June 2006
Intermediate to advanced
336 pages
10h 24m
English
Content preview from Demystifying Switched Capacitor Circuits
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Basic MOS Device Physics
9
VHjVd
kTR
RC
out in
on
on s
2
2
0
2
1
2
1
2
4
1
=
(
)
=
+
(
∞
∫
π
ωω
π
ω
))
=⋅
⋅
(
)
∞
∫
2
0
21
d
kTR
RC
RC
on
on s
on s
ω
π
ω
ω
arctan
==
=∞
=
0
ω
kT
C
s
(1.12)
hence the name kT/C noise (sometimes also called the sampling noise). Interestingly,
the total noise power at the output is independent of the actual on-resistance value
(R
on
). This is because when the thermal noise power density is increased with the on-
resistance (R
on
), the noise bandwidth of the fi lter, which is given by
ff
RC RC
ndB
on s on s
== =
−
ππ
π
22
1
2
1
4
3
(1.13)
is decreased with the same magnitude. Specifi cally, the total noise power can be
easily calculated by multiplying the spectral density given by Equati ...
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