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Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown...

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Lean and edge angle Lean angle and balancing centrifugal forces –changes with speed and slope Edge angle and geometric turning –considering side cut radius Angulation –difference between edge and lean angles
23
Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic Institute Worcester, Massachusetts,
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Page 1: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

Modeling Edging Forces in Skiing using Merchant's Theory

for Metal Cutting

Christopher A. BrownMechanical Engineering Department

Worcester Polytechnic InstituteWorcester, Massachusetts, USA

Page 2: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

outline

• Lean and edge angle– speed, radius, side cut and angulation

• Ski-snow forces– Merchant theory– friction, edge angle and penetration

Page 3: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

Lean and edge angle

• Lean angle and balancing centrifugal forces– changes with speed and slope

• Edge angle and geometric turning– considering side cut radius

• Angulation– difference between edge and lean angles

Page 4: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

lean angle

mv²/r

mg cos

lean angle

)cos(**)tan(

2

grvLeanAngle

Page 5: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

edgeangle

edge angle

Page 6: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

lean angle vs. turn radius for 5 slopesV= const 20m/s

30

45

60

75

90

0 10 20 30 40 50 60

turn radius (m)

lean

ang

le (d

eg)

50°

10°

Page 7: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

lean angle vs. turn radius for 5 speedsSlope= const 15 deg.

15

30

45

60

75

90

0 10 20 30 40 50 60turn radius (m)

lean

ang

le (d

eg)

15m/s 20m/s30m/s

25m/s

35m/s

Page 8: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

Length (L)

r

Cd

rCd

LCd

*24

22

Page 9: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

waist

edge angle

Cd

sidecut

snow

ski

cossidecutCd

Page 10: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

Rossignol

Volkl

K2

SL

Type

SG

GS

Model

DH

P 40

95 Pro

Length (m)

Biaxial

GSSL

GS

P 40

P 20P 30

0.00921

Sidecut (m)

0.01238

0.00978

0.009380.01122

0.00702

0.00850

1.6311.641

1.670

1.9061.7461.576

1.936

max. radius (m)

36

24324866

40

34

Page 11: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

edge angle vs. turn radius for different skis

0

10

20

30

40

50

60

70

80

90

0 10 20 30 40 50 60

turn radius (m)

edge

ang

le (d

eg)

Volkl SG

Volkl GS

Volkl DH

Volkl SL

Rossignol SLRossignol GSK2 GS

Page 12: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

angulation angle

edge angle

lean angle

angulation = edge - lean

Page 13: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

angulation vs. radius

-45

-35

-25

-15

-5

5

0 10 20 30 40 50 60 70turn radius (m)

angu

latio

n (d

eg)

speed=20m/s slope=15°

Volkl SL

Rossignol GS

Volkl GS

Rossignol SL

K2 GS

Volkl SG

Volkl DH

Page 14: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

Ski snow forces -Machining analogy

• Tool = Ski• Workpiece = Snow• Cutting = Skidding

• limiting condition on carving

• Cutting force = Turning force• Rake angle = Edge angle (+90 deg)

Page 15: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

M

Fr

Fc

Ft

SIDE WALL(relief face)

SKI(tool)

(negative rake)

EDGE ANGLE(90+rake)

p

SHEAR PLANE

Shear Angleø

SPRAY

(chip)

Page 16: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

F

Critical Angle

from Brown and Outwater 1989

Page 17: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

from Brown and Outwater 1989 On the skiability of snow,

Page 18: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

Objectives of machining calculations

- minimum conditions for carving

• Turning force from mass, speed and radius• Edge penetration

– as a function of edge angle and friction• Thrust force (normal to the snow)

– can be influenced by body movements

Page 19: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

FcFn

FtR

N

F

--

-

pFs

SnowSki

Force relationships

ForcesFc = centrifugal

(cutting)Ft = thrustFs = shearFn = normal to

shear planeF = friction on skiN = normal to ski

shear angleedge angle

Page 20: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

FcFn

FtR

N

F

--

-

pFs

snowski

Fc = Fs cos + Fn sin

Fn = Fs / tan(--)

Fc = Fs(cos + sin / tan(--)) = (-)/2

Merchant’s solutionpredicts where the snow will fail when

skidding starts - essential for the solution

Merchant solution modified for edge angle

Page 21: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

Conditions for carving

Fs = As As = Ls p / sin

As: area of the shear planep: edge penetration

Ls: length of the edge in the snow: shear strength of the snow

Fc < p Ls / (cos + (sin / tan(--)))

p > Fc tan(--)

Ls (cos tan(--) + sin )

Page 22: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

discussion

• Negative now angulation predominates • Edge roundness, penetration and length

– shorter skis should hold better• Penetration can be a function of snow

strength• Leg strength should put a lower limit on

edge angle

Page 23: Modeling Edging Forces in Skiing using Merchant's Theory for Metal Cutting Christopher A. Brown Mechanical Engineering Department Worcester Polytechnic.

acknowledgements

Thanks to Chris Hamel and Mike Malchiodi ofWPI for help in preparation and equation checking.

Thanks to Dan Mote for explaining that skiing is machining.

Thanks to Branny von Turkovich for teaching memachining.


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