To provide some perspective on the dimensions of atomic defects, consider a metal specimen that has a dislocation density of \(10^{4} \mathrm{mm}^{-2}\). Suppose that all the dislocations in \(1000 \mathrm{~mm}^{3}\left(1 \mathrm{~cm}^{3}\right)\) were somehow removed and linked end to end. How far (in miles) would this chain extend? Now suppose that the density is increased to \(10^{10} \mathrm{~mm}^{-2}\) by cold working. What would be the chain length of dislocations in \(1000 \mathrm{~mm}^{3}\) of material?

Short Answer

Expert verified
The chain length of dislocations for a dislocation density of \(10^4 \,\mathrm{mm}^{-2}\) is approximately 0.062 miles, and for a dislocation density of \(10^{10} \,\mathrm{mm}^{-2}\), it is approximately 621 miles.

Step by step solution

01

Calculate the total number of dislocations for both densities

First, we need to calculate the total number of dislocations in the specimen for both densities, which can be obtained by multiplying the density with the volume of the specimen. For the first case with a dislocation density of \(10^4 \,\mathrm{mm}^{-2}\), the total number of dislocations is: Total dislocations = Density × Volume Total dislocations = \(10^4 \,\mathrm{mm}^{-2} \times 1000 \,\mathrm{mm}^{3}\) Total dislocations = \(10^7\) dislocations For the second case with a dislocation density of \(10^{10} \,\mathrm{mm}^{-2}\), the total number of dislocations is: Total dislocations = \(10^{10} \,\mathrm{mm}^{-2} \times 1000 \,\mathrm{mm}^{3}\) Total dislocations = \(10^{13}\) dislocations
02

Find the chain lengths of dislocations

Next, we need to find the chain lengths of the dislocations for both cases. To do this, we assume that each dislocation has a length equal to the average distance between them, which can be estimated as the inverse of the square root of the dislocation density. For the first case with a dislocation density of \(10^4 \,\mathrm{mm}^{-2}\): Average dislocation distance = \(\sqrt{1/(10^4 \,\mathrm{mm}^{-2})}\) Chain length = Total dislocations × Average dislocation distance Chain length = \(10^7 \times \sqrt{1/(10^4 \,\mathrm{mm}^{-2})}\) Chain length = \(10^7 \times \sqrt{1/10^4} \,\mathrm{mm}\) Chain length = \(10^7 \times 0.01 \,\mathrm{mm} = 10^5 \,\mathrm{mm}\) For the second case with a dislocation density of \(10^{10} \,\mathrm{mm}^{-2}\): Average dislocation distance = \(\sqrt{1/(10^{10} \,\mathrm{mm}^{-2})}\) Chain length = Total dislocations × Average dislocation distance Chain length = \(10^{13} \times \sqrt{1/(10^{10} \,\mathrm{mm}^{-2})}\) Chain length = \(10^{13} \times \sqrt{1/10^{10}} \,\mathrm{mm}\) Chain length = \(10^{13} \times 0.0001 \,\mathrm{mm} = 10^9 \,\mathrm{mm}\)
03

Convert the chain length to miles

Finally, we need to convert the chain lengths from millimeters to miles. We know that 1 mile = 1,609,344 millimeters. For the first case with a dislocation density of \(10^4 \,\mathrm{mm}^{-2}\): Chain length (in miles) = Chain length (in mm) / 1,609,344 mm/mile Chain length (in miles) = \(10^5 \,\mathrm{mm} / 1,609,344 \,\mathrm{mm/mile}\) Chain length (in miles) ≈ 0.062 miles For the second case with a dislocation density of \(10^{10} \,\mathrm{mm}^{-2}\): Chain length (in miles) = Chain length (in mm) / 1,609,344 mm/mile Chain length (in miles) = \(10^9 \,\mathrm{mm} / 1,609,344 \,\mathrm{mm/mile}\) Chain length (in miles) ≈ 621 miles In conclusion, for the first case, the chain of dislocations would extend about 0.062 miles, and for the second case, it would extend about 621 miles.

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Most popular questions from this chapter

(a) What is the approximate ductility (\%EL) of a brass that has a yield strength of \(275 \mathrm{MPa}\) \((40,000 \mathrm{psi}) ?\) (b) What is the approximate Brinell hardness of a 1040 steel having a yield strength of 690 \(\mathrm{MPa}(100,000 \mathrm{psi})\) ?

Two previously undeformed cylindrical specimens of an alloy are to be strain hardened by reducing their cross-sectional areas (while maintaining their circular cross sections). For one specimen, the initial and deformed radii are \(16 \mathrm{~mm}\) and \(11 \mathrm{~mm}\), respectively. The second specimen, with an initial radius of \(12 \mathrm{~mm}\), must have the same deformed hardness as the first specimen; compute the second specimen's radius after deformation.

Explain the differences in grain structure for a metal that has been cold worked and one that has been cold worked and then recrystallized.

For each of edge, screw, and mixed dislocations, cite the relationship between the direction of the applied shear stress and the direction of dislocation line motion.

Experimentally, it has been observed for single crystals of a number of metals that the critical resolved shear stress \(\tau_{\text {crsss }}\) is a function of the dislocation density \(\rho_{D}\) as $$ \tau_{\text {crss }}=\tau_{0}+A \sqrt{\rho_{D}} $$ where \(\tau_{0}\) and \(A\) are constants. For copper, the critical resolved shear stress is \(2.10 \mathrm{MPa}\) (305 psi) at a dislocation density of \(10^{5} \mathrm{~mm}^{-2}\). If it is known that the value of \(A\) for copper is \(6.35\) \(\times 10^{-3} \mathrm{MPa} \cdot \mathrm{mm}(0.92 \mathrm{psi} \cdot \mathrm{mm})\), compute \(\tau_{\text {crss }}\) at a dislocation density of \(10^{7} \mathrm{~mm}^{-2}\).

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