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	<title>Chain-growth polymerization - Revision history</title>
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	<updated>2026-06-01T00:03:48Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<title>137.122.205.68: /* Comparison with other polymerization methods */</title>
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		<updated>2014-08-27T19:44:34Z</updated>

		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;Comparison with other polymerization methods&lt;/span&gt;&lt;/p&gt;
&lt;a href=&quot;https://en.formulasearchengine.com/index.php?title=Chain-growth_polymerization&amp;amp;diff=310557&amp;amp;oldid=9297&quot;&gt;Show changes&lt;/a&gt;</summary>
		<author><name>137.122.205.68</name></author>
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	<entry>
		<id>https://en.formulasearchengine.com/index.php?title=Chain-growth_polymerization&amp;diff=9297&amp;oldid=prev</id>
		<title>en&gt;Christian75: Clean up using AWB</title>
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		<updated>2013-09-02T12:42:57Z</updated>

		<summary type="html">&lt;p&gt;Clean up using &lt;a href=&quot;/index.php?title=Testwiki:AWB&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Testwiki:AWB (page does not exist)&quot;&gt;AWB&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;[[File:PSK BER curves.svg|thumb|right|280px|[[Bit-error rate]] (BER) vs &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; curves for different [[digital modulation]] methods is a common application example of &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;. Here an [[AWGN]] channel is assumed.]]&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;&amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;&amp;#039;&amp;#039;&amp;#039; (the &amp;#039;&amp;#039;&amp;#039;energy per bit to noise power spectral density ratio&amp;#039;&amp;#039;&amp;#039;) is an important parameter in [[digital communication]] or [[data transmission]]. It is a normalized [[signal-to-noise ratio]] (SNR) measure, also known as the &amp;quot;SNR per bit&amp;quot;. It is especially useful when comparing the [[bit error rate]] (BER) performance of different digital [[modulation]] schemes without taking bandwidth into account. &lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; is equal to the SNR divided by the &amp;quot;gross&amp;quot; [[link spectral efficiency]] in [[(bit/s)/Hz]], where the bits in this context are transmitted data bits, inclusive of error correction information and other protocol overhead. When [[forward error correction]] (FEC) is being discussed, &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; is routinely used to refer to the energy per information bit (i.e. the energy per bit net of FEC overhead bits); in this context, E&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt;/N&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; is generally used to relate actual transmitted power to noise.&amp;lt;ref&amp;gt;&lt;br /&gt;
{{cite book&lt;br /&gt;
 | title = Turbo coding&lt;br /&gt;
 | edition = &lt;br /&gt;
 | author = Chris Heegard and Stephen B. Wicker&lt;br /&gt;
 | publisher = Kluwer&lt;br /&gt;
 | year = 1999&lt;br /&gt;
 | isbn = 978-0-7923-8378-9&lt;br /&gt;
 | page = 3&lt;br /&gt;
 | url = http://books.google.com/books?id=aTWkPD_COsoC&amp;amp;pg=PA3&lt;br /&gt;
 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The [[noise spectral density]] &amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;, usually expressed in units of [[watt]]s per [[hertz]], can also be seen as having dimensions of energy, or units of [[joule]]s, or joules per cycle.  &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; is therefore a non-dimensional ratio.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; is commonly used with modulation and coding designed for noise-limited rather than interference-limited communication, since additive white noise (with constant noise density &amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;) is assumed. &lt;br /&gt;
&lt;br /&gt;
==Relation to carrier-to-noise ratio==&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; is closely related to the [[carrier-to-noise ratio]] (CNR or C/N), i.e. the [[signal-to-noise ratio]] (SNR) of the received signal, after the receiver filter but before detection:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;C/N=E_b/N_0\cdot\frac{f_b}{B}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
:&amp;#039;&amp;#039;f&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; is the channel data rate ([[net bitrate]]), and&lt;br /&gt;
:&amp;#039;&amp;#039;B&amp;#039;&amp;#039; is the channel bandwidth&lt;br /&gt;
&lt;br /&gt;
The equivalent expression in logarithmic form (dB):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\text{CNR}_{\text{dB}} = 10\log_{10}(E_b/N_0) + 10\log_{10}\left(\frac{f_b}{B}\right)&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
Caution: Sometimes, the noise power is denoted by &amp;lt;math&amp;gt;N_0/2&amp;lt;/math&amp;gt; when negative frequencies and complex-valued equivalent [[baseband]] signals are considered rather than [[passband]] signals, and in that case, there will be a 3 dB difference.&lt;br /&gt;
&lt;br /&gt;
==Relation to &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; can be seen as a normalized measure of the &amp;#039;&amp;#039;&amp;#039;energy per symbol to noise power spectral density&amp;#039;&amp;#039;&amp;#039; (&amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;): &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{E_b}{N_0} =\frac{E_s}{\rho N_0}&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
where &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt; is the energy per symbol in joules and &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; is the nominal [[spectral efficiency]] in (bit/s)/Hz.&amp;lt;ref&amp;gt;{{Cite web | last = Forney | first = David | title = MIT OpenCourseWare, 6.451 Principles of Digital Communication II, Lecture Notes section 4.2  | url=http://ocw.mit.edu/ | accessdate = 21 September 2010 }}&amp;lt;/ref&amp;gt; &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; is also commonly used in the analysis of digital modulation schemes. The two quotients are related to each other according to the following:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{E_s}{N_0} =\frac{E_b}{N_0}\log_2 M &amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
where &amp;#039;&amp;#039;M&amp;#039;&amp;#039; is the number of alternative modulation symbols.&lt;br /&gt;
&lt;br /&gt;
Note that this is the energy per bit, not the energy per information bit.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; can further be expressed as:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{E_s}{N_0} = \frac{C}{N}\frac{B}{f_s}&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
:&amp;#039;&amp;#039;C/N&amp;#039;&amp;#039; is the [[carrier-to-noise ratio]] or [[signal-to-noise ratio]].&lt;br /&gt;
:&amp;#039;&amp;#039;B&amp;#039;&amp;#039; is the channel bandwidth in hertz.&lt;br /&gt;
:&amp;#039;&amp;#039;f&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt; is the symbol rate in [[baud]] or symbols per second.&lt;br /&gt;
&lt;br /&gt;
==Shannon limit==&lt;br /&gt;
{{main | Shannon–Hartley theorem}}&lt;br /&gt;
&lt;br /&gt;
The [[Shannon–Hartley theorem]] says that the limit of reliable [[information rate]] (data rate exclusive of error-correcting codes) of a channel depends on bandwidth and signal-to-noise ratio according to:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; I &amp;lt; B \log_2 \left( 1+\frac{S}{N} \right) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
:&amp;#039;&amp;#039;I&amp;#039;&amp;#039; is the [[information rate]] in [[bits per second]] excluding [[error-correcting code]]s;&lt;br /&gt;
:&amp;#039;&amp;#039;B&amp;#039;&amp;#039; is the [[Bandwidth (signal processing)|bandwidth]] of the channel in [[hertz]];&lt;br /&gt;
: &amp;#039;&amp;#039;S&amp;#039;&amp;#039; is the total signal power (equivalent to the carrier power &amp;#039;&amp;#039;C&amp;#039;&amp;#039;); and&lt;br /&gt;
: &amp;#039;&amp;#039;N&amp;#039;&amp;#039; is the total noise power in the bandwidth.&lt;br /&gt;
&lt;br /&gt;
This equation can be used to establish a bound on E&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/N&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; for any system that achieves reliable communication, by considering a gross bit rate &amp;#039;&amp;#039;R&amp;#039;&amp;#039; equal to the net bit rate &amp;#039;&amp;#039;I&amp;#039;&amp;#039; and therefore an average energy per bit of &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; = &amp;#039;&amp;#039;S/R&amp;#039;&amp;#039;, with noise spectral density of &amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; = &amp;#039;&amp;#039;N/B&amp;#039;&amp;#039;.  For this calculation, it is conventional to define a normalized rate &amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;l&amp;lt;/sub&amp;gt; = &amp;#039;&amp;#039;R/&amp;#039;&amp;#039;2&amp;#039;&amp;#039;B&amp;#039;&amp;#039;, a bandwidth utilization parameter of bits per second per half hertz, or bits per dimension (a signal of bandwidth &amp;#039;&amp;#039;B&amp;#039;&amp;#039; can be encoded with 2&amp;#039;&amp;#039;B&amp;#039;&amp;#039; dimensions, according to the [[Nyquist–Shannon sampling theorem]]).  Making appropriate substitutions, the Shannon limit is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; {R \over B} = 2 R_l &amp;lt; \log_2 \left( 1 + 2R_l\frac{E_b}{N_0} \right) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Which can be solved to get the Shannon-limit bound on &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{E_b}{N_0} &amp;gt; \frac{2^{2R_l}-1}{2R_l}  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
When the data rate is small compared to the bandwidth, so that &amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;l&amp;lt;/sub&amp;gt; is near zero, the bound, sometimes called the &amp;#039;&amp;#039;ultimate Shannon limit&amp;#039;&amp;#039;,&amp;lt;ref&amp;gt;{{cite book | title = Algorithms for Communications Systems and Their Applications | author = Nevio Benvenuto and Giovanni Cherubini | year = 2002 | page = 508 | publisher = John Wiley &amp;amp; Sons | isbn = 0-470-84389-6}}&amp;lt;/ref&amp;gt; is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{E_b}{N_0} &amp;gt; \ln(2)  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
which corresponds to –1.59 dB because:&lt;br /&gt;
:&amp;lt;math&amp;gt;ln(2) = 0.693&amp;lt;/math&amp;gt; and &lt;br /&gt;
:&amp;lt;math&amp;gt;10log(0.693) = -1.59 dB&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
However, [[spread spectrum]] allows negative signal-to-noise ratio  before despreading, since the bandwidth is much higher than the bit rate.&lt;br /&gt;
&lt;br /&gt;
==Cutoff rate==&lt;br /&gt;
&lt;br /&gt;
For any given system of coding and decoding, there exists what is known as a &amp;#039;&amp;#039;cutoff rate&amp;#039;&amp;#039; &amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;, typically corresponding to an &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; about 2 dB above the Shannon capacity limit. {{Citation needed|date=April 2009}}The cutoff rate used to be thought of as the limit on practical [[error correction codes]] without an unbounded increase in processing complexity,&lt;br /&gt;
but has been rendered largely obsolete by the more recent discovery of [[turbo codes]] or by the LDPC (Low Density Parity Check) codes.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
*[http://www.sss-mag.com/ebn0.html Eb/N0 Explained.] An introductory article on &amp;#039;&amp;#039;E&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt;/&amp;#039;&amp;#039;N&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{Noise}}&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Eb-N0}}&lt;br /&gt;
[[Category:Noise]]&lt;br /&gt;
[[Category:Signal processing]]&lt;br /&gt;
[[Category:Engineering ratios]]&lt;/div&gt;</summary>
		<author><name>en&gt;Christian75</name></author>
	</entry>
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