Christman GeneralizedReceiver: Difference between revisions

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<math>\displaystyle v(t) = Re[g(t) \cdot e^{j\omega_{c}t}]</math>,
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<math>\displaystyle v(t) = Re[g(t) \cdot e^{j\omega_{c}t}]</math>,  where <math>\displaystyle g(t) = x(t) + jy(t)</math>.
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where <math>g(t) = x(t) + jy(t)</math> is the signal to be sent and  <math>\scriptstyle e^{j\omega_{c}t} = \cos{\omega_{c}t} + j\sin{\omega_{c}t}</math> (Euler's identity) shifts the signal in the frequency domain by <math>\omega_{c} = 2 \pi f_{c}</math>.
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Using Euler's identity, <math>\scriptstyle e^{j\omega_{c}t} = \cos{\omega_{c}t} + j\sin{\omega_{c}t}</math>, we are able to re-write the above equation and simplify so to obtain the following relationship:
The above formula can then be rewritten to obtain the following relationship:
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<math>\displaystyle v(t) = Re[(x(t) + jy(t)) \cdot e^{j\omega_{c}t}] = Re[(x(t) + jy(t)) \cdot (\cos{\omega_{c}t} + j\sin{\omega_{c}t}) = x(t)\cos{\omega_{c}t} - y(t)\sin{\omega_{c}t}</math>.
<math>\displaystyle v(t) = Re[g(t) \cdot e^{j\omega_{c}t}] = Re[(x(t) + jy(t)) \cdot (\cos{\omega_{c}t} + j\sin{\omega_{c}t}) = x(t)\cos{\omega_{c}t} - y(t)\sin{\omega_{c}t}</math>.


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To visualize this process, observe the following figure:
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This is why it is necessary to split <math>m(t)</math> into the the two signals <math>x(t) \text{ and } y(t)</math>. As you can also from the above relationship, in order to obtain the appropriate output signal <math>v(t)</math> one must multiply <math>x(t)</math> by a cosine function and <math>y(t)</math> by a negative sine function and then sum the results (this is illustrated in the figure above). In simplified terms and details, this is essentially how the data <math>m(t)</math> is transmitted. The process of receiving the data is very similar, as is described below.
This is why it is necessary to split <math>m(t)</math> into the the two signals <math>x(t) \text{ and } y(t)</math>. As you can also from the above relationship, in order to obtain the appropriate output signal <math>v(t)</math> one must multiply <math>x(t)</math> by a cosine function and <math>y(t)</math> by a negative sine function and then sum the results (this is illustrated in the figure above). In simplified terms and details, this is essentially how the data <math>m(t)</math> is transmitted. The process of receiving the data is very similar, as is described below.
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<center>[[Image:HW2_GenRec.jpg]]</center>
<center>[[Image:HW2_GenRec.jpg]]</center>

Revision as of 09:10, 6 April 2010

How It Works: Generalized Receiver


The process of transmitting data, m(t), via a wireless signal, v(t), is shown below:


As can be seen from the figure above, in order to transmit m(t), one must first process the data using a baseband processor (usually accomplished with software). As a result of this process the original data will be split into two signals, x(t) and y(t). Why is this you ask? In the world of "Communication Systems" a signal to be transmitted can be written as

v(t)=Re[g(t)ejωct],


where g(t)=x(t)+jy(t) is the signal to be sent and ejωct=cosωct+jsinωct (Euler's identity) shifts the signal in the frequency domain by ωc=2πfc.
The above formula can then be rewritten to obtain the following relationship:

v(t)=Re[g(t)ejωct]=Re[(x(t)+jy(t))(cosωct+jsinωct)=x(t)cosωcty(t)sinωct.

To visualize this process, observe the following figure:
This is why it is necessary to split m(t) into the the two signals x(t) and y(t). As you can also from the above relationship, in order to obtain the appropriate output signal v(t) one must multiply x(t) by a cosine function and y(t) by a negative sine function and then sum the results (this is illustrated in the figure above). In simplified terms and details, this is essentially how the data m(t) is transmitted. The process of receiving the data is very similar, as is described below.