For an isotropic radiator, the radiation intensity for a given total radiated power of (P) is given by
P/4π
An isotropic radiator is a hypothetical antenna that radiates power uniformly in all directions. While such an antenna does not exist in practice, it serves as an important theoretical reference point for evaluating the performance of real-world antennas. Its radiation pattern is perfectly spherical, meaning the power density is the same at any point on a sphere centered around the antenna.
Radiation intensity ($U$) is a crucial parameter in antenna theory, representing the power radiated by an antenna per unit solid angle. It is expressed in Watts per steradian (W/sr). Mathematically, it can be defined as:
$$ U = \frac{dP}{d\Omega} $$
where $dP$ is the power radiated into a differential solid angle $d\Omega$.
For an isotropic radiator, the total radiated power ($P$) is spread uniformly over the entire spherical surface. The total solid angle encompassing a full sphere is $4\pi$ steradians. This is a fundamental constant used in spherical coordinates.
Since an isotropic radiator distributes its total radiated power ($P$) uniformly over the entire solid angle of a sphere ($4\pi$ steradians), the radiation intensity ($U$) can be found by dividing the total radiated power by the total solid angle:
$$ U = \frac{\text{Total Radiated Power}}{\text{Total Solid Angle}} $$
Substituting the given total radiated power ($P$) and the total solid angle for a sphere ($4\pi$ steradians):
$$ U = \frac{P}{4\pi} \text{ W/sr} $$
This formula indicates that for an isotropic radiator, the radiation intensity is constant in all directions, as expected from its definition of uniform radiation.
Based on the definition and properties of an isotropic radiator, the radiation intensity for a given total radiated power ($P$) is indeed given by $P/4\pi$. This fundamental relationship is essential for understanding antenna characteristics and calculating other related parameters like gain and directivity.
Therefore, the correct expression for the radiation intensity of an isotropic radiator is $P/4\pi$.
A device that makes possible the use of the same antenna for transmission and reception both
Match column A with column B.
Column A | Column B | ||
1. | Point electromagnetic source | P. | Highly directional |
2. | Dish antenna | Q. | End fire |
3. | Yagi-Uda antenna | R. | Isotropic |
Broadside arrays have
A. Number of dipoles of unequal size
B. Number of dipoles equally spaced
C. Collinear dipoles
D. Dipoles in phase
E. Dipoles are 90 out of phase
Choose the correct answer from the options given below:
Consider the following statements:
(a) Fiber optic cable is much lighter than copper cable
(b) Fiber optic cable is not affected by power surges or electromagnetic interference
(c) Optical transmission is inherently bidirectional.
Which of the statements is (are) correct?A Yagi-uda array does not have