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ANT0104 Ultra Wideband Omnidirectional Antenna

Type:ANT0104

Frequency:20MHz~3000MHz

Gain, Typ (dB):≥0 Max. deviation from circularity :±1.5dB(TYP.)

Horizontal radiation pattern:±1.0dB

Polarization:vertical polarization

VSWR: ≤2.5: 1 Impedance, (Ohm):50

Connecter:N-50K

Outline:Unit: φ162×492mm


Product Detail

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Leader-mw Introduction to Ultra Wideband Omnidirectional Antenna

Introducing leader microwave tech.,(leader-mw)new ultra-wideband omnidirectional antenna ANT0104. This powerful antenna is designed to operate over a wide frequency range from 20MHz to 3000MHz, making it suitable for a variety of applications including wireless communications, radar systems and more.

The maximum gain of this antenna is greater than 0dB, and the maximum roundness deviation is ±1.5dB, ensuring reliable and consistent signal transmission. Its performance is further enhanced by a ±1.0dB horizontal radiation pattern, providing excellent coverage in all directions.

ANT0104 has vertical polarization characteristics, making it ideal for applications where vertical transmission is preferred. In addition, the antenna's VSWR ≤2.5:1 and 50 ohm impedance provide optimal impedance matching and minimal signal loss.

Its compact and rugged design makes it suitable for both indoor and outdoor use, and its omnidirectional functionality allows for seamless connectivity in any environment.

Whether you need to increase the signal strength of your wireless network, enhance the performance of your radar system, or simply want to ensure reliable communications over a wide frequency range, the ANT0104 Ultra Wideband Omnidirectional Antenna is the perfect solution.

Leader-mw Specification

ANT0104 20MHz~3000MHz

Frequency Range: 20-3000MHz
Gain, Typ: 0TYP.
Max. deviation from circularity ±1.5dB(TYP.)
Horizontal radiation pattern: ±1.0dB
Polarization: Linear-vertical polarization
VSWR: ≤ 2.5: 1
Impedance: 50 OHMS
Port Connectors: N-Female
Operating Temperature Range: -40˚C-- +85 ˚C
weight 2kg
Surface Color: Green

 

Remarks:

Power rating is for load vswr better than 1.20:1

Leader-mw Environmental Specifications
Operational Temperature -30ºC~+60ºC
Storage Temperature -50ºC~+85ºC
Vibration 25gRMS (15 degrees 2KHz) endurance, 1 hour per axis
Humidity 100% RH at 35ºc, 95%RH at 40ºc
Shock 20G for 11msec half sine wave,3 axis both directions
Leader-mw Mechanical Specifications
Item materials surface
Vertebral body cover 1 5A06 rust-proof aluminum Color conductive oxidation
Vertebral body cover 2 5A06 rust-proof aluminum Color conductive oxidation
antenna vertebral body 1 5A06 rust-proof aluminum Color conductive oxidation
antenna vertebral body 2 5A06 rust-proof aluminum Color conductive oxidation
chain connected epoxy glass laminated sheet
Antenna core Red cooper passivation
Mounting kit 1 Nylon
Mounting kit 2 Nylon
outer cover Honeycomb laminated fiberglass
Rohs compliant
Weight 2kg
Packing Aluminum alloy packing case (customizable)

Outline Drawing:

All Dimensions in mm

Outline Tolerances ± 0.5(0.02)

Mounting Holes Tolerances ±0.2(0.008)

All Connectors: SMA-Female

01041
0104
Leader-mw Test Data
Leader-mw measurement of antenna

For the practical measurement of antenna directivity coefficient D, we define it from the dimension of antenna radiation beam range.

Directivity D is the ratio of the maximum radiated power density P(θ,φ) Max to its mean value P(θ,φ)av on a sphere in the far-field region, and is a dimensionless ratio greater than or equal to 1. The calculation formula is as follows:

image

In addition, directivity D can be calculated by the following formula:

D = 4 PI / Ω _A

In practice, the logarithmic calculation of D is often used to represent the directional gain of an antenna:

D = 10 log ⁡ d

The above directivity D can be interpreted as the ratio of the sphere range (4π rad²) antenna beam range ω _A. For example, if an antenna radiates only to the upper hemispherical space and its beam range is ω _A=2π rad², then its directivity is:

image

If the logarithm of both sides of the above equation is taken, the antenna's directional gain relative to isotropy can be obtained. It should be noted that this gain can only reflect the antenna's directional pattern radiation, in unit of dBi, since transmission efficiency is not considered as the ideal gain. The calculation results are as follows:

3.01 class: : dBi d = 10 log ⁡ 2 material

The antenna gain units are dBi and dBd, where:

DBi: is the gain obtained by the antenna radiation relative to the point source, because the point source has ω _A=4π and the directional gain is 0dB;

DBd: is the gain of antenna radiation relative to half-wave dipole antenna;

The conversion formula between dBi and dBd is:

2.15 class: : dBi 0 DBD material


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