Est. read time: 1 minute | Last updated: December 17, 2024 by John Gentile


Contents

Open In Colab

Uniform Linear Array (ULA)

image.png

A ULA is defined as an array with NN elements equally spaced a distance dd from each other along a linear axis. Each RF channel- related to an RF antenna element- is sampled synchronously such that the digital samples are aligned in time across all channels so coherent processing can be performed. It can be seen that when dealing with a signal from the far field impinging on the array with angle, θ0\theta_{0}, the difference in propagation path length, LL, between elements in a ULA is given by:

L(n)=ndsin(θ0),0nN1L(n) = nd\sin(\theta_{0}), \quad 0 \leq n \leq N - 1

The reason we assume far field characteristics for the majority of this work to simplify the math and operations of phased arrays; for the case of a phased array receiver in the near field, an RF emitter is so close to the array that the incident angle of the received energy is different for every element due to the spherical wavefront of the source:

image.png

However, in the far field, where the same emitter is farther away from the receiving array, the wavefronts become approximately planar, and each receive element sees an equivalent incidence angle, θ\theta, of the arriving wave:

image.png

The specific point at which a given system is operating in the far field is dependent on many factors of the array’s antenna properties, however a general equation can be found based on an array’s antenna diameter, DD, and the wavelength of the operating carrier frequency, λ\lambda:

FarField>2D2λFar Field > \frac{2D^{2}}{\lambda}

References