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100mJ Laser Target Designator

100mJ Laser Target Designator

Model: SUK:LDR1064-100

Short Description:

The LDR1064-100 medium laser photometer (hereinafter referred to as the laser photometer) is a precision photoelectric product which transmits the laser to a specific target and calculates the distance information according to the laser flight time. It has the characteristics of outstanding performance and simple operation. The laser photometer belongs to the eye safety products, through the serial communication.


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Technical Parameter

Product Tags

TECHNICAL SPECIFICATIONS

Wavelength

1.064μm

Output energy

total temperature: 100mJ ~ 120mJ, average output energy ≥110mJ, single pulse energy > 100mJ (2 seconds before removal)

Adjacent pulse energy fluctuation range

≤8%

Beam dispersion Angle

0.15mrad (the acceptance method adopts hole-hole method, and the ratio of hole-hole to hole-free is not less than 86.5%)

Spatial pointing instability of beam

≤0.03mrad (1σ)

Irradiation frequency

accurate coding 45ms~56ms (check code 20Hz)

Pulse cycle accuracy

≤±2.5μs

Pulse width

15ns±5ns

Irradiation time

no less than 90s, interval 60s, or no less than 60s, interval 30s, 4 cycles of continuous irradiation at room temperature and low temperature, 2 cycles of continuous irradiation at high temperature

Ranging range

the minimum value is not more than 300m, the maximum is not less than 35km (23km visibility, medium atmospheric turbulence, for 2.3m×2.3m target, target reflection coefficient is greater than 0.2)

Irradiation distance

for 2.3m×2.3m target, not less than 16km

Normal temperature power-up preparation time

<30 seconds

Low temperature power-up preparation time

<3 minutes

Service life

≥2 million times

Ranging counting range

200m ~ 40km

Ranging accuracy

 ±2m

Accurate measurement rate

 ≥98%

Ranging frequency

1Hz, 5Hz, 10Hz, 20Hz

Installation datum and laser transmission optical axis of non-parallel

≤0.5mrad

Installation datum flatness

0.01mm (design guarantee)

Insulation resistance

under standard atmospheric pressure, the insulation resistance value of the specified measuring point should conform to the provisions of Table 1

 

Table 1 specifies the insulation resistance values of the measuring points

Serial number

Environmental conditions

Insulation resistance

Megohm meter output voltage

1

Standard atmospheric conditions

20 m Ω or greater

100V

u External logo (including product number) should be fixed firmly, clear, complete and easy to identify.

 

PRINCIPLE OF RANGING

 

After the laser imager is started, the laser pulse with a periodic frequency of 1Hz is emitted, which reaches the measured target through the transmitting antenna. Most of the beam is absorbed or diffusely reflected by the target, while a very small part of the beam returns to the receiving antenna and converges on the detector module. The detector module samples the reflected signal and obtains the distance information of the measured target through an algorithm.

Examples of calculation:

Measurement time (one round trip) =10us

Propagation time (one way) =10us/2=5us

Ranging distance = Light speed × travel time =300000km/s×5us=1500m

 

 RANGING CAPABILITY IN DIFFERENT VISIBITY

 

Atmospheric visibility has a great impact on the ranging performance of laser photometer. Please refer to Figure 2 for the ranging capability of this product in different visibility.

 

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Figure 2  The relationship between the ranging ability of laser photometer and atmospheric visibility

 HUMAN EYE SAFETY

The laser rangefinder uses a laser source in the band of 1064nm. When using the laser in this band, it is necessary to avoid the outgoing beam directly into the human eye as far as possible to prevent human eye injury.

 

MECHICAL INTERFACE

 

The mechanical interface of the laser photometer consists of 3 through holes, which are fixed to the installation platform by 3 M5 screws. The dimensions of the mechanical and optical interfaces are shown in Figure 3 below.

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                                                                                         Figure 3 shows the mechanical and optical interfaces


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