🌱 Tony's Memex Tony's Intertwingled Memex
Digital Garden | OER Curriculum
Home / Digital Garden / Stress Concentration at Structural Notch (Mechanical Engineering) Solution

Stress Concentration at Structural Notch (Mechanical Engineering) Solution

Problem Overview

We analyze the geometric continuity, differentiability, and stress concentration characteristics of the V-notch profile:

y(x)=∣x−5∣+2y(x) = |x - 5| + 2
at the notch vertex x=5x = 5.


Step-by-Step Mathematical Solution

Step 1: Prove Continuity at x=5x = 5

Rewrite y(x)y(x) as a piecewise function:

y(x)={−(x−5)+2=−x+7x<5(x−5)+2=x−3x≥5y(x) = \begin{cases} -(x - 5) + 2 = -x + 7 & x < 5 \\ (x - 5) + 2 = x - 3 & x \ge 5 \end{cases}

  • Left-hand limit: lim⁡x→5−(−x+7)=−5+7=2\lim_{x \to 5^-} (-x + 7) = -5 + 7 = 2
  • Right-hand limit: lim⁡x→5+(x−3)=5−3=2\lim_{x \to 5^+} (x - 3) = 5 - 3 = 2
  • Function value: y(5)=∣5−5∣+2=2y(5) = |5 - 5| + 2 = 2

Since lim⁡x→5−y(x)=lim⁡x→5+y(x)=y(5)=2\lim_{x \to 5^-} y(x) = \lim_{x \to 5^+} y(x) = y(5) = 2, the bracket contour is continuous at x=5x = 5.

Step 2: Test for Differentiability at x=5x = 5

Compute the one-sided derivative limits using the difference quotient:

  • Left-hand derivative:
    lim⁡h→0−y(5+h)−y(5)h=lim⁡h→0−∣(5+h)−5∣+2−2h=lim⁡h→0−∣h∣h=lim⁡h→0−−hh=−1\lim_{h \to 0^-} \frac{y(5+h) - y(5)}{h} = \lim_{h \to 0^-} \frac{|(5+h) - 5| + 2 - 2}{h} = \lim_{h \to 0^-} \frac{|h|}{h} = \lim_{h \to 0^-} \frac{-h}{h} = -1
  • Right-hand derivative:
    lim⁡h→0+y(5+h)−y(5)h=lim⁡h→0+∣h∣h=lim⁡h→0+hh=+1\lim_{h \to 0^+} \frac{y(5+h) - y(5)}{h} = \lim_{h \to 0^+} \frac{|h|}{h} = \lim_{h \to 0^+} \frac{h}{h} = +1

Because lim⁡h→0−Δyh=−1≠+1=lim⁡h→0+Δyh\lim_{h \to 0^-} \frac{\Delta y}{h} = -1 \neq +1 = \lim_{h \to 0^+} \frac{\Delta y}{h}, the two-sided limit does not exist. The function has a sharp corner and is non-differentiable at x=5x = 5.


Engineering Conclusion

In structural mechanics and elasticity theory, an abrupt geometric corner with zero radius of curvature (r→0r \to 0) causes the theoretical stress concentration factor Kt=1+2a/rK_t = 1 + 2\sqrt{a/r} to approach infinity. Under dynamic cyclic service loads, physical stress lines crowd at this non-differentiable vertex, inducing localized plastic deformation and micro-crack nucleation.

To eliminate this catastrophic failure mode, mechanical engineers replace sharp corners with tangent transition arcs or smooth polynomial curves (fillets), ensuring that the geometric derivative y′(x)y'(x) remains continuous (C1C^1) across the entire surface profile and distributing internal stresses uniformly.