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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1880
Estimating Crushing Force of Cone Crusher using Analytical Method
Prashant P. Deshpande1, Prof. Dr. K. K. Dhande2
1PG student Dr. D. Y. Patil Institute of Technology, Pimpri Pune-18, India
2Head of Mechanical Dept. Prof. Dr. D. Y. Patil Institute of Technology, Pimpri Pune-18, India
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract - Cone crushers are widely used in Aggregate and
Mineral processing industries as Secondary or Tertiary stage
crusher to crush blasted rock material. In this work to
calculate the output from a cone crusher, models for size
reduction and flow are needed. The interaction between these
two models & quite complex as the overall size reduction in a
cone crusher is a result ofarepeatedconsecutivecomminution
process. The flow model & important sinceit describeshow the
rock material moves through the crusher chamber. Thereby
the flow model provides input to the size reduction model. In
turn, the size reduction model predicts the size distribution
after compressing the rock material. In this work a simplified
methodology for estimating crushing force of cone crusher is
presented.
Key Words: (Cone Crusher, Crushing chamber, crushing
force, analytical method
1. INTRODUCTION
The objective of crushing in any industry is to liberate
valuable minerals from crushed material or to produce
aggregate which is used as construction materials. Cone
crushers is commonly used in aggregate producing and
mineral processing industries. Crushing chamber is
considered as heart of cone crusher as it decides the
performance of crusher by affecting capacity, product size
and product shape.
Cone crusher is the main material crushing to a certain
degree of particles and plays a key role in the corresponding
production process. For optimizing the sizing of cone
crusher components it is firststepto evaluatecrushingforce.
The aim of this paper is to look inside the crushing chamber
and examines the crushing force which is the important
parameter based on which sizing of cone crusher
components needs to be decided.
1.1 CONE CRUSHER BASICS
A. Construction
In cone crusher components Concave & Mantel forms the
crushing chamber geometry. The Core and Mantel is shrink
fitted on shaft. Shaft is pivoted in bush bearing which gyrates
at constant speed with Mantel as shown in Fig. 1. The
nutational motion is achieved using eccentric sleeves which
turns main shaft using V-belt drive thru gear mechanism.
B. Working
In a cone crusher the rock material is crushed between rigid
surfaces. The motion of the movingsurfaceisindependentof
the loading of the crusher. Therefore, the explored
comminution principle is form conditioned compressive
crushing.
Particles are nipped, compressed and crushed between
mantle and concave. Breakage of particles can bebothsingle
particle (particles are broken betweenconeandmantle) and
inter particle (between other particles). The mantle and the
concave must be replaced regularly as theyarecontinuously
subjected to wear.
Crushing takes place continuously and is inter-particle to a
great extent. Inter-particle crushing is achieved when a
particle is stressed and broken between other particles.
Inter-particle breakage is desirable from the pointofviewof
wear and service life. Inter-particle breakage is also
considered to give the best shape of the produced particles.
To achieve inter-particle breakage choke fed conditions are
normally recommended. Choke fedconditionsimplythatthe
inlet of the crusher is covered with feed material. The feed
material is then fed into the crusher by the influence of
gravity.
Fig -1: Basic principle of cone crusher working
The basic operating principle of a cone crusher is shown in
Figure 1 The properties, i.e. size distribution and quality
parameters, of the product leaving the crusherarea result of
the interaction between crusher and rock material. In turn,
the interaction is dependent on chamber geometry, crusher
dynamics and rock material characteristics.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1881
Concave, mantle, eccentricity and location of the pivot point
together form the chamber geometry of the cone crusher.
Like a crank, the eccentricity turns the main shaft with
constant speed. At the top the main shaft is journal led in a
pivot point. For some designs, the pivot point is just virtual.
The mantle is fixed to the main shaft and the concave to the
crusher frame. The resulting motion of the mantle and main
shaft will be a nutating motion.
Fig -2: Free body force diagram cone crusher
If a vertical cross-section of the crusher is considered, the
mantle will move cyclically forwards and backwards
relatively to the fixed concave. During the squeezing motion
the intervening rock material will be subjected to a
compressive stress field and thereby comminuted. During
the releasing motion the material is able to flow down
through the chamber. The motion is driven by the influence
of gravity and is governed by the motion of the mantel.
At a fixed point of location somewhere in the crusher
chamber, the distance betweenmantleandconcave will vary
between open and closed position, as shown in Figure2.The
motion can be described with a cyclic function of the
eccentric angle. The eccentric angle corresponds to the
position of the eccentricity and therefore also totheposition
of the main shaft.
Schematic representation of Cone crusher & forcesacting on
it
2. CRUSHING FORCE ESTIMATION ANALYTICAL
METHOD
Under normal working state, the size of the force of cone
crusher are influenced by the physical and chemical
properties such as ore, hardness, mechanical properties,
breaking method and ore crushing cavity in the distribution
and so on many factors. If using a theoretical formula to
calculate the crushing force is a difficult, so using by crusher
work normally when the hydraulic cylinder pressure to
calculate crushing force. Crushing force calculation formula
as shown in formula 1.
All parameters of the cone crusher are shown in table 1.To
break into the various parametersintable1generationforce
calculation formula, to calculate maximum crushing force of
cone crusher. Due to the crushing force is perpendicular to
the moving cone lining board, we can undertake
decomposition for crushing the biggest force Fc.
Table -1: Input parameters used to construct crushing
chamber
D CSS D1 α P γ
[mm] [mm] [mm] [deg] [bar] [deg]
1300 25 380 56 45 0.98
Fc : The biggest crushing force
D1: The hydraulic cylinder piston diameter = 380 mm
P: Normal Operating pressure = 45 bar
Pu: Pressure during Uncrushable= 55 bar
n: The number of hydraulic cylinder = 1
α : Dynamic cone Angle on the conical bottom(degree)
γ : Precession Angle( degree)
G: The moving cone weight= 29920 N
 ga
GPnD
Fc



cos
..178.0 2
(1)
Cylindrical roller bearing radial force
 aFcFrFrF  90cos.211 (2)
3. RESULTS AND DISCUSSION
During normal operating condition, considering duty
conditions based on industrial trials it is observed that at 45
bar the crusher operates in normal condition for this size.
Accordingly using equations 1 & 2
Crushing force operating Fco1 = 832 kN
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1882
When uncrushable item comes in crushing chamber based
on past industrial data it is observed that the pressure rises
upto 55 bar hence the maximum crushing force value due to
uncrushable is calculated as
Crushing force Uncrushable Fcu1 = 1028 kN
4. CONCLUSIONS
The crushing force values obtained from simplified
equations are shown using graphical method in fig. 3.
Fig -3: Comparison of crushing force
Percentage of error between two methods is approximate
24%. Is due to difference in pressure when uncrushable
material arrives incrushingchamber.Henceduringdesignof
crusher components it isimportanttoconsiderthecondition
of uncrushable.
ACKNOWLEDGEMENT
The author gratefully acknowledges for the valuable
suggestions and supportreceivedfromMr.Sakhardandeand
Mr. Mondal of R&D department from thyssenkrupp
Industries India, Pimpri Pune.
REFERENCES
[1] Evertsson, C. M., & Bearman, R. A. (1997). Investigation
of inter particle breakage as applied to cone crushing.
Minerals Engineering, 10(2), 199-214.
[2] Evertsson, C. M. (1998). Output prediction of cone
crushers. Minerals engineering, 11(3), 215-231.
[3] Evertsson, C. M. (1999). Modelling of flow in cone
crushers. Minerals engineering, 12(12), 1479-1499.
[4] Gang, D., Dongming, H., & Xiumin, F. (2009). Cone
crusher chamber optimization using multiple
constraints. International Journal ofMineral Processing,
93(2), 204-208.
[5] Zhang, Z., Chen, S., & Yang, Y. (2015, November). Cone
crusher in the cylindrical roller bearingcontactanalysis.
In 5th International ConferenceonCivil Engineeringand
Transportation. Atlantis Press.
[6] Gupta, A., & Yan, D. S. (2016). Mineral processing design
and operations: an introduction. Elsevier.

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IRJET- Estimating Crushing Force of Cone Crusher using Analytical Method

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1880 Estimating Crushing Force of Cone Crusher using Analytical Method Prashant P. Deshpande1, Prof. Dr. K. K. Dhande2 1PG student Dr. D. Y. Patil Institute of Technology, Pimpri Pune-18, India 2Head of Mechanical Dept. Prof. Dr. D. Y. Patil Institute of Technology, Pimpri Pune-18, India ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract - Cone crushers are widely used in Aggregate and Mineral processing industries as Secondary or Tertiary stage crusher to crush blasted rock material. In this work to calculate the output from a cone crusher, models for size reduction and flow are needed. The interaction between these two models & quite complex as the overall size reduction in a cone crusher is a result ofarepeatedconsecutivecomminution process. The flow model & important sinceit describeshow the rock material moves through the crusher chamber. Thereby the flow model provides input to the size reduction model. In turn, the size reduction model predicts the size distribution after compressing the rock material. In this work a simplified methodology for estimating crushing force of cone crusher is presented. Key Words: (Cone Crusher, Crushing chamber, crushing force, analytical method 1. INTRODUCTION The objective of crushing in any industry is to liberate valuable minerals from crushed material or to produce aggregate which is used as construction materials. Cone crushers is commonly used in aggregate producing and mineral processing industries. Crushing chamber is considered as heart of cone crusher as it decides the performance of crusher by affecting capacity, product size and product shape. Cone crusher is the main material crushing to a certain degree of particles and plays a key role in the corresponding production process. For optimizing the sizing of cone crusher components it is firststepto evaluatecrushingforce. The aim of this paper is to look inside the crushing chamber and examines the crushing force which is the important parameter based on which sizing of cone crusher components needs to be decided. 1.1 CONE CRUSHER BASICS A. Construction In cone crusher components Concave & Mantel forms the crushing chamber geometry. The Core and Mantel is shrink fitted on shaft. Shaft is pivoted in bush bearing which gyrates at constant speed with Mantel as shown in Fig. 1. The nutational motion is achieved using eccentric sleeves which turns main shaft using V-belt drive thru gear mechanism. B. Working In a cone crusher the rock material is crushed between rigid surfaces. The motion of the movingsurfaceisindependentof the loading of the crusher. Therefore, the explored comminution principle is form conditioned compressive crushing. Particles are nipped, compressed and crushed between mantle and concave. Breakage of particles can bebothsingle particle (particles are broken betweenconeandmantle) and inter particle (between other particles). The mantle and the concave must be replaced regularly as theyarecontinuously subjected to wear. Crushing takes place continuously and is inter-particle to a great extent. Inter-particle crushing is achieved when a particle is stressed and broken between other particles. Inter-particle breakage is desirable from the pointofviewof wear and service life. Inter-particle breakage is also considered to give the best shape of the produced particles. To achieve inter-particle breakage choke fed conditions are normally recommended. Choke fedconditionsimplythatthe inlet of the crusher is covered with feed material. The feed material is then fed into the crusher by the influence of gravity. Fig -1: Basic principle of cone crusher working The basic operating principle of a cone crusher is shown in Figure 1 The properties, i.e. size distribution and quality parameters, of the product leaving the crusherarea result of the interaction between crusher and rock material. In turn, the interaction is dependent on chamber geometry, crusher dynamics and rock material characteristics.
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1881 Concave, mantle, eccentricity and location of the pivot point together form the chamber geometry of the cone crusher. Like a crank, the eccentricity turns the main shaft with constant speed. At the top the main shaft is journal led in a pivot point. For some designs, the pivot point is just virtual. The mantle is fixed to the main shaft and the concave to the crusher frame. The resulting motion of the mantle and main shaft will be a nutating motion. Fig -2: Free body force diagram cone crusher If a vertical cross-section of the crusher is considered, the mantle will move cyclically forwards and backwards relatively to the fixed concave. During the squeezing motion the intervening rock material will be subjected to a compressive stress field and thereby comminuted. During the releasing motion the material is able to flow down through the chamber. The motion is driven by the influence of gravity and is governed by the motion of the mantel. At a fixed point of location somewhere in the crusher chamber, the distance betweenmantleandconcave will vary between open and closed position, as shown in Figure2.The motion can be described with a cyclic function of the eccentric angle. The eccentric angle corresponds to the position of the eccentricity and therefore also totheposition of the main shaft. Schematic representation of Cone crusher & forcesacting on it 2. CRUSHING FORCE ESTIMATION ANALYTICAL METHOD Under normal working state, the size of the force of cone crusher are influenced by the physical and chemical properties such as ore, hardness, mechanical properties, breaking method and ore crushing cavity in the distribution and so on many factors. If using a theoretical formula to calculate the crushing force is a difficult, so using by crusher work normally when the hydraulic cylinder pressure to calculate crushing force. Crushing force calculation formula as shown in formula 1. All parameters of the cone crusher are shown in table 1.To break into the various parametersintable1generationforce calculation formula, to calculate maximum crushing force of cone crusher. Due to the crushing force is perpendicular to the moving cone lining board, we can undertake decomposition for crushing the biggest force Fc. Table -1: Input parameters used to construct crushing chamber D CSS D1 α P γ [mm] [mm] [mm] [deg] [bar] [deg] 1300 25 380 56 45 0.98 Fc : The biggest crushing force D1: The hydraulic cylinder piston diameter = 380 mm P: Normal Operating pressure = 45 bar Pu: Pressure during Uncrushable= 55 bar n: The number of hydraulic cylinder = 1 α : Dynamic cone Angle on the conical bottom(degree) γ : Precession Angle( degree) G: The moving cone weight= 29920 N  ga GPnD Fc    cos ..178.0 2 (1) Cylindrical roller bearing radial force  aFcFrFrF  90cos.211 (2) 3. RESULTS AND DISCUSSION During normal operating condition, considering duty conditions based on industrial trials it is observed that at 45 bar the crusher operates in normal condition for this size. Accordingly using equations 1 & 2 Crushing force operating Fco1 = 832 kN
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1882 When uncrushable item comes in crushing chamber based on past industrial data it is observed that the pressure rises upto 55 bar hence the maximum crushing force value due to uncrushable is calculated as Crushing force Uncrushable Fcu1 = 1028 kN 4. CONCLUSIONS The crushing force values obtained from simplified equations are shown using graphical method in fig. 3. Fig -3: Comparison of crushing force Percentage of error between two methods is approximate 24%. Is due to difference in pressure when uncrushable material arrives incrushingchamber.Henceduringdesignof crusher components it isimportanttoconsiderthecondition of uncrushable. ACKNOWLEDGEMENT The author gratefully acknowledges for the valuable suggestions and supportreceivedfromMr.Sakhardandeand Mr. Mondal of R&D department from thyssenkrupp Industries India, Pimpri Pune. REFERENCES [1] Evertsson, C. M., & Bearman, R. A. (1997). Investigation of inter particle breakage as applied to cone crushing. Minerals Engineering, 10(2), 199-214. [2] Evertsson, C. M. (1998). Output prediction of cone crushers. Minerals engineering, 11(3), 215-231. [3] Evertsson, C. M. (1999). Modelling of flow in cone crushers. Minerals engineering, 12(12), 1479-1499. [4] Gang, D., Dongming, H., & Xiumin, F. (2009). Cone crusher chamber optimization using multiple constraints. International Journal ofMineral Processing, 93(2), 204-208. [5] Zhang, Z., Chen, S., & Yang, Y. (2015, November). Cone crusher in the cylindrical roller bearingcontactanalysis. In 5th International ConferenceonCivil Engineeringand Transportation. Atlantis Press. [6] Gupta, A., & Yan, D. S. (2016). Mineral processing design and operations: an introduction. Elsevier.