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The uniform linear array (ULA) arranges identical sensor elements
along a line in space with uniform spacing. You can design a ULA with `phased.ULA`

.
When you use this object, you must specify these aspects of the array:

Sensor elements of the array

Spacing between array elements

Number of elements in the array

Create and view a ULA having four isotropic antenna elements separated by 0.5 meters

array = phased.ULA('NumElements',4,'ElementSpacing',0.5); viewArray(array);

You can return the coordinates of the array sensor elements in the form `[x;y;z]`

by using the `getElementPosition`

method. See Rectangular Coordinates for toolbox conventions.

sensorpos = getElementPosition(array);

`sensorpos`

is a 3-by-4 matrix with each column representing the position of a sensor element. Note that the *y*-axis is the array axis. The positive *x*-axis is the array look direction (0 degrees broadside). The elements are symmetric with the respect to the phase center of the array.

The default element for a ULA is the `phased.IsotropicAntennaElement`

object.
You can specify a different element using the `Element`

property.

Obtain the responses of the elements of a 4-element ULA array at 1 GHz.

**Note:** This example runs only in R2016b or later. If you are using an earlier release, replace each call to the function with the equivalent `step`

syntax. For example, replace `myObject(x)`

with `step(myObject,x)`

.

Specify isotopic antennas for the array elements. Then, specify a 4-element ULA. Obtain the response by executing the System object™.

antenna = phased.IsotropicAntennaElement(... 'FrequencyRange',[3e8 1e9]); array = phased.ULA('NumElements',4,'ElementSpacing',0.5,... 'Element',antenna); freq = 1e9; azangles = -180:180; response = array(freq,azangles);

`response`

is a 4-by-361 matrix where each column contains the responses at each azimuth angle. Matrix rows correspond to the four elements. Because the elements of the ULA are isotropic antennas, `response`

is a matrix of ones.

This example computes the delay between elements of a 4-element ULA using the `phased.ElementDelay`

System object™. Assume that the incident waveform satisfies the far-field condition. The delays are computed with respect to the phase center of the array. By default, `phased.ElementDelay`

assumes that the incident waveform is an electromagnetic wave propagating at the speed of light.

**Note:** This example runs only in R2016b or later. If you are using an earlier release, replace each call to the function with the equivalent `step`

syntax. For example, replace `myObject(x)`

with `step(myObject,x)`

.

Construct 4-element ULA using value-only syntax and compute the delay for a signal incident on the array from -90° azimuth and 0° elevation. Delay units are in seconds.

```
array = phased.ULA(4);
delay = phased.ElementDelay('SensorArray',array);
tau = delay([-90;0])
```

```
tau =
1.0e-08 *
-0.2502
-0.0834
0.0834
0.2502
```

`tau`

is a 4-by-1 vector of delays with respect to the phase center of the array, which is the origin of the local coordinate system *(0;0;0)*. See Global and Local Coordinate Systems for a description of global and local coordinate systems. Negative delays indicate that the signal arrives at an element before reaching the phase center of the array. Because the waveform arrives from an azimuth angle of -90°, the signal arrives at the first and second elements of the ULA before it reaches the phase center resulting in negative delays for these elements.

If the signal is incident on the array at 0° broadside from a far-field source, the signal illuminates all elements of the array simultaneously resulting in zero delay.

tau = delay([0;0])

```
tau =
0
0
0
0
```

If the incident signal is an acoustic pressure waveform propagating at the speed of sound, you can calculate the element delays by setting the `PropagationSpeed`

property to 340 m/s. This value is a typical speed of sound at sea level.

delay = phased.ElementDelay('SensorArray',array,... 'PropagationSpeed',340); tau = delay([90;0])

```
tau =
0.0022
0.0007
-0.0007
-0.0022
```

The *steering vector* represents the relative
phase shifts for the incident far-field waveform across the array
elements. You can determine these phase shifts with the `phased.SteeringVector`

object.

For a single carrier frequency, the steering vector for a ULA
consisting of *N* elements is:

$$\left(\begin{array}{c}{e}^{-j2\pi f{\tau}_{1}}\\ {e}^{-j2\pi f{\tau}_{2}}\\ {e}^{-j2\pi f{\tau}_{3}}\\ .\\ .\\ .\\ {e}^{-j2\pi f{\tau}_{N}}\end{array}\right)$$

where τ_{n} denotes the time delay
relative to the array phase center at the n-th array element.

Compute the steering vector for a 4-element ULA at an operating frequency of 1 GHz. Assume that the waveform is incident on the array from 45° azimuth and 10° elevation.

**Note:** This example runs only in R2016b or later. If you are using an earlier release, replace each call to the function with the equivalent `step`

syntax. For example, replace `myObject(x)`

with `step(myObject,x)`

.

```
fc = 1e9;
array = phased.ULA(4);
steervec = phased.SteeringVector('SensorArray',array);
sv = steervec(fc,[45;10])
```

sv = -0.0495 + 0.9988i -0.8742 + 0.4856i -0.8742 - 0.4856i -0.0495 - 0.9988i

You can also compute the steering vector with the following equivalent code.

```
delay = phased.ElementDelay('SensorArray',array);
tau = delay([45;10]);
exp(-1i*2*pi*fc*tau)
```

ans = -0.0495 + 0.9988i -0.8742 + 0.4856i -0.8742 - 0.4856i -0.0495 - 0.9988i

To obtain the array response, which is a weighted-combination
of the steering vector elements for each incident angle, use the `phased.ArrayResponse`

System
object™.

Construct a four-element ULA with elements spaced at 0.25 m. Obtain the array magnitude response (absolute value of the complex-valued array response) for azimuth angles *(-180:180)* at 1 GHz. Then, plot the normalized magnitude response in dB.

**Note:** This example runs only in R2016b or later. If you are using an earlier release, replace each call to the function with the equivalent `step`

syntax. For example, replace `myObject(x)`

with `step(myObject,x)`

.

fc = 1e9; array = phased.ULA('NumElements',4,'ElementSpacing',0.25); azangles = -180:180; response = phased.ArrayResponse('SensorArray',array); resp = abs(response(fc,azangles)); plot(azangles,mag2db((resp/max(resp)))) grid on title('Azimuth Cut at Zero Degrees Elevation') xlabel('Azimuth Angle (degrees)')

Visualize the array response using the `pattern`

method. Create a 3-D plot of the response in *UV* space; other plotting options are available.

pattern(array,fc,[-1:.01:1],[-1:.01:1],'CoordinateSystem','uv',... 'PropagationSpeed',physconst('Lightspeed'))

You can simulate the effects of phase shifts across your array
using the `collectPlaneWave`

method of any array System
object.

The `collectPlaneWave`

method modulates input
signals by the element of the steering vector corresponding to an
array element. Stated differently, `collectPlaneWave`

accounts
for phase shifts across elements in the array based on the angle of
arrival. However, `collectPlaneWave`

does not account
for the response of individual elements in the array.

Simulate the reception of a 100-Hz sine wave modulated by a carrier frequency of 1 GHz at a 4-element ULA. Assume the angle of arrival of the signal is *(-90;0)*.

**Note:** This example runs only in R2016b or later. If you are using an earlier release, replace each call to the function with the equivalent `step`

syntax. For example, replace `myObject(x)`

with `step(myObject,x)`

.

array = phased.ULA(4); t = unigrid(0,0.001,0.01,'[)'); x = cos(2*pi*100*t)'; y = collectPlaneWave(array,x,[-90;0],1e9,physconst('LightSpeed'));

The preceding code is equivalent to the following.

```
steervec = phased.SteeringVector('SensorArray',array);
sv = steervec(1e9,[-90;0]);
y1 = x*sv.';
```

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