The stress required to operate a Frank-Read source is inversely proportional to the length of the dislocation segment acting as the source. In a polycrystalline material, the maximum length of such an immobilized segment is related to the grain size ($d$). Therefore, the shear stress ($\tau$) required is proportional to the inverse of the grain size: $\tau \propto \frac{1}{d}$.
We can establish a relationship between the initial state (1) and the final state (2):
$ \tau_1 d_1 = \tau_2 d_2 $
Where:
Convert the initial grain size to nanometers (nm) for consistency:
$ d_1 = 10 \text{ µm} = 10 \times 10^3 \text{ nm} $
Rearrange the formula to solve for $ \tau_2 $:
$ \tau_2 = \tau_1 \times \frac{d_1}{d_2} $
Substitute the values:
$ \tau_2 = 100 \text{ MPa} \times \frac{10 \times 10^3 \text{ nm}}{10 \text{ nm}} $
$ \tau_2 = 100 \text{ MPa} \times 10^3 $
$ \tau_2 = 100,000 \text{ MPa} $
Expressing this in scientific notation:
$ \tau_2 = 10^5 \text{ MPa} $
When the grain size is reduced to $ 10 \text{ nm} $, the shear stress required to operate the Frank-Read source increases significantly to $ 10^5 \text{ MPa} $.
The Burger's vector of a dislocation in a cubic crystal (with lattice parameter a) is $\frac{a}{2}[110]$ and dislocation line is along $[112]$ direction. The angle (in degrees) between the dislocation line and its Burger's vector is _________