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Introduction to force
equilibrium method
A presentation by Mayank Mishra on Mechanics of forming process
 Types of Forming process and its mechanism
 Rolling
 Forging
 Drawing
 Deep drawing
 Bending
 Extrusion
οƒ˜Why we want to find and analyse forces applied
β€’ A definite geometry can be produced
β€’ Extent of Change in properties of material can be found
β€’ It will make process economical as we are not going to apply more
than required force
Rolling
Mechanics of rolling operations
Here our goal is to find out
 The roll separating force
 Torque and power required to drive the belt
 Power losses in bearings
 For calculations of all these factors we make few assumptions
οƒ˜ The rolls are straight and rigid cylinder
οƒ˜ The width of strip is much larger then its thickness and no significant
widening takes place
οƒ˜ Coefficient of friction is low and constant
οƒ˜ Yield stress of material remains constant
𝑝
2π‘˜
=
2𝑦
𝑑
1 βˆ’
𝜎
2π‘˜
β…‡^Β΅(πœ†π‘— βˆ’ πœ†)
𝑝
2π‘˜
=
2𝑦
𝑑
1 βˆ’
𝜎
2π‘˜
β…‡^(Β΅πœ†)
Roll separating force
Drive torque and power
Forging
 Forging assumptions
 Forging F attains its maximum value at the end of operation
 Coefficient of friction remains constant
 Thickness of workpiece is small as compared to other dimensions
 The entire workpiece is in plastic state during the process
Total forging force per unit length of workpiece
𝐹 = 2
0
π‘₯
𝑝1 𝑑π‘₯ +
π‘₯
𝑙
𝑃2 𝑑π‘₯
 Forging of rectangular billet
Forging of disk
Drawing
Assumptions
 The coefficient of friction πœ‡ and half angle 𝛼 are same
 The yield stress 𝜎 𝑦 is constant
 βˆ’π‘ & 𝜎 π‘₯ are the principal stress
 𝜎 π‘₯ doesn’t vary in radial direction
𝐷 = 1 βˆ’ (𝑑𝑖/𝑑 𝑓)2
∈= log 1 βˆ’ 𝑑 βˆ’1
 Drawing of a cylindrical
rod
 Determination of drawing force and power
𝐹 = 𝜎 π‘₯𝑓 𝐴 𝑓
𝑃 = 𝐹𝑉
Deep drawing
Objective of our analysis
 To correlate the initial and final dimension of job
 To estimate the drawing force F
𝐹 = πœŽπ‘§2πœ‹π‘Ÿπ‘ 𝑑
πœŽπ‘Ÿ
2π‘˜
=
πœ‡πΉβ„Ž
2πœ‹π‘‘πΎπ‘Ÿπ‘—
+ log
π‘Ÿπ‘—
π‘Ÿ
At r=π‘Ÿπ‘‘
πœŽπ‘Ÿ
2π‘˜
=
πœ‡πΉβ„Ž
2πœ‹π‘‘πΎπ‘Ÿπ‘—
+ log
π‘Ÿπ‘—
π‘Ÿπ‘‘
Bending
In bending operations apart from determination of work load, an estimated
amount of elastic recovery is there So when final shape is prescribed a suitable
amount of overbending is required to take care of this spring back
 Details in bending
𝐹 π‘šπ‘Žπ‘₯ =
𝑀
𝐿
1 + cos tanβˆ’1 πœ‡ + πœ‡ sin tanβˆ’1 πœ‡
Extrusion
It is similar to drawing but here along with tensile
load at exit end a compressive load is also applied at
inlet
 Determination of work load from stress analysis
Frictional load during
extrusion
𝐹 =
πœ‹
4
𝑑𝑖
2
𝜎π‘₯𝐡𝐡 +
𝑑𝑖
3
𝑑𝑖 π‘™πœŽ 𝑦

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Introduction to force equilibrium method

  • 1. Introduction to force equilibrium method A presentation by Mayank Mishra on Mechanics of forming process
  • 2.  Types of Forming process and its mechanism  Rolling  Forging  Drawing  Deep drawing  Bending  Extrusion οƒ˜Why we want to find and analyse forces applied β€’ A definite geometry can be produced β€’ Extent of Change in properties of material can be found β€’ It will make process economical as we are not going to apply more than required force
  • 4. Mechanics of rolling operations Here our goal is to find out  The roll separating force  Torque and power required to drive the belt  Power losses in bearings  For calculations of all these factors we make few assumptions οƒ˜ The rolls are straight and rigid cylinder οƒ˜ The width of strip is much larger then its thickness and no significant widening takes place οƒ˜ Coefficient of friction is low and constant οƒ˜ Yield stress of material remains constant
  • 5.
  • 6. 𝑝 2π‘˜ = 2𝑦 𝑑 1 βˆ’ 𝜎 2π‘˜ β…‡^Β΅(πœ†π‘— βˆ’ πœ†) 𝑝 2π‘˜ = 2𝑦 𝑑 1 βˆ’ 𝜎 2π‘˜ β…‡^(Β΅πœ†)
  • 7.
  • 8. Roll separating force Drive torque and power
  • 9. Forging  Forging assumptions  Forging F attains its maximum value at the end of operation  Coefficient of friction remains constant  Thickness of workpiece is small as compared to other dimensions  The entire workpiece is in plastic state during the process
  • 10. Total forging force per unit length of workpiece 𝐹 = 2 0 π‘₯ 𝑝1 𝑑π‘₯ + π‘₯ 𝑙 𝑃2 𝑑π‘₯  Forging of rectangular billet
  • 12. Drawing Assumptions  The coefficient of friction πœ‡ and half angle 𝛼 are same  The yield stress 𝜎 𝑦 is constant  βˆ’π‘ & 𝜎 π‘₯ are the principal stress  𝜎 π‘₯ doesn’t vary in radial direction
  • 13. 𝐷 = 1 βˆ’ (𝑑𝑖/𝑑 𝑓)2 ∈= log 1 βˆ’ 𝑑 βˆ’1  Drawing of a cylindrical rod  Determination of drawing force and power 𝐹 = 𝜎 π‘₯𝑓 𝐴 𝑓 𝑃 = 𝐹𝑉
  • 15. Objective of our analysis  To correlate the initial and final dimension of job  To estimate the drawing force F 𝐹 = πœŽπ‘§2πœ‹π‘Ÿπ‘ 𝑑 πœŽπ‘Ÿ 2π‘˜ = πœ‡πΉβ„Ž 2πœ‹π‘‘πΎπ‘Ÿπ‘— + log π‘Ÿπ‘— π‘Ÿ At r=π‘Ÿπ‘‘ πœŽπ‘Ÿ 2π‘˜ = πœ‡πΉβ„Ž 2πœ‹π‘‘πΎπ‘Ÿπ‘— + log π‘Ÿπ‘— π‘Ÿπ‘‘
  • 16. Bending In bending operations apart from determination of work load, an estimated amount of elastic recovery is there So when final shape is prescribed a suitable amount of overbending is required to take care of this spring back
  • 17.  Details in bending 𝐹 π‘šπ‘Žπ‘₯ = 𝑀 𝐿 1 + cos tanβˆ’1 πœ‡ + πœ‡ sin tanβˆ’1 πœ‡
  • 18. Extrusion It is similar to drawing but here along with tensile load at exit end a compressive load is also applied at inlet
  • 19.  Determination of work load from stress analysis Frictional load during extrusion 𝐹 = πœ‹ 4 𝑑𝑖 2 𝜎π‘₯𝐡𝐡 + 𝑑𝑖 3 𝑑𝑖 π‘™πœŽ 𝑦