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If for a material, \(Y\) and \(B\) are Young's modulus and Bulk modulus then : (a) \(Y<3 B\) (b) \(Y=3 B\) (c) \(Y>3 B\) (d) \(3 Y=B\)

Short Answer

Expert verified
(a) \(Y < 3B\) is generally correct since \(\nu\) for materials is not zero.

Step by step solution

01

Understanding the Relationship

Young's modulus and Bulk modulus are related to each other through Poisson's ratio, \( u \), which describes the material's behavior when stressed. The relationship is given by the formula: \[ Y = 3B(1 - 2u) \].
02

Analyzing the Formula

Since \( u \) typically ranges from 0 to 0.5 for most materials, the expression \( 1 - 2u \) will range from 1 to 0.
03

Substituting Extreme Values

If \( u = 0 \), we substitute into the formula: \[ Y = 3B(1 - 2(0)) = 3B \]. This implies \( Y = 3B \) if \( u = 0 \). If \( u \) is in the range (0, 0.5), then \( 1 - 2u \) is less than 1, and hence \( Y < 3B \).
04

Conclusion

Given \( u \) for practical materials is seldom 0, typically \( Y < 3B \). Therefore, option \( (a) \) is generally the correct choice.

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Key Concepts

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

Bulk Modulus
The Bulk Modulus of a material characterizes its ability to withstand changes in volume when subjected to uniform pressure. In simpler terms, it determines how compressible a material is. Mathematically, Bulk Modulus is defined as the ratio of the change in pressure to the relative change in volume. The higher the Bulk Modulus, the less compressible the material is. This property is vital in applications where materials are exposed to high pressures, such as in undersea pipelines or aircraft cabins.
Materials with high Bulk Modulus (like steel) can endure substantial pressure changes without significant volume alterations. Conversely, materials with low Bulk Modulus are more compressible and deform more easily under pressure. Understanding this property helps engineers and scientists select the appropriate materials for specific environments and applications.
Poisson's Ratio
Poisson's Ratio, denoted by the symbol \( u \), provides insight into the material's behavior under stress, particularly during tensile or compressive stress. This ratio is defined as the negative ratio of the transverse strain to the axial strain. Essentially, it describes how much a material will become thinner or thicker in response to stretching or compressing.
  • If \( u \) is close to zero, the material shows little lateral expansion or contraction when longitudinally stretched or compressed.
  • If \( u \) is close to 0.5, the material experiences significant lateral changes when stressed. This is often the maximum practical value for most materials.
For engineering purposes, knowing Poisson's Ratio helps predict how materials will behave under different loading conditions. For example, rubber has a high Poisson's Ratio near 0.5, indicating it swells noticeably when compressed, while cork's Poisson's Ratio is near 0, showing minimal expansion.
Material Properties
Material Properties refer to the inherent attributes or characteristics of materials that define their behavior under various conditions. These properties help in determining what applications the material is suited for. They include mechanical, thermal, electrical, and chemical properties.
  • Mechanical Properties: Include Young’s modulus, Bulk modulus, shear modulus, yield strength, and tensile strength, which collectively describe how a material will respond to forces and stresses.
  • Thermal Properties: Such as conductivity, coefficient of thermal expansion, and specific heat capacity, which dictate how a material reacts to temperature changes.
  • Electrical Properties: Include conductivity, resistivity, and dielectric strength, essential in selecting materials for electrical applications.
  • Chemical Properties: Include corrosion resistance and chemical stability, vital for materials used in chemically harsh environments.
Understanding these properties is critical in the material selection process, ensuring suitability and safety in practical applications.

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Most popular questions from this chapter

The linear strain in \(x, y\) and \(z\) -directions are \(e_{x}, e_{y}\) and \(e_{z}\) respectively. Then the volumetric strain is given by: (a) \(e_{x} e_{y} e_{z}\) (b) \(e_{x}+e_{y}+e_{z}\) (c) \(e_{t}=e_{x} e_{y}\) (d) \(e_{z}=\frac{e_{r}+e_{y}}{2}\)

Two cylinders of same material and of same length are joined end to end as shown in figure. The upper end of \(A\) is rigidly fixed. Their radii are in ratio of \(1: 2\) respectively. If the lower end of \(B\) is twisted by an angle \(\theta\), the angle of twist of cylinder \(A\) is: (a) \(\frac{15}{16} \theta\) (b) \(\frac{16}{15} \theta\) (c) \(\frac{16}{17} \theta\) (d) \(\frac{17}{16} \theta\)

Two wires, one made of copper and other of steel are joined end to end. (as shown in figure). The area of cross-section of copper wire is twice that of steel wire. They are placed under compressive force of magnitudes \(F\). The ratio of their lengths such that change in lengths of both wires are same is: \(\left(Y_{S}=2 \times 10^{11} \mathrm{~N} / \mathrm{m}^{2}\right.\) and \(\left.Y_{C}=1.1 \times 10^{11} \mathrm{~N} / \mathrm{m}^{2}\right)\) (a) \(2.1\) (b) \(1.1\) (c) \(1.2\) (d) 2

What will happen if a metal wire is stretched a little beyond its elastic limit (or yield point) and released? (a) It loses its elastic property completely (b) It does not contract (c) It contracts, but its final length will be greater than its initial length (d) It contracts only up to its length at the elastic limit

Equal weights are suspended from two wires of the same metal one of these wire is of length \(2 \mathrm{~m}\) and diameter 1 \(\mathrm{mm}\), while the other is of length \(1 \mathrm{~m}\) and diameter \(0.5\) \(\mathrm{mm}\). Then : (a) first wire has greater extension (b) second wire has greater extension (c) both wire have the same extension (d) extension in both wires are zero

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