Motion Systems Handbook 2019

Page 96

MOTION SYSTEMS HANDBOOK

Hertz contact stresses:

How they affect linear bearings Linear bearings that use balls or rollers to carry a load are subjected to Hertz contact stresses — a type of material stress that plays a significant role in determining the bearing’s load capacity and fatigue life. When two surfaces of different radii are in contact and a load is applied (even an extremely small load) a small contact area is formed, and the surfaces experience very high stresses. These stresses are known as Hertz (or Hertizian) contact stresses. In rolling element linear bearings, Hertz contact stresses occur on the balls (or cylinders) and the raceways. In theory, the contact between two spheres occurs at a point, and the contact between two cylinders occurs as a line. In either case — point or line contact — the resulting pressure between the two surfaces would be infinite and the surfaces would experience immediate yielding. But in real-world applications, when two surfaces are pressed together with a force, some elastic deformation occurs at each surface, and a contact area is formed. The stresses that occur on the two surfaces may still be very high — sufficient to initiate spalling or other forms of failure — but they are no longer infinite. The analysis of Hertzian contact stresses relies on four primary assumptions: • • • •

The surfaces are smooth and frictionless The bodies are isotropic and elastic The contact area is small relative to the sizes of the bodies in contact The strains on the bodies are small and within the elastic limit

Hertzian stresses are present when any two surfaces with different radii are in contact — even if one surface is flat or if one surface is convex and the other is concave, which is the case for rolling element bearings: the ball or roller is convex, and the raceway is concave. In the analysis of Hertz contact stresses, a convex surface (the ball or roller) has a positive radius and the concave surface (the raceway) has a negative radius. Flat surfaces have an infinite radius.

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DESIGN WORLD — MOTION

Linear Guide Rails & Slides & Ways — Motion Control HB 08-19 V3.indd 92

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Because the surfaces have different radii, the contact area between a spherical ball and a bearing raceway has an elliptical shape. Under these conditions, the maximum pressure between the two surfaces for a spherical ball and raceway is given as: Where a and b are the width and length of the contact area and F = Normal force on the assembly. For a cylindrical roller and raceway the contact is rectangular with: Where (2)b = Width of the contact area and L = the length of contact. In fact, Hertz contact stresses have a significant effect on bearing dynamic load capacity and L10 life. Shear stresses, which cause fatigue — a primary mode of failure of rolling elements — are proportional to the maximum Hertz pressure between the two bodies. Hertz contact, and the resulting deformation of surfaces, is also what causes bearings to skid rather than roll. This is because the Hertz contact areas have different diameters than the rolling elements themselves, so the rolling elements slip. Hertz contact has implications for bearing preload as well. Preloading the rolling elements gives them a larger — and finite — Hertz contact area, which increases stiffness. But the increased contact results in high heat generation. This is why a preload amount of just 8% is considered high preload for linear bearings, with preload greater than 10 to 15% being extremely rare. Also, because Hertz contact is nonlinear, a small amount of preload can provide significant stiffness boost without resulting in unacceptable slip, friction, and heat.

motioncontroltips.com | designworldonline.com

8/21/19 12:50 PM


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The basics of compression springs

2min
pages 138-139

Update on shock & vibration technologies

4min
pages 130-137

Sensors for motion systems

2min
pages 128-129

Update on sealing technologies

2min
pages 126-127

The basics of retaining rings

1min
pages 124-125

Positioning systems: An overview

3min
pages 120-123

Stepper motors – an overview

4min
pages 116-119

Servomotors: the basics

3min
pages 112-115

Summary of direct-drive motors

6min
pages 108-111

Fundamentals of gearmotors

3min
pages 104-107

Fundamentals of dc motors

3min
pages 100-103

When should you use dual guide rails?

1min
pages 98-99

Hertz contact stresses: How they affect linear bearings

2min
pages 96-97

Calculating linear bearing life

4min
pages 92-95

Human-machine interfaces (HMIs) in evolution from operator terminals

2min
pages 90-91

Gearbox service factor and service class explained

7min
pages 82-89

Encoders – the basics

5min
pages 76-81

Flexible couplings for motion design

7min
pages 66-73

Conveyors for simple to complex transport

5min
pages 62-65

Programmable automation controllers (PACs) and industrial PCs

5min
pages 58-61

Servo versus closed-loop stepper motion controls

5min
pages 54-57

Flexible and controlled cabling and connections

4min
pages 48-53

Brakes, clutches, and torque limiters

7min
pages 42-47

Sizing and applying belts and pullets

3min
pages 38-41

Basics of sprockets and chain drives

3min
pages 36-38

Rotary bearings for precision motion applications

5min
pages 30-35

The basics of ball & roller screws

3min
pages 28-29

Chain actuation – rigid type

2min
pages 26-27

Pneumatic actuators

6min
pages 22-25

Linear actuators: Make versus buy

10min
pages 14-21

What ancient myths can teach us about today's technology

2min
page 8
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