The dielectric constant and electric susceptibility are both measures related to how materials respond to electric fields, but they describe different aspects of this behavior. Here's a detailed breakdown of the two concepts:
### 1. Dielectric Constant
**Definition:**
The dielectric constant, often denoted as \(\kappa\) or \(\epsilon_r\), is a measure of a material's ability to store electrical energy in an electric field relative to the vacuum. It essentially tells us how much the material can reduce the effective electric field within it compared to the field in a vacuum.
**Mathematical Expression:**
The dielectric constant is defined as the ratio of the permittivity of the material (\(\epsilon\)) to the permittivity of free space (\(\epsilon_0\)):
\[ \kappa = \frac{\epsilon}{\epsilon_0} \]
where:
- \(\epsilon\) is the absolute permittivity of the material.
- \(\epsilon_0\) is the permittivity of free space (approximately \(8.854 \times 10^{-12}\) F/m).
**Physical Interpretation:**
A higher dielectric constant means the material can store more electrical energy per unit voltage applied. It also indicates that the material can reduce the effective electric field within it compared to a vacuum. This property is crucial in applications like capacitors, where materials with high dielectric constants are used to increase capacitance.
### 2. Electric Susceptibility
**Definition:**
Electric susceptibility, denoted by \(\chi_e\), measures how easily a material becomes polarized in response to an electric field. It is a dimensionless quantity that indicates the extent to which a material will be polarized when exposed to an electric field.
**Mathematical Expression:**
Electric susceptibility is related to the dielectric constant by the following relationship:
\[ \kappa = 1 + \chi_e \]
where \(\chi_e\) is the electric susceptibility.
**Physical Interpretation:**
Electric susceptibility is a measure of the material’s response to an external electric field in terms of polarization. A higher susceptibility means the material will become more polarized, leading to a greater dielectric constant.
### Key Differences:
1. **Nature of Measurement:**
- **Dielectric Constant (\(\kappa\))**: Measures the overall ability of a material to store electrical energy compared to a vacuum. It’s a ratio involving the absolute permittivity of the material.
- **Electric Susceptibility (\(\chi_e\))**: Measures the extent to which a material becomes polarized in response to an electric field. It reflects the material’s polarizability.
2. **Units:**
- **Dielectric Constant**: Dimensionless, but derived from permittivity which has units of Farads per meter (F/m).
- **Electric Susceptibility**: Dimensionless.
3. **Relationship:**
- **Dielectric Constant**: \(\kappa = \frac{\epsilon}{\epsilon_0}\).
- **Electric Susceptibility**: \(\kappa = 1 + \chi_e\), which implies \(\chi_e = \kappa - 1\).
### Example:
Consider a material with a dielectric constant of 5. This implies:
- The electric susceptibility \(\chi_e\) of the material is \(\kappa - 1 = 5 - 1 = 4\).
- The material can store electrical energy more effectively compared to a vacuum, and it becomes polarized to a greater extent under an electric field.
In summary, while both dielectric constant and electric susceptibility describe how materials interact with electric fields, the dielectric constant is more about energy storage capacity, and electric susceptibility is about the degree of polarization.