Connexions

You are here: Home » Content » Carrier Frequency Modulation
Content Actions
Lenses

What is a lens?

Lenses

A lens is a custom view of Connexions content. You can think of it as a fancy kind of list that will let you see Connexions through the eyes of organizations and people you trust.

What is in a lens?

Lens makers point to Connexions materials (modules and collections), creating a guide that includes their own comments and descriptive tags about the content.

Who can create a lens?

Any individual Connexions member, a community, or a respected organization.

This content is ...
Affiliated with (?)
This content is either by members of the organizations listed or about topics related to the organizations listed. Click each link to see a list of all content affiliated with the organization.
  • This module is included inLens: Rice University OpenCourseWare
    By: OpenCourseWare ConsortiumAs a part of collection:"Digital Communication Systems"

    Click the "Rice University OCW" link to see all content affiliated with them.

    Rice University OCW
Tags

(?)

These tags come from the endorsement, affiliation, and other lenses that include this content.

Carrier Frequency Modulation

Module by: Behnaam Aazhang

Summary: A method of carrier modulation in which signal information is carried in the carrier frequency of the signal.

Frequency Shift Keying (FSK)

The data is impressed upon the carrier frequency. Therefore, the M M different signals are
s m t=A P T tcos2π f c t+2πm-1Δft+ θ m s m t A P T t 2 f c t 2 m 1 Δ f t θ m (1)
for m12M m 1 2 M
The M M different signals have M M different carrier frequencies with possibly different phase angles since the generators of these carrier signals may be different. The carriers are
f 1 = f c f 1 f c (2)
f 2 = f c +Δf f 2 f c Δ f f M = f c +M-1Δf f M f c M 1 Δ f Thus, the MM signals may be designed to be orthogonal to each other.
< s m , s n >=0TA2cos2π f c t+2πm-1Δft+ θ m cos2π f c t+2πn-1Δft+ θ n dt=A220Tcos4π f c t+2πn+m-2Δft+ θ m + θ n dt+A220Tcos2πm-nΔft+ θ m - θ n dt=A22sin4π f c T+2πn+m-2ΔfT+ θ m + θ n -sin θ m + θ n 4π f c +2πn+m-2Δf+A22sin2πm-nΔfT+ θ m - θ n 2πm-nΔf-sin θ m - θ n 2πm-nΔf s m s n t 0 T A 2 2 f c t 2 m 1 Δ f t θ m 2 f c t 2 n 1 Δ f t θ n A 2 2 t 0 T 4 f c t 2 n m 2 Δ f t θ m θ n A 2 2 t 0 T 2 m n Δ f t θ m θ n A 2 2 4 f c T 2 n m 2 Δ f T θ m θ n θ m θ n 4 f c 2 n m 2 Δ f A 2 2 2 m n Δ f T θ m θ n 2 m n Δ f θ m θ n 2 m n Δ f (3)
If 2 f c T+n+m-2ΔfT 2 f c T n m 2 Δ f T is an integer, and if m-nΔfT m n Δ f T is also an integer, then < S m , S n >=0 S m S n 0 if ΔfT Δ f T is an integer, then < s m , s n >0 s m s n 0 when f c f c is much larger than 1T 1 T .
In case m, θ m =0 m θ m 0
< s m , s n >A2T2sinc2m-nΔfT s m s n A 2 T 2 sinc 2 m n Δ f T (4)
Therefore, the frequency spacing could be as small as Δf=12T Δ f 1 2 T since sincx=0 sinc x 0 if x=±1 x ± 1 or ±2 ± 2 .
If the signals are designed to be orthogonal then the average probability of error for binary FSK with optimum receiver is
P e =Q E s N 0 P e Q E s N 0 (5)
in AWGN.
Note that sincx sinc x takes its minimum value not at x=±1 x ± 1 but at ±1.4 ± 1.4 and the minimum value is -0.216-0.216. Therefore if Δf=0.7T Δ f 0.7 T then
P e =Q1.216 E s N 0 P e Q 1.216 E s N 0 (6)
which is a gain of 10log1.2160.85dθ 10 1.216 0.85 d θ over orthogonal FSK.

Comments, questions, feedback, criticisms?

Send feedback