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3D Time-of-flight distance measurement with custom - Universität ...

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OPTICAL TOF RANGE MEASUREMENT 29<br />

A 0<br />

P opt<br />

f=20 MHz, T=50 ns<br />

∆t<br />

A 1 A 2 A 3 A 0<br />

Figure 2.7 Optical sinusoidally modulated input signal, sampled <strong>with</strong> 4 sampling<br />

points per modulation period. The signal frequency <strong>of</strong> 20MHz defines<br />

the unambiguous <strong>distance</strong> range <strong>of</strong> 7.5 m.<br />

These general equations are simplified for our application, where we use a<br />

sinusoidal wave (only base frequency, no harmonics) as the modulation signal and<br />

synchronously sample this wave <strong>with</strong> four equally spaced sampling points <strong>of</strong><br />

duration ∆t. The optical input signal is illustrated in Figure 2.7. We can thus rewrite<br />

the above equations to:<br />

Phase ϕ, amplitude A and <strong>of</strong>fset B <strong>of</strong> a sinusoidal signal obtained by the four<br />

sampling points A0..A3:<br />

A3<br />

− A1<br />

ϕ = atan<br />

A0<br />

− A<br />

Equation 2.17<br />

2<br />

( A − A )<br />

2<br />

δ 3 1 + ( A0<br />

− A2<br />

)<br />

A = ⋅<br />

Equation 2.18<br />

∆t<br />

⋅ sin δ<br />

2<br />

2<br />

A0<br />

+ A1<br />

+ A2<br />

+ A3<br />

B = Equation 2.19<br />

4 ⋅ ∆t<br />

Using DFT, the finite number N <strong>of</strong> sampling points only allows the determination <strong>of</strong><br />

a finite number <strong>of</strong> N/2-1 discrete frequency components. For this case (N=4), the<br />

system is only sensitive to one discrete frequency. Since this frequency selectivity<br />

is a well-known property <strong>of</strong> lock-in amplifiers, we also call the demodulation pixels<br />

lock-in pixels.<br />

B<br />

A<br />

t

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