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10/24/2023 1
Cutting force
Cutting force components and their
significances
10/24/2023
Cutting force
2
Cutting force R resolved into PX, PY and PZTurning force resolved into PZ, PX and PY
R
Significance of PZ, PX and PY
10/24/2023
Cutting force
3
 PZ : called the main or major component as it is the
largest in magnitude. It is also called power component
as it being acting along and being multiplied by VC
decides cutting power (PZ.VC) consumption.
 Py : may not be that large in magnitude but is
responsible for causing dimensional inaccuracy and
vibration.
 PX : It, even if larger than PY, is least harmful and hence
least significant.
The Cutting Force
10/24/2023
P
Ft
Fc
Fc – Cutting force, Ft – Thrust force
 Externally applied forces
4
Cutting force
The cutting force cont’d…
10/24/2023
F
F – Friction force, Fn– Normal force
 Forces on the tool side
Fn
5
Cutting force
The cutting force cont’d…
10/24/2023
Fco
Fs – Shear force, Fco– Compressive force
 Forces on the chip side,
Fs
6
Cutting force
The cutting force cont’d…
10/24/2023
Fco
Fs
F
Fn
R
Ft
Fc
Merchant’s Circle
β
β – friction angle
α
α
β -α
 Merchant’s theory
 



 


2
1
4
7
Cutting force
Cutting force cont’d…
10/24/2023
 2
1
2
2
t
c F
F
R 

 2
1
2
2
n
f F
F
R 

 2
1
2
2
co
s F
F
R 

The shear force
s
F To shear a work material can be expressed in terms
of
cutting force c
F

 sin
cos t
c
s F
F
F 

Area of shear is given by
s
A

sin
c
s
A
A 
8
Cutting force
As
The cutting force cont’d…
10/24/2023
The shear strength of a material on the shear plane
may be obtained by
s

c
t
c
s
s
s
A
F
F
A
F 



sin
)
sin
cos
( 


Ernest and merchant theory suggests that is formed
in such a way that the energy required to shear a material
will be minimum.

Fco
Fs
R


 

)
cos( 

 

 R
s F
F



sin
c
s
s
s
s
A
A
F 

s

s
A
C
A
Shear strength
Area of shear
Area of uncut chip
9
Cutting force
The cutting force cont’d…
10/24/2023
 













cos
1
sin
c
s
R
A
F
)
cos( 
 
 R
C F
F
 
 
















cos
cos
sin
c
s
c
A
F
The equation my now be differentiated with respect to
equal to zero to find the value of for which is
minimum.

 c
F
0


d
dFc
 


  

 2
1
4
Solution
10
Cutting force
The cutting force cont’d…
10/24/2023
The result didn’t agree with the experimental, since the assump
didn’t considered the dependency of shear stress with normal s
Merchant reconsidered the assumption and he included his new
Assumption
11
Cutting force
The cutting force cont’d…
10/24/2023
)
sin( 

 

 R
co F
F
Fco
Fs
R


 




sin
c
s
s
s
co
A
A
F 

))
sin(
(
sin




 

 R
c
s F
A
s
s




 

 )
cot(
)
cot( 



 

 s
s
)
cot( 








 s
so
s k
)
tan(
1 








k
so
s
12
Cutting force
The cutting force cont’d…
10/24/2023
)
,
,
( 


 f
s 
))
tan(
1
)(
cos(
sin
)
cos(

















k
A
F c
so
C
The new equation for c
F
• It is now assumed that and are constants for a partic
Material
K so

• and are constants for the cutting operation
c
A 
0


d
dFc
 


 

 c
2
1 c Is constant
13
Cutting force
Lee and Shafer’s solution
10/24/2023
The theory of lee and Shafer's was the result of
an attempt to apply the plasticity and slip lines
theory to orthogonal metal cutting
Assumptions
 The material is rigid
 The behavior of the material is independent of the
rate of deformation
 The effect of temperature during deformation is
neglected
14
Cutting force
Lee and Shafer’s solution
cont’d…
10/24/2023
• ABC is deformation zone
•AB shear plane
•AC is stress free so that slip
lines
meet this line at an angle of 45
•Slip lines :
•Parallel to AB
•Perpendicular to AB
 


  

 4
The theory of lee and Shafer's is not applied for tools
with negative rake angle .
15
Cutting force
Influence of cutting parameters on
cutting force
10/24/2023
16
Cutting force
Friction force
10/24/2023
Sticking friction
Sliding friction
r
A a
A
real area Apparent area
r
f
f A
F 

y
n
r
F
A


n
f
F
F


f
F
f
 Shear strength
Friction force
n
F Normal force
17
Cutting force
Model of chip–tool friction in
orthogonal cutting
10/24/2023
18
Cutting force
Friction force cont’d…
10/24/2023
It is assumed that the stress distribution on the tool face could
be represented by the expression
f
f 
 
y
f qx


The maximum normal stress occurs when
and therefore
max
f
 f
l
x 
y
f qx

m
ax

y
f
f l
q

 max

y
l
x
f
f f
)
(
max

 
19
Cutting force
Force of friction cont’d…
10/24/2023
)
1
(
)
( 1
max
y
l
l
l
a
l
a
F y
f
y
st
f
w
f
st
w
st
f







)
1
(
max
y
l
a
F
f
w
f
n















f
st
f
st
n
f
l
l
y
F
F
1
tan
max




20
Cutting force
Cutting forces on turning
10/24/2023
Cutting force
Feed force
Radial force
Thrust force
c
F
f
F
r
F
D
F
•No motion on the radial
No work done by radial
motion
• The feed force is negligible
•Power(P) needed for turning is :
60
c
cV
F
P   
Watt
21
Cutting force
Specific cutting Energy
10/24/2023
The rate of energy consumption during machining
is
m
P
V
F
P c
m 
The energy consumed per unit volume of metal
removed, specific cutting energy is
s
P
c
c
w
m
s
A
F
Z
P
P 

m
P
c
F
s
P
w
Z
Power consumed
Cutting force
Specific cutting energy
Metal removal rate
Un deformed chip cross
section
c
A
22
Cutting force
Shaping and planning
10/24/2023
Cutting force
23
Shaping operation
10/24/2023
Cutting force
24


cos
/
cos
1
d
w
f
t


 Primary principal cutting edge angle
Forces on Shaping
10/24/2023
Cutting force
25


sin
cos
T
n
T
f
F
F
F
F


T
c
F
F cutting component acts against v
Thrust component perpendicular to transient
surface
n
f
F
F Feed component
Normal component
Forces in Drilling
10/24/2023
Cutting force
26
2
/
f
f Feed per revolution
Feed per cutting
edge


sin
)
2
/
(
sin
)
2
/
(
1
D
w
f
t








 



sin
tan
)
/
2
(
tan 1 D
r


r Radius of the point on the cutting
rake angle
Helix angle

2

2
Force on drilling cont’d…
10/24/2023
Cutting force
27
Development of torque and thrust
during drilling
friction
ch
T F
F
F
F 

 
sin
2
ch
F
F Total Thrust force
Force on chisel edge
friction
ch
c M
M
z
F
M 


ch
M
M
Total Moment
Moment due to chisel
edge
80%M
8%M
12%M

sin
5
6
.
0
T
c
F
F
D
F
M



Forces on Milling
10/24/2023
Cutting force
28
D
d
Nn
V
t
c
f
c
2
max 
D
d
Nn
V
t
c
f
ave 
ave
c
t
t max Max. uncut chip thickness
Average chip thickness
t
f
c
t d

2
D

Forces on milling cont’d…
10/24/2023
Cutting force
29
Thrust force doesn't cause any torque
The total torque is caused by the cutting force
Components of milling force
C
F
T
F )
2
/
(
_
_ d
F
M c
tooth
cutting
one 
d Diameter of the cutter
Arbor rotation and torque

Variation of torque due to single cutting

Forces on milling cont’d…
10/24/2023
Cutting force
30
Z

 2

)
i
Z

 2

)
ii
Z

 2

)
iii
Type of tooth Nature of torque






Power consumed by machine
tool
10/24/2023
Cutting force
31
m
m
e
P
P


m
e
m
P
P

Power consumed
Electric Power consumed by machine tool spindle
rotor
Machine tool transmission efficiency
4
.
0

 t
P
P o
s
t
P
Ps
0
Specific cutting energy
A constant in (J/mm3) depends on tool material
Uncut chip thickness in mm

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5.pptx

  • 2. Cutting force components and their significances 10/24/2023 Cutting force 2 Cutting force R resolved into PX, PY and PZTurning force resolved into PZ, PX and PY R
  • 3. Significance of PZ, PX and PY 10/24/2023 Cutting force 3  PZ : called the main or major component as it is the largest in magnitude. It is also called power component as it being acting along and being multiplied by VC decides cutting power (PZ.VC) consumption.  Py : may not be that large in magnitude but is responsible for causing dimensional inaccuracy and vibration.  PX : It, even if larger than PY, is least harmful and hence least significant.
  • 4. The Cutting Force 10/24/2023 P Ft Fc Fc – Cutting force, Ft – Thrust force  Externally applied forces 4 Cutting force
  • 5. The cutting force cont’d… 10/24/2023 F F – Friction force, Fn– Normal force  Forces on the tool side Fn 5 Cutting force
  • 6. The cutting force cont’d… 10/24/2023 Fco Fs – Shear force, Fco– Compressive force  Forces on the chip side, Fs 6 Cutting force
  • 7. The cutting force cont’d… 10/24/2023 Fco Fs F Fn R Ft Fc Merchant’s Circle β β – friction angle α α β -α  Merchant’s theory          2 1 4 7 Cutting force
  • 8. Cutting force cont’d… 10/24/2023  2 1 2 2 t c F F R    2 1 2 2 n f F F R    2 1 2 2 co s F F R   The shear force s F To shear a work material can be expressed in terms of cutting force c F   sin cos t c s F F F   Area of shear is given by s A  sin c s A A  8 Cutting force As
  • 9. The cutting force cont’d… 10/24/2023 The shear strength of a material on the shear plane may be obtained by s  c t c s s s A F F A F     sin ) sin cos (    Ernest and merchant theory suggests that is formed in such a way that the energy required to shear a material will be minimum.  Fco Fs R      ) cos(       R s F F    sin c s s s s A A F   s  s A C A Shear strength Area of shear Area of uncut chip 9 Cutting force
  • 10. The cutting force cont’d… 10/24/2023                cos 1 sin c s R A F ) cos(     R C F F                     cos cos sin c s c A F The equation my now be differentiated with respect to equal to zero to find the value of for which is minimum.   c F 0   d dFc          2 1 4 Solution 10 Cutting force
  • 11. The cutting force cont’d… 10/24/2023 The result didn’t agree with the experimental, since the assump didn’t considered the dependency of shear stress with normal s Merchant reconsidered the assumption and he included his new Assumption 11 Cutting force
  • 12. The cutting force cont’d… 10/24/2023 ) sin(       R co F F Fco Fs R         sin c s s s co A A F   )) sin( ( sin         R c s F A s s         ) cot( ) cot(         s s ) cot(           s so s k ) tan( 1          k so s 12 Cutting force
  • 13. The cutting force cont’d… 10/24/2023 ) , , (     f s  )) tan( 1 )( cos( sin ) cos(                  k A F c so C The new equation for c F • It is now assumed that and are constants for a partic Material K so  • and are constants for the cutting operation c A  0   d dFc         c 2 1 c Is constant 13 Cutting force
  • 14. Lee and Shafer’s solution 10/24/2023 The theory of lee and Shafer's was the result of an attempt to apply the plasticity and slip lines theory to orthogonal metal cutting Assumptions  The material is rigid  The behavior of the material is independent of the rate of deformation  The effect of temperature during deformation is neglected 14 Cutting force
  • 15. Lee and Shafer’s solution cont’d… 10/24/2023 • ABC is deformation zone •AB shear plane •AC is stress free so that slip lines meet this line at an angle of 45 •Slip lines : •Parallel to AB •Perpendicular to AB          4 The theory of lee and Shafer's is not applied for tools with negative rake angle . 15 Cutting force
  • 16. Influence of cutting parameters on cutting force 10/24/2023 16 Cutting force
  • 17. Friction force 10/24/2023 Sticking friction Sliding friction r A a A real area Apparent area r f f A F   y n r F A   n f F F   f F f  Shear strength Friction force n F Normal force 17 Cutting force
  • 18. Model of chip–tool friction in orthogonal cutting 10/24/2023 18 Cutting force
  • 19. Friction force cont’d… 10/24/2023 It is assumed that the stress distribution on the tool face could be represented by the expression f f    y f qx   The maximum normal stress occurs when and therefore max f  f l x  y f qx  m ax  y f f l q   max  y l x f f f ) ( max    19 Cutting force
  • 20. Force of friction cont’d… 10/24/2023 ) 1 ( ) ( 1 max y l l l a l a F y f y st f w f st w st f        ) 1 ( max y l a F f w f n                f st f st n f l l y F F 1 tan max     20 Cutting force
  • 21. Cutting forces on turning 10/24/2023 Cutting force Feed force Radial force Thrust force c F f F r F D F •No motion on the radial No work done by radial motion • The feed force is negligible •Power(P) needed for turning is : 60 c cV F P    Watt 21 Cutting force
  • 22. Specific cutting Energy 10/24/2023 The rate of energy consumption during machining is m P V F P c m  The energy consumed per unit volume of metal removed, specific cutting energy is s P c c w m s A F Z P P   m P c F s P w Z Power consumed Cutting force Specific cutting energy Metal removal rate Un deformed chip cross section c A 22 Cutting force
  • 25. Forces on Shaping 10/24/2023 Cutting force 25   sin cos T n T f F F F F   T c F F cutting component acts against v Thrust component perpendicular to transient surface n f F F Feed component Normal component
  • 26. Forces in Drilling 10/24/2023 Cutting force 26 2 / f f Feed per revolution Feed per cutting edge   sin ) 2 / ( sin ) 2 / ( 1 D w f t              sin tan ) / 2 ( tan 1 D r   r Radius of the point on the cutting rake angle Helix angle  2  2
  • 27. Force on drilling cont’d… 10/24/2023 Cutting force 27 Development of torque and thrust during drilling friction ch T F F F F     sin 2 ch F F Total Thrust force Force on chisel edge friction ch c M M z F M    ch M M Total Moment Moment due to chisel edge 80%M 8%M 12%M  sin 5 6 . 0 T c F F D F M   
  • 28. Forces on Milling 10/24/2023 Cutting force 28 D d Nn V t c f c 2 max  D d Nn V t c f ave  ave c t t max Max. uncut chip thickness Average chip thickness t f c t d  2 D 
  • 29. Forces on milling cont’d… 10/24/2023 Cutting force 29 Thrust force doesn't cause any torque The total torque is caused by the cutting force Components of milling force C F T F ) 2 / ( _ _ d F M c tooth cutting one  d Diameter of the cutter Arbor rotation and torque  Variation of torque due to single cutting 
  • 30. Forces on milling cont’d… 10/24/2023 Cutting force 30 Z   2  ) i Z   2  ) ii Z   2  ) iii Type of tooth Nature of torque      
  • 31. Power consumed by machine tool 10/24/2023 Cutting force 31 m m e P P   m e m P P  Power consumed Electric Power consumed by machine tool spindle rotor Machine tool transmission efficiency 4 . 0   t P P o s t P Ps 0 Specific cutting energy A constant in (J/mm3) depends on tool material Uncut chip thickness in mm