Problem 20
Question
Amorphous silica, \(\mathrm{SiO}_{2}\), has a density of about \(2.2 \mathrm{~g} / \mathrm{cm}^{3}\), whereas the density of crystalline quartz, another form of \(\mathrm{SiO}_{2}\), is \(2.65 \mathrm{~g} / \mathrm{cm}^{3}\). Which of the following statements is the best explanation for the difference in density? (a) Amorphous silica is a network-covalent solid, but quartz is metallic. (b) Amorphous silica crystallizes in a primitive cubic lattice. (c) Quartz is harder than amorphous silica. (d) Quartz must have a larger unit cell than amorphous silica. (e) The atoms in amorphous silica do not pack as efficiently in three dimensions as compared to the atoms in quartz.
Step-by-Step Solution
Verified Answer
The answer is (e): Atoms in amorphous silica do not pack as efficiently in three dimensions as in quartz.
1Step 1: Understanding Density
Density is defined as mass per unit volume. For two substances of the same chemical composition like amorphous silica and crystalline quartz, a difference in density must be attributed to how tightly the atoms or molecules are packed together in each structure.
2Step 2: Comparing the Structures
Amorphous silica lacks a long-range ordered structure, unlike crystalline quartz, which has a repeating, ordered lattice. This means the atoms in amorphous silica are not packed as efficiently in three dimensions compared to the highly structured and packed nature of quartz.
3Step 3: Evaluating the Options
Let's evaluate the provided options:
(a) is incorrect since both amorphous silica and quartz are network covalent solids; quartz is not metallic.
(b) is incorrect because amorphous silica lacks a crystalline lattice structure.
(c) is irrelevant as hardness isn't directly related to density.
(d) is incorrect; typically, a larger unit cell suggests lower density.
(e) directly relates packing efficiency to density differences, which aligns with the structural differences between amorphous and crystalline forms.
Key Concepts
Amorphous SilicaCrystalline QuartzPacking EfficiencyNetwork-Covalent Solids
Amorphous Silica
Amorphous silica, represented by the chemical formula \( \mathrm{SiO}_2 \), is one of the clearest examples of a material that lacks an ordered structure. Unlike its crystalline counterpart, quartz, amorphous silica does not have a long-range periodic arrangement of its atoms.
This absence of a regular lattice structure makes amorphous silica seemingly random and more like a glass. In this form, the molecules are not tightly packed, leading to a lower density—approximately \(2.2 \mathrm{g} / \mathrm{cm}^{3}\). Without a repeating pattern, the atoms have less connectivity and order, which affects its density and a number of its physical properties.
Understanding the nature of amorphous silica is important in fields such as mineralogy, materials science, and chemistry, where the contrast between amorphous materials and their crystalline counterparts significantly impacts their applications and behavior.
This absence of a regular lattice structure makes amorphous silica seemingly random and more like a glass. In this form, the molecules are not tightly packed, leading to a lower density—approximately \(2.2 \mathrm{g} / \mathrm{cm}^{3}\). Without a repeating pattern, the atoms have less connectivity and order, which affects its density and a number of its physical properties.
Understanding the nature of amorphous silica is important in fields such as mineralogy, materials science, and chemistry, where the contrast between amorphous materials and their crystalline counterparts significantly impacts their applications and behavior.
Crystalline Quartz
Crystalline quartz is also a form of \( \mathrm{SiO}_2 \), but unlike amorphous silica, it features a highly ordered lattice structure. In quartz, the atoms are arranged in a repeating pattern that extends in three dimensions. This regularity is what gives quartz its characteristic shape, clarity, and well-defined optical properties.
The densely packed arrangement in quartz contributes to its higher density of \(2.65 \mathrm{g} / \mathrm{cm}^{3}\), compared to amorphous silica.
The structure of quartz not only affects its density but also its mechanical properties, such as toughness and thermal stability. This organized packing allows quartz to be used in a variety of technological and industrial applications, where robustness and resilience are crucial.
The densely packed arrangement in quartz contributes to its higher density of \(2.65 \mathrm{g} / \mathrm{cm}^{3}\), compared to amorphous silica.
The structure of quartz not only affects its density but also its mechanical properties, such as toughness and thermal stability. This organized packing allows quartz to be used in a variety of technological and industrial applications, where robustness and resilience are crucial.
Packing Efficiency
Packing efficiency refers to how tightly atoms or molecules are packed within a substance. Higher packing efficiency means more atoms occupy a given volume, leading to a higher density.
In crystalline solids like quartz, the ordered lattice structure allows for high packing efficiency as atoms fit together without much void space. This efficient use of space results in a solid that is not only denser but also stronger and less prone to deformation.
On the other hand, amorphous materials such as amorphous silica have much lower packing efficiency. Due to their lack of a systematic arrangement, there is significant empty space between atoms, resulting in a lower density.
Understanding packing efficiency is crucial for determining the properties of various materials, such as their strength, durability, and how they interact with light and electricity.
In crystalline solids like quartz, the ordered lattice structure allows for high packing efficiency as atoms fit together without much void space. This efficient use of space results in a solid that is not only denser but also stronger and less prone to deformation.
On the other hand, amorphous materials such as amorphous silica have much lower packing efficiency. Due to their lack of a systematic arrangement, there is significant empty space between atoms, resulting in a lower density.
Understanding packing efficiency is crucial for determining the properties of various materials, such as their strength, durability, and how they interact with light and electricity.
Network-Covalent Solids
Network-covalent solids are a unique class of solids characterized by a continuous network of covalent bonds. Both amorphous silica and crystalline quartz belong to this category.
In these solids, atoms are connected through covalent bonds across the entire material, which can impart distinctive physical properties such as hardness, high melting points, and poor electrical conductivity.
Unlike ionic or metallic solids, which rely on ion-electron interactions or free electrons for cohesion, network-covalent solids like quartz exhibit extreme stability due to their extensive covalent bonding. In the case of amorphous silica, the lack of order does not diminish the strength of the individual covalent bonds, but it does impact the overall structural integrity and efficiency.
This classification of solids plays a significant role in various applications—from serving as critical components in electronics to being used in the creation of strong, heat-resistant materials.
In these solids, atoms are connected through covalent bonds across the entire material, which can impart distinctive physical properties such as hardness, high melting points, and poor electrical conductivity.
Unlike ionic or metallic solids, which rely on ion-electron interactions or free electrons for cohesion, network-covalent solids like quartz exhibit extreme stability due to their extensive covalent bonding. In the case of amorphous silica, the lack of order does not diminish the strength of the individual covalent bonds, but it does impact the overall structural integrity and efficiency.
This classification of solids plays a significant role in various applications—from serving as critical components in electronics to being used in the creation of strong, heat-resistant materials.
Other exercises in this chapter
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