Principles of Interference Press Fits and Shrink Fits

An interference fit (commonly called a press fit or shrink fit) is a semi-permanent or permanent mechanical assembly technique where a male cylindrical component (shaft or pin) has an outer diameter intentionally manufactured larger than the mating female bore of a hub, gear, pulley, or bearing ring. When assembled, the negative clearance (interference $\delta$) creates mutual elastic deformation: the shaft contracts radially under compression, while the surrounding hub expands outward under tension.

This elastic strain establishes a severe continuous radial interface contact pressure ($p$) across the mating boundary. Frictional adhesion between the pressurized micro-asperities of the two mating surfaces allows direct transmission of large torsional twisting moments ($T$) and bidirectional axial thrust loads ($F_{\text{axial}}$) without requiring failure-prone keyways, splines, set screws, or fusion welding.

Thick-Walled Cylinder Mechanics: Lamé Elasticity Formulations

To accurately calculate the interface contact pressure, both components are modeled as concentric thick-walled elastic cylinders using Gabriel Lamé's classical 1852 elastostatic boundary value equations.

For a thick-walled cylinder subjected to internal pressure $p_i$ and external pressure $p_o$, radial stress $\sigma_r(r)$ and tangential hoop stress $\sigma_t(r)$ at radius $r$ are:

$$\sigma_r(r) = \frac{p_i r_i^2 - p_o r_o^2}{r_o^2 - r_i^2} - \frac{(p_i - p_o) r_i^2 r_o^2}{r^2 (r_o^2 - r_i^2)}$$ $$\sigma_t(r) = \frac{p_i r_i^2 - p_o r_o^2}{r_o^2 - r_i^2} + \frac{(p_i - p_o) r_i^2 r_o^2}{r^2 (r_o^2 - r_i^2)}$$

Derivation of Contact Pressure ($p$) from Total Interference ($\delta$)

At the mating nominal diameter $d = 2r$, the total diametral interference $\delta = d_{\text{shaft}} - d_{\text{hole}}$ is the absolute sum of the radial dilation of the hub bore ($\Delta d_o$) and the radial contraction of the shaft surface ($\Delta d_i$):

$$\delta = |\Delta d_o| + |\Delta d_i|$$

Applying Hooke's generalized plane stress law ($\varepsilon_t = \frac{\Delta d}{d} = \frac{\sigma_t - \nu \sigma_r}{E}$) to both cylinders yields the master press-fit interference relationship:

$$p = \frac{\delta}{d \left[ \frac{1}{E_o}\left( \frac{d_o^2 + d^2}{d_o^2 - d^2} + \nu_o \right) + \frac{1}{E_i}\left( \frac{d^2 + d_i^2}{d^2 - d_i^2} - \nu_i \right) \right]} \quad [\text{Pascals}]$$

Where:

  • $d$: Nominal mating contact diameter ($\text{m}$).
  • $d_o$: Outer diameter of the exterior hub ($\text{m}$).
  • $d_i$: Internal bore diameter of a hollow shaft ($d_i = 0$ for a solid solid shaft, simplifying the bracketed shaft term to $\frac{1 - \nu_i}{E_i}$).
  • $E_o, E_i$: Young's Modulus of elasticity of the hub and shaft materials ($\text{Pa}$).
  • $\nu_o, \nu_i$: Poisson's ratio of the hub and shaft materials.
  • $\delta$: Total diametral interference ($\text{m}$).

Load Transmission Capacities: Axial Force and Torque

Once contact pressure $p$ is established across engagement length $L$, the assembly's frictional load-holding capacity is governed by Coulomb friction with coefficient $\mu$:

1. Axial Holding Capacity and Insertion Push Force ($F_{\text{axial}}$)

The total normal force acting across the cylindrical surface area $A_{\text{contact}} = \pi \cdot d \cdot L$ is $N_{\text{total}} = p \cdot \pi \cdot d \cdot L$. The maximum axial force the joint can sustain before slipping (and the required hydraulic ram push-on assembly force) is:

$$F_{\text{axial}} = \mu \cdot p \cdot \pi \cdot d \cdot L \quad [\text{Newtons}]$$

2. Torsional Torque Capacity ($T_{\text{max}}$)

Because frictional shear traction acts at radius $r = \frac{d}{2}$, the maximum transmittable torque before angular slippage is:

$$T_{\text{max}} = F_{\text{axial}} \cdot \left( \frac{d}{2} \right) = \frac{1}{2} \mu \cdot p \cdot \pi \cdot d^2 \cdot L \quad [\text{N}\cdot\text{m}]$$

Peak Tangential Hoop Stress and Hub Rupture Safety

The most vulnerable region in any interference assembly is the inner bore surface of the hub ($r = d/2$), where tensile tangential hoop stress reaches its maximum value:

$$\sigma_{t,\text{max}} = p \left( \frac{d_o^2 + d^2}{d_o^2 - d^2} \right) \quad [\text{Tensile}]$$

Combining tensile hoop stress with compressive radial stress ($\sigma_r = -p$), the equivalent von Mises stress at the hub bore is:

$$\sigma_{\text{von Mises}} = \sqrt{\sigma_t^2 - \sigma_t \sigma_r + \sigma_r^2} = \sqrt{\sigma_t^2 + \sigma_t p + p^2}$$

To avoid plastic yielding, cracking, or permanent loosening of the joint, the von Mises stress must satisfy $\sigma_{\text{von Mises}} \le \frac{S_{y,\text{hub}}}{\text{FoS}}$.

Thermal Shrink-Fit Assembly Temperature ($\Delta T$)

Mechanical press fitting at ambient temperature requires massive hydraulic rams and risks destructive surface galling, scoring, and metal transfer. Thermal shrink fitting bypasses mechanical abrasion by thermally expanding the hub or cryogenic shrinking the shaft.

To provide smooth drop-in assembly with a safe assembly diametral clearance (typically $c = 0.02\text{--}0.05\ \text{mm}$), the required temperature differential $\Delta T$ is:

$$\Delta T = \frac{\delta + c}{\alpha_{\text{hub}} \cdot d} \quad [^\circ\text{C}]$$

Where $\alpha_{\text{hub}}$ is the linear thermal expansion coefficient of the hub material (e.g., $12 \times 10^{-6}\ /^\circ\text{C}$ for carbon steel; $23 \times 10^{-6}\ /^\circ\text{C}$ for aluminum).

ISO Fit Class Type of Fit Typical Interference Range Primary Application Field
H7 / p6 Light Press Fit $0.015\text{--}0.035\ \text{mm}$ Locating dowels, small gear hubs, non-slip bushings
H7 / r6 Medium Drive Fit $0.025\text{--}0.055\ \text{mm}$ Couplings, machine tool pulleys, permanent bearing collars
H7 / s6 Heavy Permanent Shrink Fit $0.040\text{--}0.090\ \text{mm}$ Locomotive wheel tires, heavy crane bull gears, turbines
H7 / u6 Extreme Force Fit $0.060\text{--}0.150\ \text{mm}$ Maximum torque assemblies, stress relief heat treatment required

Step-by-Step Engineering Case Study: Heavy Drive Gear on Solid Steel Shaft

Scenario: A steel spur gear hub ($E_o = 207\ \text{GPa}$, $\nu_o = 0.30$, $S_y = 400\ \text{MPa}$) with outer diameter $d_o = 120\ \text{mm}$ and width $L = 75\ \text{mm}$ is shrink-fitted onto a solid steel shaft ($d_i = 0$, $E_i = 207\ \text{GPa}$, $\nu_i = 0.30$) of nominal diameter $d = 60\ \text{mm}$. The total diametral interference is ground to $\delta = 0.050\ \text{mm}$ ($50\ \mu\text{m}$). The interface coefficient of friction is $\mu = 0.15$.

Step 1: Calculate Cylinder Geometric Compliances:

$$\frac{d_o^2 + d^2}{d_o^2 - d^2} = \frac{120^2 + 60^2}{120^2 - 60^2} = \frac{14400 + 3600}{14400 - 3600} = \frac{18000}{10800} = 1.6667$$ $$\text{Term}_{\text{hub}} = \frac{1}{207 \times 10^9} [1.6667 + 0.30] = \frac{1.9667}{207 \times 10^9} = 9.501 \times 10^{-12}\ \text{m}^2/\text{N}$$ $$\text{Term}_{\text{shaft}} = \frac{1}{207 \times 10^9} [1.0 - 0.30] = \frac{0.70}{207 \times 10^9} = 3.382 \times 10^{-12}\ \text{m}^2/\text{N}$$

Step 2: Determine Interface Contact Pressure ($p$):

$$p = \frac{\delta}{d (\text{Term}_{\text{hub}} + \text{Term}_{\text{shaft}})} = \frac{0.000050\ \text{m}}{0.060 \times (9.501 + 3.382) \times 10^{-12}}$$ $$p = \frac{5.0 \times 10^{-5}}{0.060 \times 12.883 \times 10^{-12}} = \frac{5.0 \times 10^{-5}}{7.7298 \times 10^{-13}} = 64.685 \times 10^6\ \text{Pa} = 64.69\ \text{MPa}$$

Step 3: Calculate Transmittable Torque Capacity ($T_{\text{max}}$):

$$T_{\text{max}} = \frac{1}{2} \mu \cdot p \cdot \pi \cdot d^2 \cdot L = 0.5 \times 0.15 \times 64.69 \times 10^6 \times \pi \times (0.060)^2 \times 0.075$$ $$T_{\text{max}} = 4.85175 \times 10^6 \times 3.14159 \times 0.0036 \times 0.075 = 4,115.4\ \text{N}\cdot\text{m}$$

Step 4: Check Hub Bore Tensile Hoop Stress and Yield Safety:

$$\sigma_{t,\text{max}} = p \times 1.6667 = 64.69\ \text{MPa} \times 1.6667 = 107.82\ \text{MPa}$$ $$\sigma_{\text{von Mises}} = \sqrt{107.82^2 + (107.82 \times 64.69) + 64.69^2} = \sqrt{11625 + 6975 + 4185} = \sqrt{22785} = 150.95\ \text{MPa}$$ $$\text{FoS} = \frac{S_y}{\sigma_{\text{von Mises}}} = \frac{400\ \text{MPa}}{150.95\ \text{MPa}} = 2.65\ \text{(Safe)}$$

Conclusion: The joint safely transmits over $4,115\ \text{N}\cdot\text{m}$ of continuous torque with a high safety factor of $2.65$ against hub yielding.

Frequently Asked Questions (FAQ)

What is an interference press fit?

An interference press fit (or shrink fit) is a permanent or semi-permanent mechanical fastening method where the outer diameter of a shaft is slightly larger than the mating bore diameter of a hub. When forced together, elastic deformation generates intense radial contact pressure, enabling torque and axial load transmission via friction without keys, splines, or welds.

How does Lamé's thick-walled cylinder theory apply to press fits?

Lamé equations model the radial and tangential hoop stress distributions in thick-walled concentric cylinders. By matching the radial displacement $\delta$ of the inner cylinder (shaft compression) and outer cylinder (hub dilation) at the interface boundary, the exact interfacial contact pressure $p$ is determined.

What is the difference between mechanical press fitting and thermal shrink fitting?

Mechanical press fitting forces components together at ambient temperature using a hydraulic press, requiring high insertion force and creating galling or scoring risk. Thermal shrink fitting heats the hub (expanding the bore) or cools the shaft in liquid nitrogen/dry ice (shrinking the shaft) to achieve zero-clearance drop-in assembly without mechanical abrasion.

What ISO tolerance classes correspond to interference fits?

Common ISO interference fits include H7/p6 (light press fit for rigid positioning), H7/r6 (medium drive fit for permanent hubs), and H7/s6 (heavy permanent shrink fit for maximum torque transmission).