Chapter 4: Problem 20
Determine the radius of a cation having \(\mathrm{CsCl}\) structure, when all anions are in contact with the cation and touch each other. The critical radius of the anion is \(1.90 A\).
Short Answer
Expert verified
The radius of the cation is approximately 1.39 Å.
Step by step solution
01
Understand the Structure
The given cation has a CsCl structure. This structure is a cubic crystal system where the cations and anions are positioned at the center and corners of the cube, respectively.
02
Identify Key Distances
In a CsCl structure, the cations and anions are in contact. The closest distance between the center of a cation and the center of an anion is half the body diagonal of the cube.
03
Calculate the Body Diagonal
The body diagonal of a unit cell in a cubic structure is given by \(\text{diagonal} = \sqrt{3}a\), where \(a\) is the side length of the cube.
04
Relate Radius to Body Diagonal
In a CsCl structure, the radius of the cation \(r_c\) plus the radius of the anion \(r_a = 1.90 \, \text{Å}\) equals half the body diagonal. Therefore, \(\frac{\sqrt{3}a}{2} = r_c + r_a\).
05
Set Up Equation
Since the size of the unit cell can be expressed in terms of the anion radius (\(a = 2r_a = 2 \times 1.90 \, \text{Å}\)), substitute this into the equation. This gives \(\frac{\sqrt{3} \times 2 \times 1.90}{2} = r_c + 1.90\).
06
Solve for Cation Radius
Simplify the equation: \[\frac{\sqrt{3} \times 3.80}{2} = r_c + 1.90\] \[\sqrt{3} \times 1.90 = r_c + 1.90\] \[r_c = \sqrt{3} \times 1.90 - 1.90\] \[r_c \approx (1.732 \times 1.90 - 1.90) \approx 3.291 - 1.90 \approx 1.39\, \text{Å}\]
Unlock Step-by-Step Solutions & Ace Your Exams!
-
Full Textbook Solutions
Get detailed explanations and key concepts
-
Unlimited Al creation
Al flashcards, explanations, exams and more...
-
Ads-free access
To over 500 millions flashcards
-
Money-back guarantee
We refund you if you fail your exam.
Over 30 million students worldwide already upgrade their learning with Vaia!
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Cubic Crystal System
The cubic crystal system is one of the most straightforward and symmetrical forms of crystal structures. It features atoms arranged at the corners of a cube.
There are different types of cubic systems, but the CsCl structure falls under the simple cubic category, specifically known as a body-centered cubic (BCC) structure.
In this structure, there is one type of atom, the cation, located at the center of the cube, and another type, the anion, positioned at each corner.
This arrangement is essential for maintaining the structure's stability and balance. Here are some characteristics of a cubic crystal system:
There are different types of cubic systems, but the CsCl structure falls under the simple cubic category, specifically known as a body-centered cubic (BCC) structure.
In this structure, there is one type of atom, the cation, located at the center of the cube, and another type, the anion, positioned at each corner.
This arrangement is essential for maintaining the structure's stability and balance. Here are some characteristics of a cubic crystal system:
- High symmetry and regular geometry
- Equal axes and 90-degree angles between them
- Repetition of the basic unit throughout the entire crystal
Body Diagonal
In the context of a cubic crystal system, the body diagonal is a crucial concept.
The body diagonal refers to the line connecting one corner of the cube to the opposite corner, passing through the center of the cube.
This diagonal is longer than the edges of the cube. The length of the body diagonal in a cubic crystal system can be calculated using the formula \[\text{diagonal} = \sqrt{3} \ cdot a\] where \(a\) is the side length of the cube.
This equation comes from applying the Pythagorean theorem in three dimensions.
Here’s a breakdown:
The body diagonal refers to the line connecting one corner of the cube to the opposite corner, passing through the center of the cube.
This diagonal is longer than the edges of the cube. The length of the body diagonal in a cubic crystal system can be calculated using the formula \[\text{diagonal} = \sqrt{3} \ cdot a\] where \(a\) is the side length of the cube.
This equation comes from applying the Pythagorean theorem in three dimensions.
Here’s a breakdown:
- First, calculate the diagonal of a face of the cube, which is \sqrt{2} \cdot a
- Then, apply the Pythagorean theorem again with this face diagonal and the side length \(a\), providing the body diagonal formula
Anion and Cation Contact
In the CsCl structure, the arrangement and contact of anions and cations are crucial to understanding the crystal's stability.
The cation at the center of the cube is surrounded by eight anions located at the cube's corners.
These anions and cations are in direct contact, maintaining the structure’s integrity.
To determine the radius of the cation, consider that the distance from the center of the cation to the center of an anion is half the body diagonal.
\[\frac{\sqrt{3} \cdot 3.80}{2} = r_c + 1.90\]\
Simplify to find the cation radius \(r_c\): \[r_c = \sqrt{3} \cdot 1.90 - 1.90 ≈ 1.39 \text{ Å}\]\ Understanding how these ions are in contact helps in visualizing and calculating distances within the crystal lattice accurately.
The cation at the center of the cube is surrounded by eight anions located at the cube's corners.
These anions and cations are in direct contact, maintaining the structure’s integrity.
To determine the radius of the cation, consider that the distance from the center of the cation to the center of an anion is half the body diagonal.
- Given: Anion radius \(r_a = 1.90 \text{ Å}\)
- Key relationship: \(\frac{\sqrt{3} \cdot a}{2} = r_c + r_a\)
- Calculate side length: \(a = 2 \cdot r_a = 2 \cdot 1.90 \text{ Å}\)
\[\frac{\sqrt{3} \cdot 3.80}{2} = r_c + 1.90\]\
Simplify to find the cation radius \(r_c\): \[r_c = \sqrt{3} \cdot 1.90 - 1.90 ≈ 1.39 \text{ Å}\]\ Understanding how these ions are in contact helps in visualizing and calculating distances within the crystal lattice accurately.