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Electronic Noise Time vs frequency domain noises

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Presentation on theme: "Electronic Noise Time vs frequency domain noises"— Presentation transcript:

1 Electronic Noise Time vs frequency domain noises
Noise present in devices Noise propagation in filters

2 Noise in time domain

3 dBm is a unit used to measure physical power relative to 1 mW.
For example, if 2V is applied to 50, the physical power is: P= 2^2/50 W = 4/50 W = 4*20 mW P (dBm) = 10log(P/1mW) = 10log(80) = 10log(2^3*10) = 3* =19.03 dBm

4 Area For a given v(t), define: vf(t) v(t)
The power spectral density of v is: Pv(f) = power of vf(t) = power of v(t) in a one Hertz bandwidth at f The total power of v can be obtained by integrating Pv(f) over all f. Pv(f) Pv = 10*1M + 0.5*10*1M = 15M (uV)2=15(mV)2 10(uV)2/Hz Area 1MHz 2MHz

5 If the power spectral density of vn is flat (ind of f), vn is called white.
vn(t) Pvn(f)

6 dBm or dBV2 Slope: 10dB/dec log(f)

7 1/f noise corner: the intersection of 1/f noise power spectral density and white noise power spectral density dBm or dBV2 Slope: 10dB/dec 1/f noise corner log(f)

8 Looks like signal + noise
Filtered noise: Time domain: Looks like signal + noise Spectral domain: Noisy filter shape

9 Example: white noise filtered by integrator
-20dB/dec

10 Filtered noise: Chapter 9 Figure 06 Chapter 9 Figure 07

11 What’s the total power of white noise?
P = Pn(f)*BW = infinity P White noise does not exist physically! Physical “white” noise are filtered by LP/BP filters.

12 What’s the total power of 1/f noise?
goes to infinity if f2  inf or f1  0 Slope: -10dB/dec k/f f2 f1 Hence need BP filtering

13 Equivalent noise bandwidth of a filter = the bandwidth of an ideal filter allowing the same amount of noise to pass through. Chapter 9 Figure 09 -3dB BW Noise in this band can still pass through -3dB BW noise BW

14 Device noise Capacitors do not generate noise
Inductors do not generator noise Resistors generate white thermal noise Active devices generate multiple kinds of noise

15

16 Chapter 9 Figure 12

17 Chapter 9 Figure 13 Regardless how complicated the network is, as long as all C’s can be reduced to Ceq, total voltage noise power on Ceq is kT/Ceq

18 Rs L Rs L Vs VRs iL Regardless how complicated the network is, as long as all L’s can be reduced to Leq, total current noise power through Leq is kT/Leq

19 Sampling noise The switch may be sized differently, the switch’s on resistance value may differ, the on resistance value may change with Vin levels, but voltage noise power of sampled value in cap is kT/C


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