Post from Woodbear Sep 6, 2006
“Some clarification of stress and strain is needed here.
Tom has correctly defined strain, it is a measure of the geometric deformation (stretch or compression) of the back & belly wood of the bow arm. I find it easiest to think of it in terms of percentage. That is a strain of 1% means the wood is 1% different in length compared to the original length of the wood without any applied force. 1% compression means the belly is only 99% as long as it is when no force is applied. 1% tension means that the back is 101% as long as without applied force.
Think about a short section of the bow arm say 100mm long, 20mm thick, and bending with a radius of 1000mm. Assuming that the cross section is rectangular, the length of the wood on the back is 101mm, and the length of the wood on the belly is 99mm long. The surface strain is 1% in both tension, and compression.
The relationship between stress and strain is stress equals strain multiplied by the elastic modulus (stress = strain * MOE). Strain is a unitless ratio, and stress has the same units as elastic modulus (MOE), and is measured in force per unit area (i.e. g/mm^2).
In the 100mm section of bow arm for example, let the wood be Yew with MOE of about 800,000g/mm^2, and the stress will be 8,000g/mm^2, or 1% of the MOE. Since the MOE is the same through out the wood (ignoring knots & defects etc.) equal stress and equal strain must both happen at the same time.
A bow with a perfectly circular tiller, and a thickness taper, can not have uniform stress or strain. Stress and strain will be highest where the wood is thickest. To obtain uniform strain and stress, the radius of curvature of the drawn bow must be proportional to the thickness of the bow arms through out the bow. A pyramid bow with circular tiller, and uniform arm thickness has uniform strain. An ELB with a thickness taper, can have uniform stress and strain if the tiller is elliptical, with the bend radius proportional to the thickness of the arms.
What Tim was talking about as stress, should properly be called bending moment, or bending force in the bow arm. The bending moment at any point on the bow arm can be found by measuring the distance from the location on the bow arm, to the string (at full draw for the maximum value experienced by the bow.), and multiplying by the string tension. The distance must be measured at right angles from the string to the bow arm location. It is clear that the distance from the string to the nock is zero right at the nock. The maximum distance from a point on the bow to the string will be from the center of the handle to the string. Half way down the arm from the center to the nock, there will be only about the distance between the string and bow arm, and consequently only half the bending moment. This is not exact since the bow arm is not straight but bent in an arc. A convenient way to see this is to take a photo of the bow on the tiller stick at full draw, and then measure the distance from the bow arm to the string all along the bow. The bending moment is proportional to the distance from the string, since the string tension is the same every where in the string.
Dave”