Is it possible for two screw dislocations of opposite sign to annihilate each other? Explain your answer.

Short Answer

Expert verified
Explain your answer. Answer: No, two screw dislocations of opposite sign cannot cancel each other out or annihilate each other. This is because their helical paths are in opposite directions, resulting in distortions introduced into the crystal lattice that do not perfectly align or match. Consequently, their atomic displacements cannot cancel each other out, leaving the lattice defects present.

Step by step solution

01

Understanding Screw Dislocations

Screw dislocations are a type of lattice defect in crystalline materials, characterized by the displacement of atoms along a helical path. Screw dislocations can be either right-handed (positive sign) or left-handed (negative sign), depending on the direction of the atomic displacement along the helical path. Screw dislocations cause a distortion in the crystal lattice, affecting the material's mechanical properties.
02

Interactions Between Dislocations

When two dislocations interact, their relationship is influenced by the stress field around each dislocation and the elastic strain energy associated with their defects. If two dislocations move closer to each other, they can create a new configuration that minimizes the overall strain energy, leading to lower stress in the crystal.
03

Cancellation or Annihilation of Dislocations

The process of two dislocations annihilating each other involves the defects canceling each other out, resulting in a perfect crystal lattice without the screw dislocation. However, this can only happen when the two dislocations have precisely matching displacements and alignments between the helical paths they introduce to the material.
04

Considering Opposite Sign Screw Dislocations

In the case of two screw dislocations with opposite signs, the helical paths introduced by each dislocation are in opposite directions. This means that the distortions introduced by each dislocation into the crystal lattice do not perfectly align or match. As a result, the atomic displacements cannot cancel each other out, making it impossible for them to annihilate each other.
05

Conclusion

The answer to the given exercise is that it is not possible for two screw dislocations of opposite sign to annihilate each other because their distortions in the crystal lattice do not align or match. Thus, their displacements cannot cancel each other out, leaving the lattice defects present.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Crystal Lattice Defects
Crystal lattice defects play a crucial role in determining the mechanical, electrical, and thermal properties of materials. In crystalline solids, atoms are arranged in a repeating pattern known as a lattice. However, the ideal periodic arrangement is often disrupted by defects, which can vary greatly in complexity.

One basic type of defect is the point defect, which includes vacancies (missing atoms) and interstitials (extra atoms) within the lattice. But when it comes to altering the mechanical properties of materials, dislocations are the most impactful. Dislocations are line defects where an extra half-plane of atoms is inserted into the lattice, causing a mismatch along a line in the material. There are two main types of dislocations: edge dislocations and screw dislocations.

In our exercise, we focused on screw dislocations, where the atoms are displaced along a helical path around the dislocation line. This helical structure introduces significant distortions in the crystal which can affect the ease with which a material can be deformed (plasticity) and its strength. Understanding screw dislocations is essential in fields like materials science and mechanical engineering, as they are often the source of failure in crystalline materials under stress.
Elastic Strain Energy
The concept of elastic strain energy is critical in understanding how materials deform and how defects like dislocations behave within a crystal lattice. When a material is deformed, it stores energy due to the displacement of atoms from their equilibrium positions. If the material is elastic—meaning it will return to its original shape when the stress is removed—this stored energy is known as elastic strain energy.

The presence of dislocations increases the material's elastic strain energy because atoms are out of their regular positions, creating regions of compression and tension in the lattice. The system naturally wants to reduce this energy, which can cause dislocations to move or interact with other defects in search of a more energetically favorable configuration.

In our discussion, the interaction between two screw dislocations leads to a new lattice configuration that can lower the overall strain energy. However, for two screw dislocations of opposite signs, this reduction in energy cannot be fully realized because their opposing orientations prevent them from perfectly overlapping and canceling each other out.
Dislocation Interactions
Dislocation interactions are a key aspect of how materials respond to applied stress and undergo deformation. As dislocations move through a crystal lattice, they can encounter other dislocations. The outcome of these interactions can be complex due to the long-range stress fields that dislocations generate.

When two dislocations with identical signs approach each other, they repel because their stress fields create similar disturbances in the lattice. Conversely, dislocations of opposite signs may attract each other; however, annihilation only occurs if their core structures can align to cancel the distortions. This is dependent on their Burgers vectors, which describe the nature and magnitude of the lattice distortion.

An Important Consideration

As mentioned in the exercise solution, screw dislocations can have a right-handed or left-handed helicity, akin to having a positive or negative sign. For two screw dislocations of opposite signs to annihilate, they must have a perfect match in their displacement fields—something that is not possible when the helical paths are mirror opposites. This is why opposite sign screw dislocations cannot annihilate each other, leaving the defects within the crystal, an important concept for understanding material failure and designing stronger materials.

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Most popular questions from this chapter

A single crystal of a metal that has the FCC crystal structure is oriented such that a tensile stress is applied parallel to the [100] di rection. If the critical resolved shear stress for this material is 0.5 MPa, calculate the magnitude(s) of applied stress(es) necessary to cause slip to occur on the (111) plane in each of the \([1 \overline{1} 0],[10 \overline{1}],\) and [011] directions

An uncold-worked brass specimen of average grain size \(0.01 \mathrm{mm}\) has a yield strength of \(150 \mathrm{MPa}(21,750 \mathrm{psi}) .\) Estimate the yield strength of this alloy after it has been heated to \(500^{\circ} \mathrm{C}\) for \(1000 \mathrm{s}\), if it is known that the value of \(\sigma_{0}\) is \(25 \mathrm{MPa}(3625 \mathrm{psi})\).

Consider a single crystal of some hypothetical metal that has the BCC crystal structure and is oriented such that a tensile stress is applied along a [121] direction. If slip occurs on a (101) plane and in a \([\overline{1} 11]\) direction, compute the stress at which the crystal yields if its critical resolved shear stress is \(2.4 \mathrm{MPa}\)

(a) Compare planar densities (Section 3.11 and Problem 3.53 ) for the \((100),(110),\) and (111) planes for FCC. (b) Compare planar densities (Problem 3.54 ) for the \((100),(110),\) and (111) planes for \(\mathrm{BCC}\)

An undeformed specimen of some alloy has an average grain diameter of \(0.050 \mathrm{mm} .\) You are asked to reduce its average grain diameter to \(0.020 \mathrm{mm}\). Is this possible? If so, explain the procedures you would use and name the processes involved. If it is not possible, explain why.

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