discuss the experimental design

and the scheduling of variable factors for the research

study undertaken with this equipment.

Page 21: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

CHAPTER III

DESIGN OP THE EXPERIMENT

Discussion of Variable Factors

The independent variables included in this ex­

perimental project were carefully chosen to fit a real

life range of conditions confronted by operators of

pedal-activated mechanisms. Due to the fact that a num­

ber of variables were being investigated, some thought

was given to limiting the number of variables that were

introduced. For this reason all subjects assumed only a

seated position, and only male subjects were used.

Four fulcrum points were selected for study. These

were:

1. Directly underneath the ball of the foot.

2. Midway between the ball of the foot and each

subject's ankle joint.

3. Directly underneath the ankle joint.

4. Underneath the extreme rear (heel) of foot.

Fulcrum points forward of the ball of the foot were not in­

vestigated in this study due to the fact that previous

pedal studies have shown that pedals with this type of ful­

crum are not as effective as those included in this study.

14

Page 22: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

15

Resistances to pedal depression were introduced by

four helical springs. Each spring was carefully cali­

brated prior to experimentation in order to determine ten­

sile pressure in inch-pounds necessary to deflect each

spring 7.5 centimeters (2.86 inches).^ Calibration of

springs resulted in the following tensile forces necessary

to deflect the spring 7 5 centimeters:

Spring A - 12.8 inch-pounds

Spring B - 16.5 inch-pounds

Spring C - 21.3 inch-pounds

Spring D - 25#6 inch-pounds

The range of tensile forces adequately encompassed the

constant twenty inch-pounds resistance utilized by Barnes

(2).

Tibia or shinbone attitudes were introduced into

the design of the experiment in order to determine their

effect upon over-all pedal design. Tibia angles were

varied while the angular position of the pedal was held

constant at 30^. Pour tibia attitudes were incorporated

into the experimental design beginning with 90^. The

others were 100**, 110® and 120**. This chosen range of

attitude values includes that angle of the tibia required

7*5 centimeter deflection remained constant for all subjects for all experimental sessions.

Page 23: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

16

for maximum power to be exerted by the foot as shown by

Reijs (6). Converted to angular attitude, this maximum

power angle is 108*, His findings, measured by a dyna­

mometer, indicated that when the foot and tibia are at an

angle of 78* maximum power can be exerted by the foot in

a downward movement.

The trfiuismission of power through foot movement

created interest in the use of foot dimension as a vari­

able factor. In the movement of a human foot upon a

device such as a pedal, the ankle joint will function

differently depending upon fulcrum position. For example,

when the fulcrum point is located forward in relation to

the ankle joint, the joint will rotate during the depres­

sion of a pedal in the manner of a floating pivot.

Thus, a preliminary study was made of particular

male foot dimensions. Figure 10 illustrates the segments

of foot dimensions that were measured. All measurements

were taken of male subjects wearing Oxford-type footwear.

A device constructed in a shape similar to a com­

mon woodworker's square was used to take the measure­

ments. Plastic scales were attached to the appropriate

edge of the device, and measurement could be accomplished

directly and rapidly.

S«unples of twenty subjects were measured for the

dimensions a and d and for the dimensions a and c, and

Page 24: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

17

thirty subjects were measured for the dimensions a and

b.

Nearly all of the twenty subjects (a-d sample) were

contained in all three samples. A correlation coefficient

was calculated for the three samples with the following

results:

a-d 58 20 samples

a-c 65 20 samples

a-b • .88 30 samples

The high degree of correlation evident in the a-b dimen­

sions justified the fact that these dimensions, converted

to a ratio (a/b) and defined as the foot-ratio, were in­

troduced into the experiment as a variable factor. Note

that both the a and b dimensions have a common point of

reference, the ankle joint. The correlation result in­

creased the interest in the function of the ankle joint

in pedal movement. Identification of subjects with a par­

ticular a-b ratio was a comparatively easy matter due to

notation during the correlation study.

The total range of foot-ratio values noted during

the sample correlation studies extended from .80 to 1.13*

In order to achieve some balance in the experimental sched«

uling, four foot-ratio categories were established. Each

category was limited to a particular range. Within each

Page 25: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

18

category two subjects were identified. This procedure in

grouping subjects allowed the introduction of another vari­

able factor, that of replication within ratio category.

The replication factor was introduced specifically for the

purpose of attempting to determine if significance could

be detected with subjects within a particular category.

The grouping of subjects as described limited the number

of male subjects to eight. The limits established for

each foot-ratio category were:

.80 - .85

.86 - .93

.94 -1.00

1.01 -1.07

Each experimental combination was limited to five

trials, the trial being the last independent variable in­

troduced into the design.

The dependent variables were certain measures of

performance by each subject as he proceeded through the

sessions. Each pedal depression produced three experi­

mental values: reaction time, travel time, and a measure

of accuracy foot control. The type score, then, was the

dependent variable factor of the experimental design.

A number of factors were strictly controlled during

all experimental sessions. Mechanical advantage as

Page 26: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

19

impaired by each subject's foot during pedal depression

was an important consideration in the design of the physi­

cal components and experimental procedure. Obviously,

mechanical advantage will vary for each subject depending

on foot length. For this reason, the linkage point was

constructed to be adjustable, and through proper adjust­

ment no subject had a mechanical advantage over any other,

regardless of size of foot. The resistance arm was ad­

justed to six and one-half inches for all subjects at the

beginning of all sessions. This distance was measured

from point of pressure (ball of foot) to the linkage point.

Parallax in visual reference to indicator panel was

controlled by appropriate elevation or lowering of ad­

justable chair base. Each subject, regardless of stature,

had no visual difficulties in tracking the indicator to

the task line.

Since reaction time was a measure of subject per­

formance, bias due to subject age was minimized by estab­

lishing an age limit for experimental subjects. Subjects

utilized were restricted to an age range from twenty to

thirty-five years. This age range was selected in order

to have people with comparable reactions. All subjects

were Industrial engineering graduate students, with one

exception. Seven were Air Force Officers.

Page 27: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

20

The task was controlled by keeping it constant

throughout all sessions.

Environmental conditions for subject comfort during

sessions were controlled by the use of an air-conditioned

room.

Fatigue was controlled by assuring adequate rest

periods between sessions and holding each session to no

more than twenty minutes' duration.

Each subject was afforded the opportunity to "learn"

to use the pedal device before actual experimentation

began. This was done to assure that learning factor bias

was eliminated. All eight subjects performed twenty trials

at each of the four attitudes during the learning period.

Variable combinations of fulcrum point and resistance were

introduced at this time. Data were taken during the learn­

ing sessions for review and notation of stabilization in

each subject's performance. No subject experienced any

appreciable difficulties in learning to use the device.

Schedule of Subjects

Table 1 illustrates the schedule of subjects and the

combination of variable factors that they experienced dur­

ing a total of sixteen separate sessions.

Page 28: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

21

J .. •-'s.

••*•

I

• \ >

•- -

.'- n r r • • • T -

': • 1

•• - I

.-•1 ;

' I

;.;>. A t V

0C

I '

• I

> I "S -. r.

* I

- \ I

.. < . »

! i > C*

I I .

f " ' .

( • '

I

I »

1.. . -oi;:^s

Page 29: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

TABLE 1—Continued

22

? Ad 90® 100 no 120

Cc 100® no 120 90

Ac no® 120 90 100

Ba 120® 90 100 no Da 90® 100 no 120

Ab 100® no 120 90

Bb no® 120 90 100

Bo 120® 90 100 no

10 Db 100® no 120 90

Dd no® 120 90 100

Cb 120® 90 100 no Bd 90® 100 no 120

DC 100® no 120 90

Ca no® 120 90 100

Ad 120® 90 100 no Bb 90® 100 no 120

11 12 Bd no® 120 90 100

Ab 120® 90 100 no Da 90® 100 no 120

Db 100® no 120 90

Bb no® 120 90 100

Cb 120® 90 100 no Dd 90®

100 no 120

Ad 100® no 120 90

DC 120® 90 100 no Ac 90® 100 no 120

Bd 100® no 120 90

Cc no® 120 90 100

Ad 120® 90 100 no Dd 90® 100 no 120

Da 100® no 120 90

Ba no® 120 90 100

13 Da 90® 100 no 120

Ca 100® no 120 90

Ab no® 120 90 100

Aa 120® 90 100 no Db 90® 100 no 120

Ba 100® no 120 90

Be no® 120 90 100

Cc 120® 90 100

14 Ab 100® no 120 90

Cd no® 120 90 100

Cc 120® 90 100 no

Dd 90® 100 no 120

Cb 100® no 120 90

Aa no® 120 90 100

Ac 120® 90 100 no DC 90® 100 no

15 Cd no® 120 90 100

Bd 120® 90 100 no Ad 90® 100 no 120

Da 100® no 120 90

Aa no® 120 90 100

Be 120® 90 100 no Cb 90® 100 no 120 Ab 100® no 120

no 1 120 I 90

16 Bb 120® 90 100 no Aa 90® 100 no 120 Cd 100® no 120 90

Ab no® 120 90 100

Cd 120® 90 100 no

Da 90® 100 no 120 Ba 100® no 120 90 Dd 110® 120 90 100

Legend ^m^

Fulcrum Position

A r'x _ ^ •*

A - Ball B - Midpoint (be-

•1 1 • ! tween ankle joint and ball)

C - Ankle Joint D - Rear of Heel

Resistance (for 7.5 centimeter deflection)

a - 12.8 inch-pounds

b - 16.5 inch-pounds

c - 21.3 inch-pounds

d - 25.6 inch-pounds

1 1 t HI

Page 30: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

23

Each subject was confronted with a completely ran­

domized schedule of fulcrum point-resistance combinations.

The sixteen possible combinations of these factors dic­

tated the number of sessions that were to be held for each

subject. In any one session, however, the schedule was

designed to prevent a repetition of any one combination

during the same session. No more than two sessions were

held for any one person on any particular day.

The attitude factor was counterbalanced in effect

throughout the schedule. No subject assumed the same

tibia position at the start of testing until four sessions

had been completed. Only two subjects assumed the same

tibia attitude in any one session. This schedule design

minimized any systematic scheduling effect.

Experimental Procedure

Each experimental session, as scheduled, consumed

on the average approximately fifteen minutes of time. All

necessary adjustments in equipment were made prior to the

subject*8 arrival for his experimental session, except for

the mechanical advantage adjustment. After subject posi­

tioning, the mechanical advantage adjustment was made.

Trials were Initiated by means of a precompiled random

time list. The values of 1,2,...,5 seconds were random­

ized in order to provide random activation of the stimulus

Page 31: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

24

Recording Data

Figure 11 illustrates the format of the data sheet

used during this study. After each pedal depression the

accuracy measurement, travel time, and reaction time were

noted in that order.

The accuracy measurement was converted to a numeric

system adaptable to computer progreimmlng. A constant

value of 2.0 was added to each accuracy value for this

purpose. Accuracy was measured in tenths of centimeters

above or below the 7.5 centimeter task line. If, for ex­

ample, the subject stopped the indicator .2 of a centi­

meter above the task line, the value was recorded as <f.2.

Thus, the value recorded was 2.2. The value of 2.0 would

Indicate perfeet control or accuracy. All accuracy values

were noted algebraically on the data sheets but converted,

as stated above, before punching the data on IBM cards.

Reaction and travel time were noted directly as read.

The analysis and interpretation of results will be

discussed in Chapter IV.

Page 32: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

CHAPTER IV

ANALYSIS OF DATA AND CONCLUSIONS

The analysis of variance technique was utilized to

determine main effects and higher order interactions of

variables introduced into this study. To do this, the ex­

perimental data was punched on IBM cards for IBM computer

processing.

The 6.0.090 60K Anova Program was used. This pro­

gram will handle up to eighteen factors with a maximum of

999 levels per factor. With this program the data field

may be of any size, located in any position on the detail

card, with the only restriction being that the total un­

corrected sums of squares may not exceed thiirty-four

digits. In addition, the computer operator has the option

of picking up extra decimals in the calculations of the

sums of squares and means for additional accuracy where

desired.

Table 2 Illustrates the identification for sort

order, factors, levels, and codes used in IBM card pro­

cessing.

The design of the experiment generated 7680 experi­

mental values. Of this total, there were 2560 values each

25

Page 33: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

26

for reaction time, travel time, and accuracy. Each value

represented one punched card with appropriate coding and

experimental data.

TABLE 2

IDENTIFICATION TABLE

Field

5

10

15

20

25

30

35

40-41

Factor

Fulcrum Point

Resistance

Ratio

Attitude

Replication

Type Score

Trial

Observation

Level

Heel Ankle Mid-Point Ball

Light Light-Medium Medium Heavy

.80- .85

.86- .93

.94-1.00 1.01-1.07

90® 100® no® 120®

1 2

Reaction Time Travel Time Accuracy

1 - 5

Code

1 2 3 4

1 2 3 4

1 2 3 4

1 2 3 4

1 2 3

Sort Order 1 2 3 4 5

A

B

C

D

E

P

G

i 1 H5

•I

Hi

Page 34: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

27

Computer Processing

The entire lot of experimental data was processed

through the computer on the initial pass with the appropri­

ate seven-factor sums of squares control cards. Table 3

represents the results of the Seven-Factor Anova Analysis.

In Table 3 It can be seen that three main effects, eight

first-order interactions, ten second-order interactions,

three third-order interactions, and one fourth-order

interaction were significant at the 1% and 5% level.

Mean values were then obtained by further computer

processing for the above significant main effects and

interactions. Since the computer memory storage was ex­

ceeded on seven- and six-factor processing for the appro-

priate means, the two variables of replication and atti- 5

tude were dropped from the design in order to obtain the

means for the main effect and interactions of the five

remaining variables.

Analysis and Interpretation

The results of this design will be discussed under

the following topics but not specifically in the order

listed!

1. Fulcrum Main Effect - Composite Score

2. Resistance Main Effect - Composite Score

3. Foot-Ratio Main Effect - Composite Score

Page 35: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

28

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Page 36: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

29

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Page 38: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

31

M. Interactions - Composite Score

5. Fulcrum Main Effect - Type Score

6. Resistance Main Effect - Type Score

?• Foot-Ratio Main Effect - Type Score

8. Interactions - Type Score

In the analysis using composite score, a review

must be made of its content. Three type scores or de­

pendent variables were simultaneously recorded on each

trial of this study. For definition a listing follows:

1. Reaction time - the time a subject took to

begin pedal depression after receipt of visual stimulus.

2. Travel time - the time taken in pedal de­

pression to task line position, when braking occurred.

3. Accuracy - degree of departure, high or low,

if any, of indicator from task line.

Each of these scores measured an independent aspect

of performance of each subject on each trial. However,

while the primary interest in this study is in the joint

effects of each of the Independent variables and their

combined effect upon these three dependent variables, we

shall first consider the Independent variation upon the

composite score.

While the reader may find it unusual to add apples

and pears or, in this case, travel time, reaction time,

and accuracy, it is very important to know if the inde­

pendent variables do have the same effects upon the

Page 39: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

32

three scores. The composite score considers this rela­

tionship.

In Table 3 composite scores are observed to be sig­

nificant. In Figures 12 through 22 the mean effects of

the independent variables are charted.

In Figure 12 the effect of fulcrum position upon

the composite score can be observed. This effect shows

that the value of the composite score increases directly

as the fulcrum position moves from the heel out to the n

ball of the foot. ^

In Figure 13 the effect of resistance upon the com-i

posite score may be seen. Here, the effect is curvilinear I •I

rather than the linear effect of Figure 12. ;;

Figure 14 shows the foot-ratio effect. This effect J

is more curvilinear than in Figure 13. t

Figure 15 portrays the joint effect of fulcrum

point and resistance on the composite score. This effect

begins to get somewhat complicated. While the linear com­

ponent of fulcrum. Figure 12, is still observable, it

becomes highly erratic in trend when the curvilinear effect

of Figure 13 is superimposed.

Figure 16 shows the effect of superimposing the

mildly curvilinear effect of resistance to the highly cur­

vilinear effect of foot-ratio. Here, it can be noted that

while each Independent variable has a curvilinear effect

Page 40: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

33

separately, their joint effect is much more extreme as one

progresses to the highest resistance-ratio combinations.

Now, as to the significance of this effect, care

must be taken. The final evaluation of this effect can

be made only when this relationship is broken down in the

subsequent higher order interactions.

More specific meaning of the preceding phenomenon

may be more readily determined through analysis of the

interactions involving the type score factor.

Figure 17 shows the significant fulcrum point by

each type score interaction. Figure 17 definitely shows

the first concrete indication that travel time steadily

increased as the fulcrum point was positioned forward

from the rear of the pedal. Negative correlation between

travel time and reaction time appears as the fulcrum moves

from the point at rear of pedal to ankle point.

Accuracy, though consistently below task line, does

not depict appreciable variation, regardless of travel

time and fulcrum position.

Figure 18 charts resistance-type score interaction.

It shows that resistance has little effect on travel time;

in fact, during the course of this study travel time de­

creased when the heaviest resistance was imposed upon the

subjects. Note that reaction appears negatively corre­

lated to travel time. Accuracy was not appreciably af­

fected by the four levels of resistance.

Page 41: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

34

The second-order interaction of fulcrum point-

resistance-score interaction, charted in Figure 19, magni­

fies the relationships portrayed in Figures 17 and 18.

All foot-ratio subjects produced the shortest travel time

with the light spring but were affected by slower reac­

tion times. The subjects in foot-ratio 4 performed with

a decided decrease in travel time but with sharp increase

in reaction time as well. All resistance-ratio combina­

tions indicated little effect on accuracy, regardless of n

travel time. !i

Figure 20 notes the effect of foot-ratio upon type

score. Also, in comparison with Figure 14, the highly !

curvilinear effect was not primarily the result of travel

time. Here, the combined effects of reaction time and i.

accuracy had greater effect in degree of curvature. Fig- "

ure 20 indicates that subjects in the foot-ratio 1 cate­

gory appear to have the best control or accuracy, although

not to an appreciable degree.

The resistance-ratio-score interaction. Figure 21,

depicts further information concerning the graphic dis­

plays shown in Figures 18 and 20. Reaction time and re­

sistance appear positively correlated, while travel time

and accuracy appear negatively correlated.

Figure 22 shows the third-order interaction of

fulcrum point, resistance, foot-ratio, and type score

Page 42: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

35

Interaction. It offers the highest degree of interaction

and graphic magnification for the main factors in the

analysis. General upward trend in travel time is again

noted as fulcrum position is moved toward the ball of the

foot. Erratic variations in reaction time are noted for

all subjects with resistances cmd fulcrum position at

rear of pedal. Reaction time is significantly of longer

duration than with other resistance-fulcrum combinations.

Least variation in accuracy measurement appears with ful­

crum position under ankle joint. \

Conclusions

In discussing appropriate conclusions generated by

this research, one must put the issues in proper perspec­

tive. There are certainly a number of possible issues.

For example, one might ask, what is the optimum combina­

tion of these independent variables for a general pedal

design? Second, what is the optimum pedal design for ob­

taining accuracy under specific load? Third, what is the

optimum combination for total response time, reaction and

travel time, or for reaction time or for travel time

alone? The most significant result of this study is that

the answer to each of these questions cannot be the same.

However, an answer to each of these questions can be

specified; then, a detailed analysis of a graphic

n

Page 43: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

36

relationship, as shown in Figure 22, can assist in making

a determination.

In general, this study has shown that:

1. Travel time increases for pedal activation as

the fulcrum position is moved from heel toward the ball

of the foot.

2. Accuracy or control is not necessarily a re­

sult of speed of pedal movement.

3. Reaction to a stimulus appears slower when

lighter resistances are confronted by operator.

Specifically, analysis of Figure 22 will produce

the answers to the questions posed above depending upon

the condition specified. For example, what combination

produces the quickest pedal travel for subjects in foot-

ratio category 2? By analysis, foot-ratio 2 subjects can

manipulate pedals with fulcrum point at rear of heel and

heavier resistances more quickly.

For accuracy, a fulcrum position under the ankle

joint appears to give more consistent control of foot in

depression.

For reaction, subjects in foot-ratio 2 portray the

same rapid response throughout many combinations.

Figure 23 Illustrates some pedal arrangements for

optimum performance as specified. Arrangements are based

on data obtained from this study. It must be understood

Page 44: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

37

that the most significant finding of this study is that

optimization is dependent upon job specification and indi­

vidual operator. The variations in performance, shown by

subjects under experimental conditions with all combina­

tions, prove this point. We need to know how a specific

pedal mechanism will be utilized by an operator or opera­

tors. For example, will only one operator specifically

assigned to the machine activate the same pedal for ex­

tended periods of time, or will a particular machine be

pedal-activated by a number of different operators? The

arrangements, shown in Figure 23, take this into account

showing, first, a general pedal and, second, a pedal

which would be adjustable for an individual operator.

Recommendations for Further Study

This study has generated a number of questions con­

cerning various relationships. A portion of these could

be considered technical, another portion psychological.

However, confining ourselves to the original purpose, the

following recommendations for further study are made.

Reaction time, travel time, and accuracy data can

be processed separately for determining significance to

all other variable factors and graphic portrayals analyzed

in a manner similar to this study.

A further study should be undertaken, eliminating

the accuracy score. This could be done with the same

Page 45: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

38

design and experimental device. Task line would remain as

the goal, but subjects would depress pedal until task line

was reached or exceeded. This study would then determine

the relationships between reaction time and travel time

with no accuracy requirement. Another variation would be

the inclusion of a stop in physical component design which

would limit pedal travel. Comparisons of these two stud­

ies would be beneficial.

It is also recommended that an identical experiment

and design be repeated with the use of a force platform.

A study of this nature would explore the degree of ex­

penditure of effort as each subject was confronted with

the various experimental combinations.

The experimental design used in this study could

explore the standing position during pedal activation.

This independent variable could be incorporated into all

the studies mentioned above.

Finally, with a minimum of modification of the ex­

perimental device, vehicular braking studies could be

undertaken with all the variable factors utilized in this

research project.

Page 46: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

(9

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Page 47: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

' t ' I

/ . - - ^

> ^ I r . P . — L n u r i A ' n i .xpor -1 mont,,-) ]. (^ I i a l

Page 48: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

Ankle Joirit

Qb Wo

F i r . . 3 . - - • • ' " r c o - i i O n d l^•'1 n t, 1 o i i nh 1 pr.

Page 49: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

42

Pig. 4,—Pedal Assembly

Page 50: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

13

Fig. 5,—Side View of Frame Assembly

Page 51: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

44

Pig. 6.—Front of Frame Assembly

Page 52: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

15

I Fig. ?•—Pedal Linkage

Page 53: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

46

n

Pig . 8 , - - .E lec t r ica l Equipment

Page 54: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

in

^ \ > 'v/ V / V> I

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[:

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r >

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<"•) . t h i I •

Page 55: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

'J-:

r^riv\iQ Jo»r<>

F],:, l t ) . - - F o f ) l Dimrnr. Ion iint. lo :\\.\i'i\'

Page 56: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

^9

SUBJECTS NAME

AGE

A / B DIMENSION' A

RATIO

POSITION

ATTITUDE

FULCRUM POINT

DATA SHEET

DATE

B.

CODE

SPRING RESISTANCE IN-LBS IN-LBS IN -LBS. IN-LBS.

TRIALS:

RANDOM TIME REACTION TIME TRAVEL TIME ACCURACY

Fig. 11.—Sample Data Sheet

^HXA. T...NO.^U^..CAU CDUU

Page 57: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

.32"

50

8 -3" C/)

<D

(/> O O. E o o

.30-

.29-

.28 Heei Ankle Mid-point Bail

Fulcrum Position Fulcrum Main Effect

Fig. 12.—Fulcrum - Composite Score Main Effect

Page 58: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

51

.31 -a» o o

CO

r 30 w O Q. e o U

,29 1

.28 I 2

Light Light-Med. 3

Med. 4

Heavy

Resistance -Main Effect

Fig. 13.—Resistance - Composite Score Main Effect

Page 59: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

.31 -o o

CO

.•—

O .30 E o a

.29

52

.28 1 2 3 4

.80-85 .86-93 .94-1.00 I.0I-I.07

Ratio Main Effect Fig. 14.—Ratio - Composite Score Main Effect

Page 60: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

53

31 -

o o en

o 30 -

CO o o. E (3 29

28 -

27

Legend - order (Fulcrum - Resistance) Fulcrum Point Resistance

Hee l - I Light - I Ankle - 2 Llght-Med-2

Mid-point - 3 Medium -3 Ball - 4 Heavy - 4

H (- H 1- H 1 H

— c v j r o ^ — < \ j r o ^ — c M r o ^ — cvjro^ij. I I I I I I I I I I i I • I * •

— — cvJCMCsJcvJrorOrOro^^^'^f

Fulcrum-Resistance Interaction Fig. 15.—Fulcrum - Resistance - Composite Score Interaction

Page 61: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

5'*

.32

.31 " O

o

in

i . 30 E o o

.29

.28

Legend-order (Resistance-Ratio) Resistance Ratio

Light-I . 8 0 - . 8 5 - I Light Med.-2 . 8 6 - . 9 3 - 2

Medium-3 .94-1.00-3 Heavy-4 101 -1.07-4

— cvjrosr — cviro^ —cMro^ — cvJrO' I I I I I I I I I I I I • I I I

cvicvicMcsJrorororosr^^^

Resistance - Ratio Interaction Fig. 16.—Resistance - Ratio - Composite Score Interaction

Page 62: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

55

o D k . 3 O O

< ^»^

0> V) 10)

<D E

H

.55

.50

.45

40

35

.30*

.25 -

. 2 0 "

Legend Reaction time Travel time

X—Accuracy

Accurocy Tosk Line l.lcm.

•f Heel Ankle Mid-point Bali

^Accuracy task line indexed at .30 for clarity.

Fulcrum-Type Score Interaction

Fig. 17.—Fulcrum - Type Score Main Effect

Page 63: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

56

o o

O o

<

^^.50 o •^.45 E F .40

.35

. 30 « -

, 2 5 -

2 0 -

.1 5

Legend Reaction time ^Travel time

—X—Accuracy

Accurocy Tosk Line l.lcm

Light Light-med. Med. Heavy ^Accuracy task line indexed at .30 for clarity.

Resistance-Type Score Interaction

Fig, 18.—Resistance - Type Score Nain Effect

Page 64: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

57

o s §.55

<

-6-50 W

Q.45 + 0)

E.40

.35-

.30-

.25

.20

.15 I

Legend order (Fulc.um-Resistance) Fulcrum Heel - I "n'-'^ - 2

Mid-point-3 Ball- 4

Re^btG/.cs Lic^hv - I

Light med.-2 ^!odium-3 K^avy- 4

Accuracy Task Line l.lcm.

_, 1—I 1—I > i — I — I — I — I — » — I — I — - X .

Pig. 19.—Fulcrum - Resistance - Type Score Interaction

Page 65: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

58

o V .

3

0.55 -<

05.50 o ^ 4 5 + cu

E P.40 -

.35 -f

.30*

.25 -

.20 -

.15 -

Legend Reaction time Travel time

—X—Accuracy

Accurocy Tosk Line - . I cm.

.80-85 .86-93 .94-1.00 I.0I-I.07 ^Accuracy task line indexed at .30 for clarity.

Ratio-Type Score Interaction

Fig. 20.—Ratio - Type Score Interaction

Page 66: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

59

> » o o k. O O

<

'g.50 C/)

O -^.45 E P .40

.35 +

.30

.25-

. 2 0 -

.15--

Legend-order (Resistance-Ratio) Resistance Light-I

Light Med.-2 Medium-3 Heavy - 4

Ratio .80-85-1 .86-93-2 .93-1.00-3 1.01-1.07-4

Travel Time

Accurocy Tosk Line l.lcm.

Reaction Time

H 1 h H 1 f- H 1 - c v j r o ^ - c v j r o < r - c v i r o ^ y c v i r o ^ J L J - — J - c v J C V J C v i c v i r o r o r O K ) ^ ^ ^ ^

^Accuracy task line indexed at .30 for clarity

Resistance - Ratio- Type Interaction Fig. 21.—Resistance - Ratio - Type Score Interaction

Page 67: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

60

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Page 68: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

61

Optimal Pedal Arrangements Based On Researcti Data

\

Ankle joint-V

Fulcrum point

Specification: (Various number of operators on some pedal) Reaction, Speed and accuracy Resistance 12.80-16.50 inch-pounds Mectianlcal Advantage Constant For All Operators,

Ankle joint \

Fulcrunr) point

Specification: (One operator on some pedal Jong duration Reaction, speed and accuracy Adjustable for a specific foot ratio in re­gard to resistance, (see Figure 22) Mechanical advantage predetermined

Fig. 23.—Optimal Pedal Arrangements

Page 69: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

BIBLIOGRAPHY

(1) Barnes, Ralph M. Motion and Time Study, New York: John Wiley & Sonsl j"anuary, 1961, p, 286.

(2) Barnes, Ralph M.; Hardaway, Henry; and Podolsky, Odif, "Which Pedal Is Best?" Factory Management and Maintenance Magazine. New York: McGraw-Hill Book Co, January, 1942, pp. 98-99»

(3) Caminada, A. A. A. Master's Thesis, Purdue Univer­sity, 1952.

(4) Lauru, Lueien. "Physiological Study of Motions." The Advanced Management Magazine. Published by the Society for Advanced Management. Vol. 22, No. 2, pp. 17-24.

(5) Peale, R. E. Master's Thesis, Purdue University, 1953.

(6) ReiJs, J. H. 0. "Human Body Size and Capabilities in the Design of Vehicular Equipment." Harvard School of Public Health, Boston, Mass., 1953, pp, 38-40.

62

Page 70: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

APPMDIX

A. Sketches of Important Components of the Experimental Device

B. Preliminary Study of Foot-Ratio Correlation

63

Page 71: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

APPENDIX A: SKETCHES OF IMPORTANT COMPONENTS OF THE EXPERIMENTAL DEVICE

Dacron Cord ^ Linkage —^

• < . . .

Half Sections Wood Clamped to Cord

Cartridge

Alunninunr) Strip

Astatic Cartridge Assembly

64

Page 72: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

65

rV ^

Heavy Gauge''^ Copper Wire

i

r Brass LinKage Section

:S

V Front Panel

= osition

Indicotor Assembly

Page 73: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

66

Solenoid Unit

r

^

>

Brass Linkage

/, Wooden Block K / Broke Shoes

/_ Rubber Surfaced

O O O GO o

\

• < ^

Movement of Solenoid Arm on Activation

Broke Assembly

Page 74: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

APPENDIX B: PRELIMINARY STUDY OF POOT-RATIO CORRELATION

The following listing of actual (a-b) measurements

taken prior to experimentation resulted in a correlation

coefficient of .88. The coefficient was calculated by

the relationship

^ ngxy -^xgy

[n£x^-(^x)^3[n£xy^-(£y)^]

Subject Number

1

2

3

i|

5

6

7

6

9

10

11

12

13

IM

a Dimension

4.625

4.000

5.375

4.000

4.625

4.250

4.875

4.250

4.625

4.750

4.500

4.375

4.500

5.250

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

b Dimension

4.750

3.375

4.750

4.000

4.250

4.250

5.000

4.308

4.750

5.000

4.500

4.500

4.375

4.750

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

Inches

67

Page 75: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS

68

Subject Number

15

16

17

18

19

20

21

22

23

24

25

26

27

28

29

30

a Dimension

4.125

4.625

5.000

4.625

4.875

4.500

4.625

4.500

4.750

4.000

4.750

4.500

4.500

4.750

4.250

4.250

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

b Dimension

4.250

4.625

5.125

5.125

5.000

4.500

4.875

4.500

5.250

4.250

5.000

4.500

4.500

4.625

4.250

4.500

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

inches

Page 76: AN OPTIMAL DESIGN FOR A FOOT ACTIVATED A THESIS