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MECHANICS OF METAL CUTTING

Mechanics of metal cutting

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Page 1: Mechanics of metal cutting

MECHANICS OF METAL CUTTING

Page 2: Mechanics of metal cutting

Topics to be covered

Inroduction to Machining Technology Cutting Models Turning Forces Merchants Circle Power & Energies

Page 3: Mechanics of metal cutting

Elements of Metal Cutting

Page 4: Mechanics of metal cutting

Tool

Workpiece

Chip

Heat Generation Zones

(Dependent on sharpnessof tool)

(Dependent on )

(Dependent on

10%

30%

60%

Page 5: Mechanics of metal cutting

Tool TerminologyTool Terminology

Side relief angle

Side cutting edge angle(SCEA)

Clearance or end relief angle

Back Rake(BR),+

Side Rake (SR), +

End Cuttingedge angle(ECEA)

Nose Radius

TurningCutting edge

FacingCutting edge

Page 6: Mechanics of metal cutting

Cutting Geometry

Page 7: Mechanics of metal cutting
Page 8: Mechanics of metal cutting

Material Removal RateMRR vfd

Roughing(R)

f 0.4 1.25mm / rev

d 2.5 20mm

Finishing(F)

f 0.125 0.4mm / rev

d 0.75 2.0mm

vR vF

Page 9: Mechanics of metal cutting

Cutting Models

ORTHOGONAL GEOMETRY OBLIQUE GEOMETRY

Tool

workpiece

Tool

workpiece

Page 10: Mechanics of metal cutting

Assumptions(Orthogonal Cutting Model)

The cutting edge is a straight line extending perpendicular to the direction of motion, and it generates a plane surface as the work moves past it.

The tool is perfectly sharp (no contact along the clearance face).

The shearing surface is a plane extending upward from the cutting edge.

The chip does not flow to either side The depth of cut/chip thickness is constant uniform

relative velocity between work and tool Continuous chip, no built-up-edge (BUE)

Page 11: Mechanics of metal cutting

Orthogonal Cutting

r to

tc

ls sinls cos( )

tan r cos

1 rsin

AC

BD

AD DC

BDtan( ) cot

Page 12: Mechanics of metal cutting

F t

FC

Fr

DIRECTION OF ROTATION

WORKPIECE

CUTTING TOOL

DIRECTION OF FEED

Velocity of Tool relative to workpiece V

Longitudinal 'Thrust' Force (27%)

Radial Force (6%)

Tangential 'Cutting' Force (67%)

‘Turning’ Forces For Orthogonal Model

End view section 'A'-'A'Note: For the 2D Orthogonal Mechanistic Model we will ignore the radial component

Ft

'A' 'A'

cF

Page 13: Mechanics of metal cutting

FL

FC

Fr

DIRECTION OF ROTATION

WORKPIECE

CUTTING TOOL

DIRECTION OF FEED

Velocity of Tool relative to workpiece V

Longitudinal Force

Radial Force ‘Thrust’ Force

Tangential Force 'Cutting' Force

‘Facing’ Forces For Orthogonal Model

End view

Note: For the 2D Orthogonal Mechanistic Model we will ignore the Longitudinal component

Page 14: Mechanics of metal cutting

'Turning' Terminology

N is the speed in rpmD is the diameter of the

workpiecef is the feed (linear

distance/rev)d is the depth of cutV is the surface speed

= DN

Standard Terms

Beware, for turning: In the generalized orthogonal model depth of cut (to) is f (the feed), and width of cut (w) is d (the depth of cut)

N

D

d mm

feed (mm/rev)

Tool

Workpiece

rpm

Page 15: Mechanics of metal cutting

Orthogonal Cutting Model (Simple 2D mechanistic model)

Mechanism: Chips produced by the shearing process along the shear plane

t 0

+

Rake Angle

Chip

Workpiece

Clearance AngleShear Angle

t c

depth of cut

Chip thickness

Tool

Velocity V

tool

Page 16: Mechanics of metal cutting

tool

Cutting Ratio(or chip thicknes ratio)

As Sin =to

ABand Cos-) =

tc

AB

Chip thickness ratio (r) =t0

tc=

sincos( )

tc

to

A

B

Chip

Workpiece

Page 17: Mechanics of metal cutting

Experimental Determination ofCutting Ratio

Shear angle may be obtained either from photo-micrographs or assume volume continuity (no chip density change):

Since t0w 0L0 = tcw cLc and w 0=w c (exp. evidence)

Cutting ratio , r = t 0tc

= L cL0

i.e. Measure length of chips (easier than thickness)

w

tL

0

0

0

wc

Lc

ct

Page 18: Mechanics of metal cutting

Shear Plane Length

and Angle

Shear plane length AB =t0

sinShear plane angle () = Tan

-1 rcos1-rsin

or make an assumption, such as adjusts to minimize cutting force: = 45

0+ /2 - /2 (Merchant)

t c

to

A

B

Chip

tool

Workpiece

Page 19: Mechanics of metal cutting

Velocities(2D Orthogonal

Model)

Velocity Diagram

From mass continuity: Vto = V ctc

From the Velocity diagram:

V s = Vcos

cos( )

V c = Vr and V c = Vsin

cos( )

(Chip relative to workpiece)

V = Chip Velocity (Chip relative to tool)

Tool

Workpiece

Chip

Vs V = Cutting Velocity

(Tool relative to workpiece)

Shear Velocity

c

Vs

Vc

V

Page 20: Mechanics of metal cutting

Cutting Forces(2D Orthogonal Cutting)

Free Body Diagram

Generally we know:Tool geometry & typeWorkpiece material

and we wish to know:F = Cutting ForceF = Thrust ForceF = Friction ForceN = Normal ForceF = Shear ForceF = Force Normal

to Shear

c

t

s

n

Tool

Workpiece

Chip

Dynamometer

R

R

R

R

FcFt

sF

FnN

F

Page 21: Mechanics of metal cutting

Force Circle Diagram(Merchants Circle)

R

Ft

Fc

Tool

F

N

Fs

Fn

Page 22: Mechanics of metal cutting

Results fromForce Circle Diagram

(Merchant's Circle)

Friction Force F = Fcsin + Ftcos

Normal Force N = Fccos - Ftsin

Shear Force Fs = Fccos - Ftsin

= F/N and = tan typically 0.5 - 2.0)

Force Normal to Shear plane Fn = Fcsin + Ftcos

Page 23: Mechanics of metal cutting

Forces on the Cutting Tool

and the workpiece

Importance: Stiffness of tool holder, stiffness of machine, and stiffness of workpiece must be sufficient to avoid significant deflections (dimensional accuracy and surface finish)

Primary cause: Friction force of chip up rake face + Shearing force along shear plane

Cutting speed does not effect tool forces much (friction forces decrease slightly as velocity increases; static friction is the greatest)

The greater the depth of cut the greater the forces on the tool Using a coolant reduces the forces slightly but greatly

increases tool life

Page 24: Mechanics of metal cutting

Stresses On the Shear plane:

Normal Stress = s = Normal Force / Area =Fn

AB w=

Fnsintow

Shear Stress = s = Shear Force / Area =Fs

AB w=

Fssintow

On the tool rake face: = Normal Force / Area = N

tc w(often assume tc = contact length)

= Shear Force / Area = Ftc w

Note: s = y = yield strength of the material in shear

Page 25: Mechanics of metal cutting

Power

•Power (or energy consumed per unit time) is the product of force and velocity. Power at the cutting spindle:

•Power is dissipated mainly in the shear zone and on the rake face:

•Actual Motor Power requirements will depend on machine efficiency E (%):

Cutting Power Pc = FcV

Power for Shearing Ps = FsVs

Friction Power Pf = FVc

Motor Power Required =Pc

Ex 100

Page 26: Mechanics of metal cutting

Material Removal Rate (MRR)

Material Removal Rate (MRR) = Volume RemovedTime

Volume Removed = Lwto

Time to move a distance L = L/V

Therefore, MRR =Lwto

L/V= Vwto

MRR = Cutting velocity x width of cut x depth of cut

Page 27: Mechanics of metal cutting

Specific Cutting Energy(or Unit Power)

Energy required to remove a unit volume of material (often quoted as a function of workpiece material, tool and process:

Ut = EnergyVolume Removed

= Energy per unit timeVolume Removed per unit time

Specific Energy for shearing Us =FsVs

Vwto

Specific Energy for friction Uf =FVc

Vwto= Fr

wto

Ut =Cutting Power (Pc)

Material Removal Rate (MRR)=

FcVVwto

=Fc

wto

Page 28: Mechanics of metal cutting

Specific Cutting EnergyDecomposition

1. Shear Energy/unit volume (Us)(required for deformation in shear zone)

2. Friction Energy/unit volume (Uf)(expended as chip slides along rake face)

3. Chip curl energy/unit volume (Uc)(expended in curling the chip)

4. Kinetic Energy/unit volume (Um)(required to accelerate chip)

Ut = Us + Uf +Uc +Um

Page 29: Mechanics of metal cutting

Specific Cutting EnergyRelationship to Shear strength of Material

SHEAR ENERGY / UNIT VOLUME Specific Energy for shearing Us =

FsVs

Vwto

FRICTION ENERGY / UNIT VOLUME

Specific Energy for friction Uf =FVc

Vwto= Fr

wto= F

wtc=

APPROXIMATE TOTAL SPECIFIC CUTTING ENERGY

Ut = Us + Uf = s+ y1+)

U s =scos

sin cos( )= s.

Page 30: Mechanics of metal cutting

Relation between Pressure and Cutting velocity

Page 31: Mechanics of metal cutting

Effect of Rake angle on Cutting Force

Page 32: Mechanics of metal cutting

Average Unit Horsepower Values of Energy per unit volume

Page 33: Mechanics of metal cutting

Typical Orthogonal Model Violations

• Geometry and form Violations (i.e. non zero angles of inclination, not sharp - radiused end)

• Shear takes place over a volume (not a line or plane)

• Cutting is never a purely continuous process (cracks develop in chip; material not homogeneous)

• 'Size Effect' - larger stresses are required to produce deformation when the chip thickness is small (statistical probability of imperfection in the shear zone)

• BUE - some workpiece material 'welds' to the tool face (cyclic in nature)