How to calculate rolling pressure?

Rolling pressure is calculated to determine how much force is applied over the contact area during a rolling process. It depends on the rolling force and the area of contact between the rollers and the material, and it helps assess material deformation and equipment performance.


What is Rolling Pressure?

Rolling pressure (p) is the compressive pressure acting between the rolls and the metal strip during rolling.

It depends on:

  • Material strength
  • Amount of thickness reduction
  • Friction between roll and strip
  • Roll diameter

Common Assumptions in Rolling Analysis

To simplify calculations, we assume:

  • Plane strain condition
  • Rolls are rigid
  • Strip width remains constant
  • Homogeneous, isotropic material
  • Coulomb friction law applies
  • No elastic recovery during rolling

These assumptions lead to approximate but useful formulas.


1. Basic idea of rolling pressure

When metal passes between two rotating rolls, it is plastically deformed. To cause this deformation, the rolls must apply a pressure greater than the flow stress of the material.

Because:

  • Pressure is not uniform along the contact length
  • Friction affects deformation

we usually calculate an average rolling pressure.


2. Key parameters involved

  • σf\sigma_fσf​ = flow stress of the material
  • μ\muμ = coefficient of friction
  • RRR = roll radius
  • h1h_1h1​ = initial thickness
  • h2h_2h2​ = final thickness
  • Δh=h1h2\Delta h = h_1 – h_2Δh=h1​−h2​ = draft
  • havg=h1+h22h_{avg} = \frac{h_1 + h_2}{2}havg​=2h1​+h2​​ = average thickness
  • LLL = contact length

3. Contact length in rolling

The contact length between the roll and strip is approximated as:L=RΔh\boxed{L = \sqrt{R\,\Delta h}}L=RΔh​​

This comes from roll geometry and small-angle approximation.


4. Flow stress of the material

For strain-hardening materials, flow stress is commonly calculated using:σf=Kεn\boxed{\sigma_f = K\,\varepsilon^n}σf​=Kεn​

where:

  • KKK = strength coefficient
  • nnn = strain-hardening exponent
  • ε=ln(h1h2)\varepsilon = \ln \left(\frac{h_1}{h_2}\right)ε=ln(h2​h1​​) = true strain

5. Ideal rolling pressure (no friction)

If friction is ignored, the average rolling pressure is approximately:pavg=σf\boxed{p_{avg} = \sigma_f}pavg​=σf​​

This is a simplified assumption.


6. Rolling pressure with friction (practical case)

When friction is included, the average rolling pressure becomes:pavg=σf(1+μLhavg)\boxed{ p_{avg} = \sigma_f \left(1 + \frac{\mu L}{h_{avg}}\right) }pavg​=σf​(1+havg​μL​)​

Interpretation:

  • σf\sigma_fσf​: pressure required for plastic flow
  • μLhavg\frac{\mu L}{h_{avg}}havg​μL​: extra pressure due to friction
  • Higher friction → higher rolling pressure
  • Larger strip thickness → lower friction effect

7. Rolling force calculation

Once the rolling pressure is known, the rolling force is:F=pavg×b×L\boxed{ F = p_{avg} \times b \times L }F=pavg​×b×L​

where:

  • bbb = width of the strip

8. Summary of steps

  1. Calculate draft: Δh=h1h2\Delta h = h_1 – h_2Δh=h1​−h2​
  2. Find contact length: L=RΔhL = \sqrt{R\Delta h}L=RΔh​
  3. Calculate strain: ε=ln(h1/h2)\varepsilon = \ln(h_1/h_2)ε=ln(h1​/h2​)
  4. Find flow stress: σf=Kεn\sigma_f = K\varepsilon^nσf​=Kεn
  5. Compute rolling pressure: pavg=σf(1+μLhavg)p_{avg} = \sigma_f \left(1 + \frac{\mu L}{h_{avg}}\right)pavg​=σf​(1+havg​μL​)
  6. Compute rolling force: F=pavgbLF = p_{avg} b LF=pavg​bL

9. Important assumptions

  • Plane strain condition
  • Uniform deformation
  • Coulomb friction
  • No roll flattening (simplified)

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