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NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 11, NOV.-2015
1 | P a g e
ANALYSIS OF CUTTING FORCES OF THE LATHE TOOL
DYNAMOMETER
Sanjeev Sharma
Department of Mechanical Engineering,
Chandigarh Engineering College, Landran, Punjab, India
Rajdeep Singh
Department of Mechanical Engineering,
Chandigarh Engineering College, Landran, Punjab, India
Sandeep Jindal
Department of Mechanical Engineering,
Chandigarh Engineering College, Landran, Punjab, India
ABSTRACT
Current research focused on the assessment of metal machining process parameters and on the
development of adaptive control, shows that machine performance, work-piece and tool
material selections, tool life, quality of machined surfaces, the geometry of cutting tool edges,
and cutting conditions are closely related to the cutting forces. The paper deals with checking
the design of lathe tool dynamometer under the capacity of 500 kg and optimization of their
cutting force measurement. In this, mechanical gauges were replaced by resistance strain
gauges which are being utilized to sense the cutting forces during machining and give the
necessary information of cutting forces in terms of resistances which is the measure of cutting
and feed forces. The data is obtained using technique of force measurement in metal
machining processes. In particular for turning process the results are analyzed, leading to an
appraisal of the current status of the cutting force measurements w.r.t. Feed rate, depth of cut
and feed/revolution.
INTRODUCTION
A dynamometer is a machine used to measure torque and rotational speed (rpm) from which
power produced by an engine, motor, pump or other rotating prime mover can be calculated.
In order to put the analysis of the metal cutting operation on a qualitative basis, certain
observations must be made before, during and after a cut. Design criteria will be discussed
first, followed by a review of several types of force measuring equipments. Hence, it is
essential to study the metal cutting process for economical aspects of the manufacture of the
components. To investigate the performance of cutting, the measurement of cutting forces is
essential. The capacity of lathe tool dynamometer is 500kg, sensitivity is 1 kg, cross
interference of 2%, natural frequency is 800 cps (min.) and size of tool is 0.5 inch. Generally,
there are three requirements that are always in opposition in dynamometer design are
sensitivity (with in ± 1%), rigidity and stiffness. For the purpose of analysis, any
dynamometer can be reduced to a mass supported by a spring because all machine tools
operate with some vibrations and in certain cutting operations. Recorded forces is not
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 11, NOV.-2015
2 | P a g e
influenced by any vibrating motion of the dynamometer, its natural frequency must be large
as compared to the exciting vibrations. In this, mechanical gauges were replaced by resistance
strain gauges which involve the deflection with a suitable calibration between the force and
the deflection it produces, are being utilized to sense the cutting forces during machining.
This gives the necessary information of cutting forces in terms of resistances which is the
measure of cutting and feed forces.
DYNAMIC FORCE MEASUREMENT
Tool dynamometers have some additional difficulties since these generally measure
orthogonal forces by using electrical dynamometer which involve the use of transducers. The
changes in electrical signals are indirectly produced by the tool forces by causing strain or
displacement. Also, electric transducer works on the principle of Wheatstone Bridge Circuit.
It is evident that in order to measure the strains of the order of 1 in/in., the strain gauge lathe
dynamometer is used. It is frequently convenient to reduce the lathe operation to a two-
dimensional process. While any two force components may be measured, the most convenient
are the axial and the tangential components of force will cause a bending moment at some
distance from the cutting edge that will cause a moment on the beam tends to measure the
lathe forces.
METHODOLOGY ADOPTED
The study depends upon methodology opted for the proceeding as it decides the way of
collecting the data, manipulation, processing and finally the display of the results.
1. Measurement of cutting force by using electrical strain gauge is the best technique
available.
2. The machining parameters will be considered during the machining w.r.t. cutting forces
and feed forces by predicting the cutting performance such as depth of cut, feed/rev. and
speed.
3. The natural frequency of the tool holder of lathe tool dynamometer will be calculated.
4. Stress calculation will be carried out for the safe design of lathe tool dynamometer.
PRODUCT SUMMARY AND OBSERVATIONS AT DIFFERENT
DEPTH OF CUT
Cutting force have been measured by using the lathe tool dynamometer (Integral damping by
heavy cast iron body) which suit to a wide range of lathes and easily fixed to lathe cross-slide.
By the application of cutting tool theory, the effect of various parameters such as cutting
speeds, feed and cutting forces on the action of cutting tool by varying the depth of cut has
been observed in Table 1. The values of forces exerted on the machine components which
affect the geometrical accuracy of work pieces.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 11, NOV.-2015
3 | P a g e
Table 1 Cutting Speed and Forces at Different Depth of Cut
Depth
of cut,
a (mm)
Feed per
revolution
(mm)
Dia., d
(mm)
Cutting
speed
V = пDn
(m/sec)
Force
Speed
(rpm)
Cutting
Forces
Fz(kg)
Feed
Force
Fx (kg)
F, resultant
22
FxFz +
0.5 0.0781 21.78 23.25 15 3 15.29
340
1.0 0.0781 20.78 22.19 30 7 30.81
2.0 0.0781 18.78 18.78 52 20 55.71
2.5 0.0781 14.78 14.78 58 24 62.76
0.5 0.046 23.04 20.25 20 4 20.39
2801.0 0.046 22.04 19.38 42 6 42.43
1.5 0.046 18.96 16.67 49 9 49.82
0.5 0.0647 15.90 16.67 15 5 15.8
340
1.0 0.0647 21.04 21.04 32 8 32.98
2.0 0.0647 23.04 24.59 55 22 59.23
FREQUENCY CALCULATION
Natural frequency is calculated as follows: Fig. 1 where, deflection at end AB due to load of
500kg. The general equation for the deflection of the beam is:
dx×=
EI
Mm
δ
For square cross-section, 4
4
2 cm
12
d
I =
For round cross-section, I1=
64
d4
Π
K =
δ
F ; Wn= g
m
k
×
Where
M= Moment; m= Effective mass
K= Spring Stiffness constant; F= Force; δ = Deflection
V = Cutting speed = пDn (m/sec)
F, resultant = 22
FxFz +
Fx and Fz is noted from the dynamometer indicating units
Figure 1: Line Diagram of Tool Holders
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 11, NOV.-2015
4 | P a g e
Figure 2: Shear Force & Bending Moment Diagram
Shear force and bending moment are calculated by referring the Fig. 2.
∫ ∫ ∫+==
1
2
1
0 21
l
l
l
xdx
EI
M
dx
EI
Mx
dx
EI
Mm
δ
2
2
1
1
1
12
10
2
2 1
22
1
2
2
1
1
EI
ex
w
e
xlwPxxdx
EI
xw
xPx
l
l
l
⋅













 −
+





−++×






+⋅= ∫∫
( )
∫∫





 −
+





−++×





+=
2
1
1 2
22
1
2
2
1
1
1
12
2
10
2
2
l
l
l
lx
xw
l
xxlwPxdx
EI
x
wPx
{ }





−++








−++





+=
∫
∫ ∫∫∫
2
1
2
1
2
1
11
)2(
2
1
2
1
2
1
1
2
1
21
2
2
1
2
2
12
2
2
0
32
0
2
1
l
l
l
l
l
l
ll
dxxllxx
w
EI
lw
dxxlwdxPx
EI
dxx
w
dsPx
EI














−














+





+














+=
223
1
83
1 22
12
3
12
2
1
3
20
4
21
1
2
1
1
3
xlwx
lw
x
Px
EI
xwPl
EI
l
l
l
l
l
( ) ( ) 











+−+−+−+





+=
2
)(
4
1
33
1
83
1 4
1
4
21
3
1
3
2
123
1
3
2
2
4
1
2
3
1
1
l
llwll
lw
ll
P
EI
l
w
Pl
EI
….....(i)
Where,
Density of steel = 7.87gm/cc and Density of stainless steel = 7.93gm/cc
L1=8cm; L2=10.3cm; W1=155.6gm/cm and W2=64.4gm/cm
W1 & W2 are self weight of two sections.
I1= п ×
64
54
=30.6cm4
and I2 =
12
2.854 = 5.49cm4
Substituting these values in (i), we get
δ = 0.001394 + 0.008756 = 0.01015cm
K =
δ
f
=
0.0102
500 = 4.902 ×104 kg/cm
m, effective =
10001000
2211 LWLW ×
+
× = 1.245 + 0.148 =1.393kg
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 11, NOV.-2015
5 | P a g e
Wn=
∏
×
2
1
m
k
Fn=
393.1
981
1049.4
2
1
×××
Π
= 934.6cps
DESIGN STRESS CALCULATION
Stress has to be calculated by analyzing the dimensions as follows: Fig. 3.
Therefore L = 8 + 1.4 + 1.8 =11.225cm
E = 2.1×106
kg/cm2
σ =
z
m = Fc ×
z
L = 500 ×
3.858
11.225 =1455 kg/cm2
Figure 3: Dynamometer Tool
Stress has been calculated on capacity basis, now force is calculation on the basis of allowable
stress for steel. Under repeated loading, the stress, σ = 1840 kg/cm2
(after taking factor of
safety)
Using, σ = Fc ×
z
L
Cutting Force, Fc = 500 Kg
Therefore at allowable stress, the cutting force
Fc= 3.858 ×
11.225
1840 = 632.40 Kg
But cutting forces analysis is to be carried out for the design of 500kg. Therefore at stress,
1455 kg/cm2
, the cutting force
Fc= 3.858 ×
11.225
1455 = 500 Kg
So, our design is safe for above said forces.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 11, NOV.-2015
6 | P a g e
RESULTS AND DISCUSSION
As per observation recorded, the feed forces and depth of cut is directly proportional to
cutting forces. All the analysis is shown in the graphs which shows that on increasing the
depth of cut leads to increase in cutting & feed force i.e. approximately linear. Also, cutting
forces depend upon feed rate of tool so the cutting forces increase as feed rate increases.
Cutting forces is also decreases as feed/rev. increases. Moreover frequency & stress produce
in tool of dynamometer within given criteria of safe design. These have been as follows: Fig.
4, 5 and 6.
The similarity of the records obtained from the dynamic testing of two-component strain
gauge dynamometer indicated good repeatability of measurements. However, the results
shows that relatively high variation in the accuracy of horizontal and vertical force
components developed due to large effect of cross sensitivity, zero drift, and variations in
voltage supply and temperatures. Another difficulty was that differences caused by changes of
the sensitivity among the measuring bridges by changing the balance points of the circuits. In
practice, the measuring bridges were not stable and caused a number of problems.
Figure 4: Feed Per Revolution vs Cutting forces
Figure 5: Depth cut of vs cutting force
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 11, NOV.-2015
7 | P a g e
Figure 6: Depth of Cut vs Feed force
CONCLUSIONS
The cutting forces are measured by using electrical strain gauge is the best technique
available. As per cutting analysis of forces, it has concluded that the cutting & feed forces is
directly proportional to depth of cut & feed rate of tool and inversely proportional to feed/rev.
Natural frequency & stress produced in tool of dynamometer has been formulated to give the
permissible limits of the safe designs. So the design is safe within given parameters, for which
the instrument is made.
REFERENCES
1. Byrne G., Dornfled D., Inasaki I., Ketteler Konig G. W. and Teti R. (1995), “Tool
condition monitoring (TCM)—the statue of research and industrial application,” Ann.
CIRP, Vol. 44, No. 2, pp. 541–567.
2. Brett J.F., Warren T.M., Behr S.M. and Whirl Bit (1990), “A new theory of PDC bit
failure, SPE Drilling Erg”, Vol. 5, pp. 275-281.
3. Evans J.C. and Morgan I.G. (1964), “The Pneumatic Gauging Technique in its
Application to Dimensional Measurement”, Int. J. of Manufacturing Sc., Vol. 31, No.
3, pp. 979-985.
4. Field J.S. (1967), “A compact dynamometer using strain gauge principles”, The
International Journal of Production Research, Notes on Applied Science No.34,
H.M.S.O, London, 6(2):75-82.
NOVATEUR PUBLICATIONS
INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT]
ISSN: 2394-3696
VOLUME 2, ISSUE 11, NOV.-2015
8 | P a g e
5. Gautschi G.H., Gibson A. and Kobler H. (1971), “Cutting Forces in Machining
Design and Research Conference, Elimination of interactions in dynamometer
instrumentation Manchester”, The International Journal of Production Research, p.1-
8. 6(2):83-86.
6. Li D. and Mathew J. (1990), “Tool wear and failure monitoring techniques for
turning—a review”, Int. J. Mach. Tools and Manu fact, Vol. 30, no. 4, pp. 579–598.
7. Murty S.S.N. (1977), “A study on the precision of metal cutting dynamometers.
Microtecnic”, ASME, 4: 37-40.
8. Ohtani T. (1986), “Cutting force characteristics in machining of hardened steel. Bul”,
Japan Soc. of Prec. Eng., (2):127-129.
9. Stein J. L. and Huh K. (2006), “A design procedure for model-based monitoring
systems: cutting force estimation as a case study, in Control of Manufacturing
Processes”, ASME, pp. 45–57.
10. Stein J. L. and Huh K. (1991) “A design procedure for model-based monitoring
systems: cutting force estimation as a case study, in Control of Manufacturing
Processes”, ASME, pp. 45–57.
11. Tlusty J. and Andrews G. C. (1983), “A critical review of sensors for unmanned
machining” , Ann. CIRP, Vol. 32, No. 2, pp. 611–622.
12. Warren T.M., Brett J.F. and Sinor LA. (1990) “Development of a whirl-resistant bit,
SPE Ddhg Engg.”, J. Manufact. Syst., Vol. 5, pp. 267-274.

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ANALYSIS OF CUTTING FORCES OF THE LATHE TOOL DYNAMOMETER

  • 1. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 11, NOV.-2015 1 | P a g e ANALYSIS OF CUTTING FORCES OF THE LATHE TOOL DYNAMOMETER Sanjeev Sharma Department of Mechanical Engineering, Chandigarh Engineering College, Landran, Punjab, India Rajdeep Singh Department of Mechanical Engineering, Chandigarh Engineering College, Landran, Punjab, India Sandeep Jindal Department of Mechanical Engineering, Chandigarh Engineering College, Landran, Punjab, India ABSTRACT Current research focused on the assessment of metal machining process parameters and on the development of adaptive control, shows that machine performance, work-piece and tool material selections, tool life, quality of machined surfaces, the geometry of cutting tool edges, and cutting conditions are closely related to the cutting forces. The paper deals with checking the design of lathe tool dynamometer under the capacity of 500 kg and optimization of their cutting force measurement. In this, mechanical gauges were replaced by resistance strain gauges which are being utilized to sense the cutting forces during machining and give the necessary information of cutting forces in terms of resistances which is the measure of cutting and feed forces. The data is obtained using technique of force measurement in metal machining processes. In particular for turning process the results are analyzed, leading to an appraisal of the current status of the cutting force measurements w.r.t. Feed rate, depth of cut and feed/revolution. INTRODUCTION A dynamometer is a machine used to measure torque and rotational speed (rpm) from which power produced by an engine, motor, pump or other rotating prime mover can be calculated. In order to put the analysis of the metal cutting operation on a qualitative basis, certain observations must be made before, during and after a cut. Design criteria will be discussed first, followed by a review of several types of force measuring equipments. Hence, it is essential to study the metal cutting process for economical aspects of the manufacture of the components. To investigate the performance of cutting, the measurement of cutting forces is essential. The capacity of lathe tool dynamometer is 500kg, sensitivity is 1 kg, cross interference of 2%, natural frequency is 800 cps (min.) and size of tool is 0.5 inch. Generally, there are three requirements that are always in opposition in dynamometer design are sensitivity (with in ± 1%), rigidity and stiffness. For the purpose of analysis, any dynamometer can be reduced to a mass supported by a spring because all machine tools operate with some vibrations and in certain cutting operations. Recorded forces is not
  • 2. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 11, NOV.-2015 2 | P a g e influenced by any vibrating motion of the dynamometer, its natural frequency must be large as compared to the exciting vibrations. In this, mechanical gauges were replaced by resistance strain gauges which involve the deflection with a suitable calibration between the force and the deflection it produces, are being utilized to sense the cutting forces during machining. This gives the necessary information of cutting forces in terms of resistances which is the measure of cutting and feed forces. DYNAMIC FORCE MEASUREMENT Tool dynamometers have some additional difficulties since these generally measure orthogonal forces by using electrical dynamometer which involve the use of transducers. The changes in electrical signals are indirectly produced by the tool forces by causing strain or displacement. Also, electric transducer works on the principle of Wheatstone Bridge Circuit. It is evident that in order to measure the strains of the order of 1 in/in., the strain gauge lathe dynamometer is used. It is frequently convenient to reduce the lathe operation to a two- dimensional process. While any two force components may be measured, the most convenient are the axial and the tangential components of force will cause a bending moment at some distance from the cutting edge that will cause a moment on the beam tends to measure the lathe forces. METHODOLOGY ADOPTED The study depends upon methodology opted for the proceeding as it decides the way of collecting the data, manipulation, processing and finally the display of the results. 1. Measurement of cutting force by using electrical strain gauge is the best technique available. 2. The machining parameters will be considered during the machining w.r.t. cutting forces and feed forces by predicting the cutting performance such as depth of cut, feed/rev. and speed. 3. The natural frequency of the tool holder of lathe tool dynamometer will be calculated. 4. Stress calculation will be carried out for the safe design of lathe tool dynamometer. PRODUCT SUMMARY AND OBSERVATIONS AT DIFFERENT DEPTH OF CUT Cutting force have been measured by using the lathe tool dynamometer (Integral damping by heavy cast iron body) which suit to a wide range of lathes and easily fixed to lathe cross-slide. By the application of cutting tool theory, the effect of various parameters such as cutting speeds, feed and cutting forces on the action of cutting tool by varying the depth of cut has been observed in Table 1. The values of forces exerted on the machine components which affect the geometrical accuracy of work pieces.
  • 3. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 11, NOV.-2015 3 | P a g e Table 1 Cutting Speed and Forces at Different Depth of Cut Depth of cut, a (mm) Feed per revolution (mm) Dia., d (mm) Cutting speed V = пDn (m/sec) Force Speed (rpm) Cutting Forces Fz(kg) Feed Force Fx (kg) F, resultant 22 FxFz + 0.5 0.0781 21.78 23.25 15 3 15.29 340 1.0 0.0781 20.78 22.19 30 7 30.81 2.0 0.0781 18.78 18.78 52 20 55.71 2.5 0.0781 14.78 14.78 58 24 62.76 0.5 0.046 23.04 20.25 20 4 20.39 2801.0 0.046 22.04 19.38 42 6 42.43 1.5 0.046 18.96 16.67 49 9 49.82 0.5 0.0647 15.90 16.67 15 5 15.8 340 1.0 0.0647 21.04 21.04 32 8 32.98 2.0 0.0647 23.04 24.59 55 22 59.23 FREQUENCY CALCULATION Natural frequency is calculated as follows: Fig. 1 where, deflection at end AB due to load of 500kg. The general equation for the deflection of the beam is: dx×= EI Mm δ For square cross-section, 4 4 2 cm 12 d I = For round cross-section, I1= 64 d4 Π K = δ F ; Wn= g m k × Where M= Moment; m= Effective mass K= Spring Stiffness constant; F= Force; δ = Deflection V = Cutting speed = пDn (m/sec) F, resultant = 22 FxFz + Fx and Fz is noted from the dynamometer indicating units Figure 1: Line Diagram of Tool Holders
  • 4. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 11, NOV.-2015 4 | P a g e Figure 2: Shear Force & Bending Moment Diagram Shear force and bending moment are calculated by referring the Fig. 2. ∫ ∫ ∫+== 1 2 1 0 21 l l l xdx EI M dx EI Mx dx EI Mm δ 2 2 1 1 1 12 10 2 2 1 22 1 2 2 1 1 EI ex w e xlwPxxdx EI xw xPx l l l ⋅               − +      −++×       +⋅= ∫∫ ( ) ∫∫       − +      −++×      += 2 1 1 2 22 1 2 2 1 1 1 12 2 10 2 2 l l l lx xw l xxlwPxdx EI x wPx { }      −++         −++      += ∫ ∫ ∫∫∫ 2 1 2 1 2 1 11 )2( 2 1 2 1 2 1 1 2 1 21 2 2 1 2 2 12 2 2 0 32 0 2 1 l l l l l l ll dxxllxx w EI lw dxxlwdxPx EI dxx w dsPx EI               −               +      +               += 223 1 83 1 22 12 3 12 2 1 3 20 4 21 1 2 1 1 3 xlwx lw x Px EI xwPl EI l l l l l ( ) ( )             +−+−+−+      += 2 )( 4 1 33 1 83 1 4 1 4 21 3 1 3 2 123 1 3 2 2 4 1 2 3 1 1 l llwll lw ll P EI l w Pl EI ….....(i) Where, Density of steel = 7.87gm/cc and Density of stainless steel = 7.93gm/cc L1=8cm; L2=10.3cm; W1=155.6gm/cm and W2=64.4gm/cm W1 & W2 are self weight of two sections. I1= п × 64 54 =30.6cm4 and I2 = 12 2.854 = 5.49cm4 Substituting these values in (i), we get δ = 0.001394 + 0.008756 = 0.01015cm K = δ f = 0.0102 500 = 4.902 ×104 kg/cm m, effective = 10001000 2211 LWLW × + × = 1.245 + 0.148 =1.393kg
  • 5. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 11, NOV.-2015 5 | P a g e Wn= ∏ × 2 1 m k Fn= 393.1 981 1049.4 2 1 ××× Π = 934.6cps DESIGN STRESS CALCULATION Stress has to be calculated by analyzing the dimensions as follows: Fig. 3. Therefore L = 8 + 1.4 + 1.8 =11.225cm E = 2.1×106 kg/cm2 σ = z m = Fc × z L = 500 × 3.858 11.225 =1455 kg/cm2 Figure 3: Dynamometer Tool Stress has been calculated on capacity basis, now force is calculation on the basis of allowable stress for steel. Under repeated loading, the stress, σ = 1840 kg/cm2 (after taking factor of safety) Using, σ = Fc × z L Cutting Force, Fc = 500 Kg Therefore at allowable stress, the cutting force Fc= 3.858 × 11.225 1840 = 632.40 Kg But cutting forces analysis is to be carried out for the design of 500kg. Therefore at stress, 1455 kg/cm2 , the cutting force Fc= 3.858 × 11.225 1455 = 500 Kg So, our design is safe for above said forces.
  • 6. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 11, NOV.-2015 6 | P a g e RESULTS AND DISCUSSION As per observation recorded, the feed forces and depth of cut is directly proportional to cutting forces. All the analysis is shown in the graphs which shows that on increasing the depth of cut leads to increase in cutting & feed force i.e. approximately linear. Also, cutting forces depend upon feed rate of tool so the cutting forces increase as feed rate increases. Cutting forces is also decreases as feed/rev. increases. Moreover frequency & stress produce in tool of dynamometer within given criteria of safe design. These have been as follows: Fig. 4, 5 and 6. The similarity of the records obtained from the dynamic testing of two-component strain gauge dynamometer indicated good repeatability of measurements. However, the results shows that relatively high variation in the accuracy of horizontal and vertical force components developed due to large effect of cross sensitivity, zero drift, and variations in voltage supply and temperatures. Another difficulty was that differences caused by changes of the sensitivity among the measuring bridges by changing the balance points of the circuits. In practice, the measuring bridges were not stable and caused a number of problems. Figure 4: Feed Per Revolution vs Cutting forces Figure 5: Depth cut of vs cutting force
  • 7. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 11, NOV.-2015 7 | P a g e Figure 6: Depth of Cut vs Feed force CONCLUSIONS The cutting forces are measured by using electrical strain gauge is the best technique available. As per cutting analysis of forces, it has concluded that the cutting & feed forces is directly proportional to depth of cut & feed rate of tool and inversely proportional to feed/rev. Natural frequency & stress produced in tool of dynamometer has been formulated to give the permissible limits of the safe designs. So the design is safe within given parameters, for which the instrument is made. REFERENCES 1. Byrne G., Dornfled D., Inasaki I., Ketteler Konig G. W. and Teti R. (1995), “Tool condition monitoring (TCM)—the statue of research and industrial application,” Ann. CIRP, Vol. 44, No. 2, pp. 541–567. 2. Brett J.F., Warren T.M., Behr S.M. and Whirl Bit (1990), “A new theory of PDC bit failure, SPE Drilling Erg”, Vol. 5, pp. 275-281. 3. Evans J.C. and Morgan I.G. (1964), “The Pneumatic Gauging Technique in its Application to Dimensional Measurement”, Int. J. of Manufacturing Sc., Vol. 31, No. 3, pp. 979-985. 4. Field J.S. (1967), “A compact dynamometer using strain gauge principles”, The International Journal of Production Research, Notes on Applied Science No.34, H.M.S.O, London, 6(2):75-82.
  • 8. NOVATEUR PUBLICATIONS INTERNATIONAL JOURNAL OF INNOVATIONS IN ENGINEERING RESEARCH AND TECHNOLOGY [IJIERT] ISSN: 2394-3696 VOLUME 2, ISSUE 11, NOV.-2015 8 | P a g e 5. Gautschi G.H., Gibson A. and Kobler H. (1971), “Cutting Forces in Machining Design and Research Conference, Elimination of interactions in dynamometer instrumentation Manchester”, The International Journal of Production Research, p.1- 8. 6(2):83-86. 6. Li D. and Mathew J. (1990), “Tool wear and failure monitoring techniques for turning—a review”, Int. J. Mach. Tools and Manu fact, Vol. 30, no. 4, pp. 579–598. 7. Murty S.S.N. (1977), “A study on the precision of metal cutting dynamometers. Microtecnic”, ASME, 4: 37-40. 8. Ohtani T. (1986), “Cutting force characteristics in machining of hardened steel. Bul”, Japan Soc. of Prec. Eng., (2):127-129. 9. Stein J. L. and Huh K. (2006), “A design procedure for model-based monitoring systems: cutting force estimation as a case study, in Control of Manufacturing Processes”, ASME, pp. 45–57. 10. Stein J. L. and Huh K. (1991) “A design procedure for model-based monitoring systems: cutting force estimation as a case study, in Control of Manufacturing Processes”, ASME, pp. 45–57. 11. Tlusty J. and Andrews G. C. (1983), “A critical review of sensors for unmanned machining” , Ann. CIRP, Vol. 32, No. 2, pp. 611–622. 12. Warren T.M., Brett J.F. and Sinor LA. (1990) “Development of a whirl-resistant bit, SPE Ddhg Engg.”, J. Manufact. Syst., Vol. 5, pp. 267-274.