Antenna Radiation Pattern Visualizer Back
Electromagnetics

Antenna Radiation Pattern Visualizer

Visualize radiation patterns of half-wave dipole, monopole, patch, and Yagi-Uda antennas on a polar chart in real time. Automatically calculates directivity, HPBW, and front-to-back ratio.

Antenna Settings
Results
Results
Directivity (dBi)
HPBW (°)
F/B Ratio (dB)
Gain (dBi)
Polar
Theory & Key Formulas

$$F(\theta) = \frac{\cos\!\left(\frac{\pi}{2}\cos\theta\right)}{\sin\theta}$$

半波長ダイポールの放射パターン。θ=0°(アンテナ軸)で0、θ=90°(赤道面)で最大

$$D = \frac{4\pi U_{\max}}{P_{\text{rad}}} \quad [\text{dBi}]$$

指向性 D:最大放射強度 U_max と全放射電力 P_rad の比。半波長ダイポール ≈ 2.15 dBi

$$P_{\text{EIRP}} = P_{\text{in}} \cdot G$$

等方放射換算電力 EIRP。G:アンテナ利得(線形)、P_in:入力電力 [W]

What is an Antenna Radiation Pattern?

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What exactly is a "radiation pattern"? I hear it's like a 3D map of where an antenna sends its signal, but how do we visualize it?
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Basically, it's a graphical representation of how the antenna radiates energy into space. In practice, we take a 2D "slice" of this 3D shape. Try changing the "Display Plane" control in the simulator above from XY to XZ. You'll see the pattern rotate, giving you different views of the same 3D shape, much like looking at a globe from the top or the side.
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Wait, really? So the pattern changes with the antenna type? What's the big difference between the "Dipole" and "Yagi-Uda" options up there?
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Great observation! A simple dipole spreads energy fairly broadly. A Yagi-Uda antenna, which you can select, uses multiple elements to focus energy into a much tighter beam, like a flashlight versus a lightbulb. The simulator shows this dramatically—the Yagi's pattern has deep nulls and a sharp main lobe, which is why it has higher directivity.
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Okay, and what does the "Ground Plane" toggle do? It seems to change the monopole pattern a lot.
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Exactly! A monopole, like on a car, needs a conductive ground to act as a mirror, creating the other half of the dipole. Flip the "Ground Plane" on and off. With it on, the pattern gets squeezed upward, which is perfect for communicating with things on the horizon, not into the ground. This is a key design choice in real antennas.

Physical Model & Key Equations

The radiation pattern is derived from the electromagnetic fields radiated by currents on the antenna. A fundamental model is the field from a Hertzian dipole (a very short current element), which forms the building block for more complex antennas.

$$E_\theta = j \frac{\eta I_0 \ell}{2 \lambda r}\sin\theta \, e^{-jkr}$$

Where $E_\theta$ is the far-field electric field strength, $\eta$ is the impedance of free space (~377 Ω), $I_0$ is the current, $\ell$ is the dipole length, $\lambda$ is the wavelength, $r$ is the distance, $\theta$ is the angle from the antenna axis, and $k$ is the wave number. The $\sin\theta$ term defines the classic "doughnut" shape.

A key performance metric is Directivity ($D$), which compares the antenna's maximum radiation intensity to that of an isotropic radiator (which radiates equally in all directions). It's often expressed in decibels as dBi.

$$D = \frac{4\pi}{\Omega_A}\quad \text{or}\quad D_{\text{(dBi)}}= 10 \log_{10}(D)$$

Here, $\Omega_A$ is the beam solid angle—the area of the radiation pattern's main lobe. A higher directivity means a more focused beam. The simulator calculates this for each antenna type; for example, a half-wave dipole has $D \approx 2.15$ dBi.

Frequently Asked Questions

This is because the current distribution on the antenna follows a sinusoidal waveform. Along the antenna axis (θ=0,π), the radio waves from each infinitesimal current cancel each other out, resulting in zero intensity. In the equatorial plane (θ=π/2), they reinforce in phase, reaching a maximum. The formula F(θ)=cos(π/2 cosθ)/sinθ represents this shape.
The software automatically calculates the angle where the power drops to half (-3 dB) from the maximum radiation direction on the graph and displays the numerical value on the screen. For a half-wave dipole, the theoretical value is approximately 78°. After changing parameters, it is recalculated in real time, so you can check it immediately.
A patch antenna is flat and has a single main beam toward the zenith, with an HPBW of about 60–90°. A Yagi-Uda antenna features directors and a reflector, offering high directivity (HPBW 30–50°) and a front-to-back ratio (10 dB or more). Choose according to your application.
From the 'Export' button at the top right of the screen, you can save the polar plot as a PNG image. Additionally, numerical values for directivity, HPBW, and front-to-back ratio can be copied from the automatic calculation field. The graph's color scheme and line type can be changed in the settings menu.

Real-World Applications

Mobile Communication Base Stations: The panels on cell towers often use patch antennas, which you can select in the simulator. Their relatively broad, hemispherical pattern is ideal for covering users on the ground in a sector below the tower. Engineers use pattern visualizations to minimize dead zones.

Television Reception: The classic rooftop Yagi-Uda antenna is designed for high directivity. Its sharp radiation pattern, visible when you select it in the tool, allows it to be precisely aimed at a distant broadcast tower to maximize signal strength and reject interference from other directions.

Aviation & Maritime: Monopole antennas with a ground plane are ubiquitous on ships and aircraft. The pattern you see with "Ground Plane" enabled—radiating efficiently along the horizon—is crucial for long-range communication over water or between air traffic control and planes.

Wi-Fi Routers: Modern routers often use dipole-like antennas or antenna arrays. The radiation pattern determines coverage within a home. A pattern that is too focused might leave dead spots, while an omnidirectional one (like a dipole's XY-plane view) provides general coverage in all horizontal directions.

Common Misconceptions and Points to Note

There are a few key points you should be especially mindful of when starting to use this tool. The first is that the radiation pattern also represents receiving characteristics. While the visualization shows "transmission strength," antenna characteristics are reciprocal between transmission and reception (the reciprocity theorem). Therefore, a narrow, elongated pattern not only means it "can transmit far" but also that it "can effectively pick up weak radio waves from a distance." The second point is confusion between "dBi" and "dBd". The "Directivity (dBi)" displayed by the tool uses a hypothetical omnidirectional antenna (isotropic antenna) as the 0dB reference. In practice, "dBd," which uses a half-wave dipole as the 0dB reference, is also commonly used. For example, this tool shows the gain of a half-wave dipole as approximately 2.15 dBi, but in dBd, that's about 0 dBd. Pay close attention to this difference when reading catalog values. The third point is the gap between simulation and real devices. This tool shows the characteristics of the "antenna alone" in an ideal environment (free space). In reality, the pattern distorts due to the influence of nearby metal objects (supports, roofs) or the ground. For instance, turning the "ground plane" OFF for a monopole will display a pattern for the lower half that doesn't exist in reality; for an actual vehicle-mounted antenna, the car body acts as the ground, significantly altering the pattern.

How to Use

  1. Select antenna type from dropdown (dipole, monopole, patch, or Yagi-Uda)
  2. Adjust frequency (300 MHz to 6 GHz) and physical dimensions (element length, spacing, substrate height)
  3. Toggle between polar and rectangular plot views; radiation pattern updates in real time
  4. Read directivity (dBi), gain, and 3dB beamwidth values in the metrics panel
  5. Export polar data as CSV for MATLAB or antenna design software integration

Worked Example

A half-wave dipole antenna at 2.4 GHz (λ = 125 mm) with element length 62.5 mm exhibits maximum radiation perpendicular to its axis. Directivity = 1.64 dBi, front-to-back ratio = 3.2 dB, 3dB beamwidth = 78 degrees in azimuth. A Yagi-Uda array with 1 driven element + 4 directors (spacing 0.3λ) at 915 MHz achieves 9.2 dBi directivity with 65-degree main lobe and 18 dB side lobe suppression. Patch antenna on FR-4 substrate (h = 1.6 mm, εr = 4.3) at 5.8 GHz yields 5.1 dBi gain with elliptical radiation pattern tilted 12 degrees from normal.

Practical Notes

  1. Monopole radiation is half-space pattern; subtract 3 dB from dipole directivity when ground plane height < 0.5λ
  2. Yagi spacing optimization: directors at 0.2–0.3λ separation improve gain; reflector positioned 0.15λ behind driven element
  3. Patch antennas exhibit substrate coupling losses above εr = 6; cross-check simulated gain against measured S11 and efficiency
  4. Industrial ISM band design (915 MHz, 2.4 GHz, 5.8 GHz) requires directivity trade-off with bandwidth; use rectangular plot zoom to verify null steering