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Stress Transformations
“It is a narrow mind which cannot look
at a subject from various points of
view.”
― George Eliot
BIOE 3200 - Fall 2015
Learning Objectives
 Calculate stresses in multiple planes
(stress transformations) in rigid bodies
BIOE 3200 - Fall 2015
Stresses within a rigid body
BIOE 3200 - Fall 2015
Stress elements
BIOE 3200 - Fall 2015
Recall stresses defined in 3D:
BIOE 3200 - Fall 2015
Summing forces on an inclined
stress element
BIOE 3200 - Fall 2015
Stress Transformations
 𝜎𝑥𝑥
′
=
𝜎 𝑥𝑥+𝜎 𝑦𝑦
2
+
𝜎 𝑥𝑥−𝜎 𝑦𝑦
2
𝑐𝑜𝑠2𝜃 + 𝜏 𝑥𝑦 𝑠𝑖𝑛2𝜃

 𝜎 𝑦𝑦
′ =
𝜎 𝑥𝑥+𝜎 𝑦𝑦
2
+
𝜎 𝑦𝑦−𝜎 𝑥𝑥
2
𝑐𝑜𝑠2𝜃 − 𝜏 𝑥𝑦 𝑠𝑖𝑛2𝜃

 𝜏 𝑥𝑦
′
=
𝜎 𝑦𝑦−𝜎 𝑥𝑥
2
𝑠𝑖𝑛2𝜃 + 𝜏 𝑥𝑦 𝑐𝑜𝑠2𝜃
BIOE 3200 - Fall 2015

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3 stress transformations

Editor's Notes

  1. To obtain a complete picture of the stresses in a bar, we must consider stresses acting on an “inclined” (as opposed to a “normal”) section through the bar. Stresses on both normal and inclined sections are uniformly distributed.
  2. When working with stress elements, only one intrinsic state of stress exists at a point in a stressed body, regardless of the orientation of the element used to portray the state of stress. We can rotate axes to represent stresses in a new coordinate system, oriented at any angle to the original x-y system. (Draw x’ – y’ axes at angle theta to x-y axes)
  3. Normal stresses σxx, σyy, σzz (tension is positive) Shear stresses τxy = τyx, τxz = τzx, τyz = τzy Shear stress sign convention: for τij: Subscript “i” refers to direction normal to the plane on which it acts – the “face” of the stress element Subscript “j” refers to the direction the shear stress is applied. Now consider plane stress in the xy plane: only x and y faces are subjected to stresses (σz = 0 and τzx = τxz = τzy = τyz = 0). Such a stress element could be located on the free surface of a body (no stresses acting normal to the free surface).
  4. Stress transformation equations derived from summing forces on 2D stress element, and using shear stress equalities and trig identities Full explanation of math behind stress transformation equations is in text and as annotated pdf (posted on Blackboard).
  5. Point out stress components on plane stress element and transformation of stress components (primes) For stresses on the y’ face, substitute 𝜃+90 for 𝜃 in the x’ equation Summing the expressions for σ’x and σ’y can be used to find σ’x or σ’y instead of full transformation equation