Graphics Programs Reference
In-Depth Information
N o
N i
F dB
=
10
log
---------------
(1B.5)
A p
where
and
are, respectively, the noise power at the output and input of
N o
N i
the system.
If we define the input and output signal power by
and
, respectively,
S i
S o
then the power gain is
S o
S i
A P
=
-----
(1B.6)
It follows that
S i
Ni
S i
N i
S o
N o
---- 
dB
----- 
dB
----------------
F dB
=
10
log
=
–
(1B.7)
S o
N o
where
S i
N i
S o
N o
---- 
dB
----- 
dB
>
(1B.8)
Thus, it can be said that the noise figure is the loss in the signal-to-noise ratio
due to the added thermal noise of the amplifier
.
(
(
SNR
) o
=
(
SNR
) i
–
FindB
)
We can also express the noise figure in terms of the systemÓs effective tem-
perature . Consider the amplifier shown in Fig. 1B.2 , and let its effective
temperature be
T e
. Assume the input noise temperature is
. Thus, the input
T e
T o
noise power is
N i
=
kT o B
(1B.9)
and the output noise power is
N o
=
kT o BA p
+
kT e BA p
(1B.10)
where the first term on the right-hand side of Eq. (1B.10) corresponds to the
input noise, and the latter term is due to thermal noise generated inside the sys-
tem. It follows that the noise figure can be expressed as
S i
kT o B
T o
+
S o
T e
(
SNR
) i
T e
T o
------------
-----------------
F
=
------------------
=
kBA p
=
1
+
-----
(1B.11)
(
SNR
) o
Equivalently, we can write
T e
=
(
F
–
1
) T o
(1B.12)
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