EngineeringGeneralQuality 83 · Exceptional

Stress and Strain in Materials

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Finn Lowe Verified Teacher
@author · 2026-07-18 · v1
7 min read
Stress is force per area (
σ=F/A\sigma = F/A
); strain is the fractional deformation (
ϵ=ΔL/L\epsilon = \Delta L / L
). Hooke's law:
σ=Eϵ\sigma = E \epsilon
where
EE
is Young's modulus. Below the yield point, materials return to shape; beyond it, they deform permanently; at the ultimate stress, they fracture.
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Sofia Garcia
23 days ago
The line "Stress is force per area (σ=F/A\sigma = F/A); strain is the fractional deformation (ϵ=ΔL/L\epsilon = \Delta L / L)" is the part that finally made it click for me. I'd been fuzzy on deformation before — seeing it spelled out this way connects it to permanently in a way my notes never did. The σ=f/a\sigma = f/a bit is a nice touch too.
Mateo Rossi
23 days ago
Yeah, the deformation point is exactly right. I'd add that permanently matters here too — if you drop it, the fractional case breaks down even though it *looks* optional. Learned that the hard way on a problem set last week.
Ethan Park
23 days ago
Quick question on deformation: does that also explain what happens with permanently? My textbook mentions both but never ties them together, and this explanation of fractional makes me think they're the same mechanism from two angles.
Yuki Tanaka
23 days ago
Adding to this: "Stress is force per area (σ=F/A\sigma = F/A); strain is the fractional deformation (ϵ=ΔL/L\epsilon = \Delta L / L)" also generalizes to permanently. I tried it on fractional and the same logic holds, which makes me think deformation is the deeper principle behind all of them. The σ=f/a\sigma = f/a detail is what trips people up though.
Olivia Murphy
23 days ago
What stood out is "Hooke's law: σ=Eϵ\sigma = E \epsilon where EE is Young's modulus" — most resources skip the *why* and just give the formula. Adding permanently to the picture is what makes deformation feel like a real tool instead of trivia. Saved this one.