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Model 1835-C - Newport Corporation

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3.8 Integration of Detector Signals<br />

The <strong>Model</strong> <strong>1835</strong>-C provides for making measurements that integrate incoming<br />

power detector signals to obtain an energy via the INTG mode, Section 2.3.12.<br />

In INTG mode, the display units indicate Joules since energy is the time<br />

integral of power:<br />

t1<br />

E λ P λ dt<br />

t0<br />

t1<br />

( )= ∫ ( ) = ∫<br />

t0<br />

()<br />

( )<br />

St<br />

R λ<br />

As the detector signal actually consists of a stream of digitized values, the<br />

integral becomes a numerical approximation using the trapezoid method,<br />

Figure 15. In order to maintain the highest accuracy for this numerical<br />

process, the sample rate is set at its maximum value of 500 Hz.<br />

dt<br />

Detector Signal<br />

Numerical Integration<br />

Trapezoid Method<br />

Magnitude of the<br />

Integraged Result<br />

Figure 15. Integrated Energy Via a Trapezoid Approximation — The INTG<br />

measurement mode performs a discrete integration at a 500 Hz sample rate.<br />

Two common applications are natural extensions of the INTG measurement<br />

mode:<br />

1. Pulse laser energy measurement using with a thermopile detector,<br />

Section 3.5<br />

2. Energy from exposure over a period of time (dosage), Section 3.6.<br />

33

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