3D Time-of-flight distance measurement with custom - Universität ...
3D Time-of-flight distance measurement with custom - Universität ...
3D Time-of-flight distance measurement with custom - Universität ...
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140 CHAPTER 5<br />
Measured delay in ns<br />
50<br />
40<br />
30<br />
20<br />
10<br />
0<br />
Measured delay Distance error<br />
0 10 20 30 40 50<br />
Delay in ns<br />
Figure 5.23 Phase delay for 736 fW optical power on one pixel (time error:<br />
260 ps rms � <strong>distance</strong> accuracy: 3.84 cm rms). [MCD07].<br />
For this reason we use the setup described in Section 5.2.2 for the phase accuracy<br />
<strong>measurement</strong>s presented below. With an analog delay line (EG&G-ORTEC 425A)<br />
we can delay the optical 20 MHz modulated signal in steps <strong>of</strong> nanoseconds. This<br />
allows different delays <strong>of</strong> the same light power to be measured <strong>with</strong> the<br />
demodulation pixels. As an example, one <strong>measurement</strong> is shown in Figure 5.23.<br />
The time error is converted into an equivalent <strong>distance</strong> error in this figure<br />
(50 ns=7.5 m, 500 ps=7.5 cm). For the optical power <strong>of</strong> 736 fW per pixel, we get an<br />
accuracy <strong>of</strong> 260 picoseconds.<br />
By attenuating the LED light (<strong>with</strong> ND-filters) the optical input power can be varied.<br />
For higher optical power, the <strong>distance</strong> accuracy increases and for lower power it<br />
decreases. This gives the possibility <strong>of</strong> measuring the range accuracy (or time<br />
resolution) versus the optical power received in each pixel. The results <strong>of</strong> these<br />
<strong>measurement</strong>s are shown in Table 5.3 and in Figure 5.24. All <strong>measurement</strong>s have<br />
been performed (1) <strong>with</strong>out averaging and (2) <strong>with</strong> an average over 16 runs.<br />
50<br />
30<br />
10<br />
-10<br />
-30<br />
-50<br />
Accuracy in cm