A coaxial transmission line has inner and outer conductor radii \(a\) and \(b\). Between conductors \((a<\rho

Current density, denoted as \( \textbf{J} \), is a measure of the electric current per unit area of cross-section in a given region. It is a vector quantity, providing both magnitude and direction of the flow of current. For a coaxial transmission line, current density is significant as it helps in understanding the distribution of current within the conductive medium. The current density field \( \textbf{J} \) within the coaxial line having a radially dependent conductivity \( \textbf{J}(\rho) = \sigma(\rho)E(\rho) \).

For direct current (dc) and radial current, where the current flows perpendicular to the cylindrical surface, the current density only has a radial component. In our problem, to find \( \textbf{J} \), we use the given relationship between conductivity and radial distance, \( \sigma(\rho) = \frac{\sigma_0}{\rho} \), and integrate over the region between conductors to relate the total current per unit length \( I \) to \( \textbf{J} \). The concept of current density is crucial in understanding how the electric current is distributed in transmission lines and how this distribution affects the line's electrical properties.

Electric field intensity, represented as \( \textbf{E} \), is the force per unit charge experienced by a stationary test charge placed in an electric field. For a coaxial cable with radial current, \( \textbf{E} \) is directed radially outward or inward, depending on the sign of the charge on the inner conductor. The intensity of this electric field is determined by the current density \( \textbf{J} \) along with the material's conductivity. In the given problem, we express \( \textbf{E} \) in terms of \( I \) and other parameters through \( E(\rho) = J(\rho) \rho / \sigma_0 \), considering the relationship between \( \textbf{J} \) and \( \textbf{E} \) in a medium of conductivity \( \sigma(\rho) \).

Understanding electric field intensity is vital as it influences how voltage is distributed along the transmission line and affects the operation of the line in terms of energy transfer and potential differences.

Radial current refers to the component of electric current that flows radially in or out of a cylindrical conductor. In the context of a coaxial transmission line, radial current is the flow of charge per unit length between the inner and outer conductors. This current is crucial for determining many parameters of the line, such as the current density and the electric field intensity within the conductive medium. In our example, the dc radial current \( I \) per unit length is established in the coaxial transmission line, which then determines the current density field and ultimately relates to the potential difference across the conductors.

The line integral in the context of electric fields is a mathematical tool used to calculate the work done by the electric field in moving a charge between two points. This is essential in our problem for relating the electric field intensity \( \textbf{E} \) and the potential difference \( V_0 \), which is the voltage across the inner and outer conductors of the coaxial line. By taking the line integral of \( \textbf{E} \), one can integrate \( E(\rho) \) from radius \( a \) to \( b \) to find the potential difference as \( V_0 = -\int_{a}^{b} E(\rho) d\rho \).

Understanding the line integral concept helps in connecting the concepts of electric field and electric potential, which are central to the analysis of electric circuits and transmission lines.

Conductance, symbolized as \( G \), is the measure of a material's ability to conduct electric current. It is the reciprocal of resistance and is expressed in siemens (S). For a coaxial transmission line, the conductance per unit length is a key parameter as it describes how well the line can carry an electrical signal without significant losses. In our problem, once the potential difference \( V_0 \) has been related to the radial current \( I \), the conductance of the line per unit length can be found using the relation \( G = I/V_0 \). This principle is used to calculate the conductance based on the known values, which then gives us an understanding of the transmission line’s performance in terms of power efficiency and signal integrity.