Force-Analysis: Cam - Contact-Stress

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Force-Analysis: Cam - Contact-Stress

Preamble -

Engineers can buy Follower-Roller bearings from catalogs and the web. To select a bearing, they must calculate the payload, estimate contamination, lubrication, operating temperature, and decide on the reliability they need. If the Follower-Roller bearing fails, then the difference between the actual and design environment can be reviewed. If necessary, the engineer can change the Follower-Roller bearing to one that has shields or seals to reduce contamination, or one that has a full compliment of rollers or balls.

It is rare that a Follower-Roller is faulty. Suppliers have high standards that control the steel-quality, manufacturing processes, and heat-treatment of the bearing's elements. The capacity of bearings that are the same size and type but from a different suppliers will be similar.

However, the steel, manufacture, and heat-treatment processes of cams are often confidential to each machine-supplier. Each supplier may not divulge their standards to competitors.

Vehicle cam-shafts have been used for many years for 10,000,000+ of vehicles. The cams are fully lubricated and wear is minimal for 10,000,000+ rotations.

However, industrial packaging, assembly, and textile machines are manufactured from as little as 1 time, to say 1000 times.

Even though a cam is an easier machine element to analyze, it is left to the machine designer to choose the correct steel, manufacturing, heat-treatment processes, and method of lubrication, to give the cam an operational-life as required by their customers.


Note Norton: Follower-Rollers are typically made of tool steel, hardened to Rockwell C60-62 (HRC60-62). The cam surface should be equally hard or as hard as its material will permit.


Nominal Contact Stress - Cylindrical Follower-Roller and Line Contact

As a cam rolls under Follower-Roller (or the Follower-Roller rolls over a cam) the cam and the Follower-Roller become stressed and slightly flattened. The stresses at and below the contact-surface are quite complex. They are not like the stresses that you can calculate from Tension, Bending or Torsion. Hertz was the first to calculate the stress field. The stress is now frequently termed Hertzian Contact Stress (Reference Hertz (1881) has done the hard work to derive the equations we need to calculate the stress when there is contact between two bodies that are conformal or non-conformal.
[H. R. Hertz, "Über die Berührung fester elastischer Körper (On Contact Between Elastic Bodies)" Journal für die reine und angewandte Mathematik 92, 1881 pp. 156-171].
),
Hertzian Stress, or Contact-Stress.

We calculate for you the Maximum Shear Stress from the contact-stress that act in different orthogonal x,y,z directions.

It is convenient to consider two contact types:

Line-Contact : between two cylinders with parallel axes. Line-contact is equivalent to a cylindrical Follower-Roller in contact with a 2D-Cam. The contact is actually a narrow rectangle.

Elliptical-Contact : between bodies with more complex shapes. Each body has a radius in the rolling direction, and at least one body has a radius that is orthogonal to the rolling direction. Most frequently, elliptical-contact is made when a barrel shaped Follower-Roller is in contact with a 2D-Cam or a 3D-Cam.

Hertzian Stress at the Cam Surface (Line Contact)

Contact Stress field Contact-Area = L×2.b

Contact Stress field
Contact-Area = L×2.b

 

2D-Cams and Cylindrical Follower-Rollers result in so called Line contact.

the Cam-Profile is prismatic, although each point along the Cam-Profile has a different radius-of-curvature.

the Follower-Roller is cylindrical.

When the force between the Cam-Profile and Follower-Roller is very low, the contact is almost a thin line. As the force increases, the Cam-Profile and Follower-Roller deform and the contact becomes a narrow rectangle across the width of the Cam-Profile and Follower-Roller. The area of the rectangle is equal to the width of the Cam (L) × Contact-Width (2×b) (see image above).

Parameters to calculate Hertzian Contact-Stress for Line-Contact.

Maximum Hertzian Contact-Stress (N/mm2)

Length of the contact.

Cam's Elastic Modulus, Follower-Roller Elastic Modulus (N/mm2)

Cam's Poisson Ratio, Follower-Roller's Poisson Ratio (-)

Cam's Radius-of-Curvature , Follower-Roller's Radius (mm)

Contact Force (N)

Equivalent Radius-of-Curvature,

Equivalent Elastic Modulus,

Half-width, , in direction of rolling:

Mean Hertzian Stress:

Maximum Hertzian Stress:

Substituting for gives, Maximum Hertzian Stress:

 is at the middle of the contact patch, below the axis of the rolling Follower-Roller

Stress below the center of the Line Contact axis (x=0)

Principal Contact Stresses directly under the rolling axis of a Cylindircal Follower-Roller and 2D-Cam

Principal Contact Stresses directly under the rolling axis of a Cylindircal Follower-Roller and 2D-Cam

The image above shows the principal stresses (all compressive) relative to the Maximum Hertzian Contact Stress, , directly below the center-line of contact.

Scale of Horizontal-Axis :

Scale of Vertical-Axis      :

: Stress in the vertical direction

 : Stress in the horizontal direction, in direction of rolling

 : Stress in the horizontal direction, in direction that is across the width of contact

: Tresca Shear-Stress, (also known as ). It is equal to the maximum difference between any two of the principal stresses.

Maximum of Shear-Stress, (Line Contact)

Depth of Maximum Shear-Stress, (Line-Contact)


The image above shows that the stresses, , , and are compressive. Because the contact-stress drops to very low values outside of the contact, the surrounding material (called the hinterland) does not move away to accommodate the expansion.

Mohr's Circle for stress state at 0.78b below the Cam's Surface

This is another way of representing the principal stresses, but at a slice beneath the surface. The slice is at the depth equal to the Maximum Shear-Stress () - at below the surface ( is half the contact-width)

MoMohr's Circles for the Hertzian Contact Stress at a depth, or slice, below the contact equal to 0.78b. This is the depth below surface at which the Shear-Stress is the Maximum.

Mohr's Circles for the Hertzian Contact Stress at a depth, or slice, below the contact equal to 0.78b. This is the depth below surface at which the Shear-Stress is the Maximum.

Principal Shear Stresses, , ,

This image shows the Mohr's Circles for the Principal Stresses, , , , at the depth of .

Each stress is relative to the Maximum Contact Stress, that is at the surface, but at a depth below the surface.

@0.78b   = –0.32

@0.78b  = –0.15

@0.78b = –0.75

Maximum Shear Stress,

From the scale of the Mohr's Circles, we can see that the Maximum Shear Stress (vertical axis) is one half the diameter of the largest circle.

In many cases, surface roughness, friction, lubrication, thermal effects, and residual stresses will invalidate the exact results from Hertzian analysis. Consequently, you should regard the Hertzian Contact-Stress as guidelines that correlate with experimental tests that find allowable stress limits.

Schematic of Orthogonal Shear Stress due to of 'Free Rolling' and 'Traction Rolling'

GDI-Shear-Stress

Orthogonal Shear Stress moving through the contact zone - image to left.

The Hertzian Contact Stress contact-stresses lead to Octahedral shear-stress and Orthogonal shear-stresses under the surface at the contact. The image to the left schematically illustrates how a cylinder rolling over a flat body in the absence of friction develops subsurface stresses. The stress at a depth of 0.78b, just below the center of the contact, is the maximum shear stress (octahedral) - see analysis above. It occurs at 45° to the contact surface.

Orthogonal shear stresses are parallel and perpendicular to the contact surface are in-front of and behind the contact line/rectangle. The orthogonal stress in-front and behind have equal and opposite signs. The magnitudes of the orthogonal stresses are always lower than the magnitude of the octahedral shear stress. However, the range of the orthogonal stresses is higher than the octahedral stress and is thought to be a more potent contributor to the development of contact fatigue damage. The Orthogonal Shear Stress is believed to be significant with respect to sub-surface Fatigue Cracks.

The maximum Orthogonal Shear Stresses are :

below the surface.

to in-front and behind contact axis.

, with a full range of .

Shear Stress and Traction with Rolling Friction

Many elements that are in contact will slide as they pass over each other. For example, gear-teeth, and flat-faced followers sliding along a cam.

There is always a coefficient of friction and thus a friction force. This results in tangential, normal, and shear stresses that superimpose on the Hertzian Contact Stresses, described above. These stresses are illustrated schematically in the image.

Schematic of stress that superimpose with a rolling cylinder with traction or friction

Schematic of stress that superimpose with a rolling cylinder with traction or friction