Update Content - 2022-08-24
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@@ -43,9 +43,9 @@ This approach allows frequency dependent error budgeting, which is why it is ref
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#### Ground vibrations {#ground-vibrations}
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#### Electronic Noise {#electronic-noise}
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#### [Electronic Noise]({{< relref "electronic_noise.md" >}}) {#electronic-noise--electronic-noise-dot-md}
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**Thermal Noise** (or Johson noise).
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**Thermal Noise** (or Johnson noise).
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This noise can be modeled as a voltage source in series with the system impedance.
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The noise source has a PSD given by:
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\\[ S\_T(f) = 4 k T \text{Re}(Z(f)) \ [V^2/Hz] \\]
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@@ -65,7 +65,7 @@ with \\(q\_e\\) the electronic charge (\\(1.6 \cdot 10^{-19}\\, [C]\\)), \\(i\_{
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<div class="exampl">
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An averable current of 1 A will introduce noise with a STD of \\(10 \cdot 10^{-9}\\,[A]\\) from zero up to one kHz.
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A current of 1 A will introduce noise with a STD of \\(10 \cdot 10^{-9}\\,[A]\\) from zero up to one kHz.
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</div>
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