In materials like mild steel, the stress-strain curve shows a distinct yield point — where the material begins to deform plastically with minimal increase in stress. This unique behavior is attributed to the
dislocation mechanics within the crystal lattice.
Peierls-Nabarro Barrier and Yield Point: - The Peierls-Nabarro barrier represents the energy needed to move dislocations through a crystal lattice.
- Initially, dislocations are pinned due to obstacles like interstitial atoms (e.g., carbon in steel).
- Once the applied stress is sufficient to overcome this barrier, dislocations move abruptly, leading to the sharp yield point behavior.
- This sudden movement initiates plastic flow and is followed by a yield plateau.
Why Other Options Are Incorrect: - (A) Dislocation orientation isn’t the primary factor — it’s their mobility that matters.
- (B) Redistribution of internal stresses may occur, but it does not explain the abrupt yield phenomenon.
- (D) Strain hardening occurs later in the plastic region, not at the yield point.
Therefore, the yield point phenomenon in mild steel is due to the
abrupt movement of dislocations after overcoming the Peierls-Nabarro barrier.