Chapter 5: Problem 23
Potassium crystallizes in a bce structure. The atomic radius of potassium is \(235 \mathrm{pm}\). Determine (a) the number of atoms per unit cell; (b) the coordination number of the lattice; (c) the length of the side of the unit cell.
Short Answer
Expert verified
The number of atoms per unit cell in a bcc lattice is 2, the coordination number is 8, and the length of the side of the unit cell is approximately 558 pm.
Step by step solution
01
Determine the number of atoms per unit cell for a bcc lattice
In a body-centered cubic (bcc) structure, there is one atom at each corner of the cube and one atom at the center. Each corner atom is shared among eight unit cells, so each contributes 1/8 of an atom to the unit cell. Therefore, there are 8 corners each contributing 1/8 of an atom and 1 atom in the center, giving a total of: 8 * (1/8) + 1 = 1 + 1 = 2 atoms per unit cell.
02
Determine the coordination number of the bcc lattice
The coordination number is the number of atoms that each atom touches. In a bcc structure, the atom at the center of the unit cell touches the 8 atoms at the corners. Therefore, the coordination number is 8.
03
Calculate the length of the side of the unit cell
In a bcc structure, the body diagonal of the cube is equal to four times the atomic radius (since one body diagonal passes through two radiuses for the center atom and half the radius for each corner atom). Therefore, the length of the body diagonal (\r) is calculated by \r = 4 times the atomic radius. The body diagonal is also related to the cube side length (\r) by the Pythagorean theorem for a cube with side length \r: 2 \r^2. Setting the diagonal equal to 4 times the atomic radius we get: \(\r_{diagonal} = \r \times \r^2 + \r \times \r^2 + \r \times \r^2 = \r \times (3 \r^2) = \r \times (3 \times (235 \r pm \times 2)\) = \r \times 4 \times 235 \r pm = \r \times 3 \r \times S^2\. Solving for S (unit cell side length), S = \r(4 \times 235 \r pm) / \r(3)\r^2. Hence, S = \r4 \r \times 235 \r pm / \r(3)^\r(1/2) \r pm^\r(1/2) approx 558 \r pm.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Crystal Lattice
Understanding the crystal lattice is crucial when studying the properties of materials. A crystal lattice is a three-dimensional arrangement of atoms, ions, or molecules in a crystalline material. It consists of repeated geometric patterns called unit cells, which together create the overall structure of the crystal.
The potassium in our exercise exists in a body-centered cubic (bcc) crystal lattice. This specific arrangement is one of the multiple types of lattices that materials can form. A bcc lattice means that each unit cell's structure is a cube with atoms at all eight corners and a single atom at the very center of the cube. By comprehending the layout of a crystal lattice, we can predict numerous physical properties of the material, such as its density, melting point, and how it interacts with light or electricity.
In this case, the bcc structure influences how atoms interact, their spacing, and how they're coordinated with each other, which we'll explore further in the related sections.
The potassium in our exercise exists in a body-centered cubic (bcc) crystal lattice. This specific arrangement is one of the multiple types of lattices that materials can form. A bcc lattice means that each unit cell's structure is a cube with atoms at all eight corners and a single atom at the very center of the cube. By comprehending the layout of a crystal lattice, we can predict numerous physical properties of the material, such as its density, melting point, and how it interacts with light or electricity.
In this case, the bcc structure influences how atoms interact, their spacing, and how they're coordinated with each other, which we'll explore further in the related sections.
Atomic Radius
The atomic radius refers to the size of an atom, typically denoting the distance from the center of the nucleus to the boundary of the surrounding cloud of electrons. Understanding the atomic radius is fundamental in explaining various material properties, including reactivity and bond strength.
In a bcc lattice structure, the atomic radius can be directly linked to the geometry of the unit cell. Since these atoms are packed in a specific pattern, we can calculate the distances between them based on the atomic radius. Potassium's atomic radius is given to us as 235 pm (picometers), which is a small but crucial piece of the puzzle. This measurement enables us to determine the size of the unit cell and how atoms are packed within it, ultimately relating to the crystal's density and physical properties.
The atomic radius is a key component in finding the length of the unit cell's edge in the bcc structure, as stepping through the calculation shows us the relationship between the two measurements.
In a bcc lattice structure, the atomic radius can be directly linked to the geometry of the unit cell. Since these atoms are packed in a specific pattern, we can calculate the distances between them based on the atomic radius. Potassium's atomic radius is given to us as 235 pm (picometers), which is a small but crucial piece of the puzzle. This measurement enables us to determine the size of the unit cell and how atoms are packed within it, ultimately relating to the crystal's density and physical properties.
The atomic radius is a key component in finding the length of the unit cell's edge in the bcc structure, as stepping through the calculation shows us the relationship between the two measurements.
Coordination Number
The coordination number is a term that describes the number of nearest-neighbor atoms or ions surrounding an atom within a crystal structure. For many crystalline materials, it can provide insight into the strength of the bonds within the structure and its reactivity.
With the bcc structure of potassium, as shown in this exercise, we see that each atom in the center of the unit cell has eight surrounding atoms at the corners. This means the coordination number for potassium in this layout is 8. The higher the coordination number, the more atoms directly interact with any given atom, which can affect the properties of the material, such as how it deforms under stress or its thermal expansion characteristics.
The concept of coordination number also ties into the concept of atomic packing efficiency and is critical for understanding the stability of the crystal structure.
With the bcc structure of potassium, as shown in this exercise, we see that each atom in the center of the unit cell has eight surrounding atoms at the corners. This means the coordination number for potassium in this layout is 8. The higher the coordination number, the more atoms directly interact with any given atom, which can affect the properties of the material, such as how it deforms under stress or its thermal expansion characteristics.
The concept of coordination number also ties into the concept of atomic packing efficiency and is critical for understanding the stability of the crystal structure.
Unit Cell Geometry
Unit cell geometry in crystalline materials refers to the shape and dimensions of the smallest repeating unit that makes up the crystal lattice. It is the fundamental building block from which the entire crystal is constructed.
In our exercise, the geometry of the bcc unit cell is cubic, meaning all edges are of equal length and all angles are right angles. However, this simplicity can be deceptive, as determining the edge length requires careful calculation. The solution steps demonstrate that the edge length is tied to the atomic radius, and we can use this to calculate properties such as density and atomic packing factors.
By calculating the side length of the cube, which is approximately 558 pm for potassium, we gain vital information about the spacing between atoms and how they are arranged in three-dimensional space. This geometry impacts properties such as crystal's mechanical strength and its thermal and electrical conductivity.
In our exercise, the geometry of the bcc unit cell is cubic, meaning all edges are of equal length and all angles are right angles. However, this simplicity can be deceptive, as determining the edge length requires careful calculation. The solution steps demonstrate that the edge length is tied to the atomic radius, and we can use this to calculate properties such as density and atomic packing factors.
By calculating the side length of the cube, which is approximately 558 pm for potassium, we gain vital information about the spacing between atoms and how they are arranged in three-dimensional space. This geometry impacts properties such as crystal's mechanical strength and its thermal and electrical conductivity.