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	<title>Actuarial polynomials - Revision history</title>
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		<title>en&gt;Headbomb: Various citation cleanup and WP:AWB general fixes, added orphan tag using AWB</title>
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		<updated>2011-09-17T02:55:13Z</updated>

		<summary type="html">&lt;p&gt;Various citation cleanup and &lt;a href=&quot;/index.php?title=WP:AWB&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;WP:AWB (page does not exist)&quot;&gt;WP:AWB&lt;/a&gt; general fixes, added &lt;a href=&quot;/index.php?title=CAT:O&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;CAT:O (page does not exist)&quot;&gt;orphan&lt;/a&gt; tag 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;{{Multiple issues|&lt;br /&gt;
{{cleanup|date=September 2011}}&lt;br /&gt;
{{refimprove|date=September 2011}}&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
{{merge to|Operational amplifier applications|Talk=Talk:Op amp integrator#Merge_proposal|date=December 2012}}&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;operational amplifier integrator&amp;#039;&amp;#039;&amp;#039; is an electronic integration circuit. Based around the [[operational amplifier]] (op-amp), it performs the mathematical operation of [[integration (mathematics)|integration]] with respect to time; that is, its output [[voltage]] is proportional to the input voltage integrated over time.&lt;br /&gt;
&lt;br /&gt;
==Ideal circuit==&lt;br /&gt;
[[File:Integrator circuit.png|Integrator circuit]]&lt;br /&gt;
&lt;br /&gt;
Intuitively, the circuit operates by passing a [[electric current|current]] that charges or discharges the [[capacitor]] over time. If the op-amp is assumed [[Operational amplifier#Ideal op-amps|ideal]], nodes &amp;#039;&amp;#039;v&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;#039;&amp;#039; and &amp;#039;&amp;#039;v&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&amp;#039;&amp;#039; are held equal, and so &amp;#039;&amp;#039;v&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&amp;#039;&amp;#039; is a [[virtual ground]]. The input voltage passes a current &amp;lt;math&amp;gt;\frac{v_{in}}{R_1}&amp;lt;/math&amp;gt; through the [[resistor]] and series capacitor, which charges or discharges the capacitor over time. Because the resistor and capacitor are connected to a virtual ground, the input current does not vary with capacitor charge and a [[linearity|linear]] integration operation is achieved.&lt;br /&gt;
&lt;br /&gt;
The circuit can be analyzed by applying [[Kirchhoff&amp;#039;s current law]] at the node &amp;#039;&amp;#039;v&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&amp;#039;&amp;#039;, keeping ideal op-amp behaviour in mind.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;i_{\text{1}} = I_{\text{B}} + i_{\text{F}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;I_{\text{B}} = 0&amp;lt;/math&amp;gt; in an ideal op-amp, so:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;i_{\text{1}} = i_{\text{F}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Furthermore, the capacitor has a voltage-current relationship governed by the equation:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;I_{\text{C}} = C \frac{dV_{\text{c}}}{dt}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Substituting the appropriate variables:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{v_{\text{in}} - v_{\text{2}}}{R_{\text{1}}} = C_{\text{F}}\frac{d(v_{\text{2}} - v_{\text{o}})}{dt}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;v_2 = v_1 = 0&amp;lt;/math&amp;gt; in an ideal op-amp, resulting in:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{v_{\text{in}}}{R_{\text{1}}} = -C_{\text{F}}\frac{dv_{\text{o}}}{dt}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Integrating both sides with respect to time:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \int_0^t\frac{v_{\text{in}}}{R_{\text{1}}} \ dt\ = - \int_0^t C_{\text{F}} \frac{dv_{\text{o}}}{dt} \, dt&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the initial value of &amp;#039;&amp;#039;v&amp;lt;sub&amp;gt;o&amp;lt;/sub&amp;gt;&amp;#039;&amp;#039; is assumed to be 0 V, this results in a DC error of:&amp;lt;ref name=&amp;quot;microchip-opa-dc&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;v_{\text{o}} = -\frac{1}{R_{\text{1}}C_{\text{F}}}\int_0^t v_{\text{in}}\, dt&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Practical circuit==&lt;br /&gt;
[[File:Practical integrator.png|Practical integrator]]&lt;br /&gt;
&lt;br /&gt;
The ideal integrator seen above is not a practical circuit design. Non-ideal op-amps have a finite [[open-loop gain]], an [[input offset voltage]] and [[input bias current]]s (&amp;lt;math&amp;gt;I_B&amp;lt;/math&amp;gt; in the ideal circuit figure, above). This can cause several issues for the ideal design; most importantly, if &amp;lt;math&amp;gt;v_{\text{in}} = 0&amp;lt;/math&amp;gt;, both the output offset voltage and the input bias current &amp;lt;math&amp;gt;I_B&amp;lt;/math&amp;gt; can cause current to pass through the capacitor, causing the output voltage to drift over time until the op-amp saturates. Similarly, if &amp;lt;math&amp;gt;v_{\text{in}}&amp;lt;/math&amp;gt; were a signal centered about zero volts (i.e. without a [[direct current|DC]] component), no drift would be expected in an ideal circuit, but may occur in a real circuit.&lt;br /&gt;
&lt;br /&gt;
In DC [[steady state]], the capacitor acts as an open circuit. The DC gain of the ideal circuit is therefore infinite (or the open-loop gain of a non-ideal op-amp). A large resistor &amp;lt;math&amp;gt;R_F&amp;lt;/math&amp;gt; can be inserted in parallel with the [[Feedback#Electronic engineering|feedback]] capacitor, as shown in the figure above. This limits the DC gain of the circuit to a finite value, and hence changes the output drift into a finite, preferably small, DC error:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;V_\text{E} = \left( \frac{R_\text{f}}{R_1} + 1 \right) \left( V_{IOS} + I_{BI} \left( R_\text{f} \parallel R_1 \right) \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;V_{IOS}&amp;lt;/math&amp;gt; is the input offset voltage and &amp;lt;math&amp;gt;I_{BI}&amp;lt;/math&amp;gt; is the input bias current on the inverting terminal. &amp;lt;math&amp;gt;R_f \parallel R_1&amp;lt;/math&amp;gt; indicates two resistance values in parallel.&lt;br /&gt;
&lt;br /&gt;
To negate the effect of the input bias current, set &amp;lt;math&amp;gt;R_{\text{on}}=R_1 || R_f || R_L&amp;lt;/math&amp;gt;. The error voltage then becomes:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;V_\text{E} = \left( \frac{R_\text{f}}{R_1} + 1 \right) V_{IOS}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The input bias current causes the same voltage drops at both the positive and negative terminals.&lt;br /&gt;
&lt;br /&gt;
==Frequency response==&lt;br /&gt;
[[File:Frequency response of ideal and practical integrator.png|Frequency response of ideal and practical integrator.]]&lt;br /&gt;
&lt;br /&gt;
The frequency responses of the practical and ideal integrator are shown in the above figure. For both circuits, the crossover frequency &amp;lt;math&amp;gt;f_\text{b}&amp;lt;/math&amp;gt;, at which the gain is 0 dB, is given by:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;f_{\text{b}}=\frac{1}{{2\pi}{R_{\text{1}}}{ C_{\text{F}}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The 3 dB [[cutoff frequency]] &amp;lt;math&amp;gt;f_\text{a}&amp;lt;/math&amp;gt; of the practical circuit is given by:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;f_{\text{a}}=\frac{1}{{2\pi}{R_{\text{F}}}{ C_{\text{F}}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The practical integrator circuit is equivalent to an active first-order [[low-pass filter]]. The gain is relatively constant up to the cutoff frequency decreases by 20 dB per decade beyond it. The integration operation occurs for frequencies in the range &amp;lt;math&amp;gt;\left[ f_\text{a}, f_\text{b} \right]&amp;lt;/math&amp;gt;, provided that &amp;lt;math&amp;gt;f_\text{a} &amp;lt; f_\text{b}&amp;lt;/math&amp;gt;. This condition can be achieved by appropriate choice of &amp;lt;math&amp;gt;R_\text{F}C_\text{F}&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;R_1 C_\text{F}&amp;lt;/math&amp;gt; time constants.&lt;br /&gt;
&lt;br /&gt;
==Applications==&lt;br /&gt;
The integrator is mostly used in [[analog computer]]s, [[analog-to-digital converter]]s and wave-shaping circuits.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*[http://www.mycircuits9.com/2012/12/op-amp-as-integrator-tutorial-with-design-derivation.html OP AMP Integrator Complete Tutorial]&lt;br /&gt;
&lt;br /&gt;
{{Reflist|refs=&lt;br /&gt;
&amp;lt;ref name=&amp;quot;microchip-opa-dc&amp;quot;&amp;gt;{{cite web&lt;br /&gt;
 | title = AN1177 Op Amp Precision Design: DC Errors&lt;br /&gt;
 | publisher = Microchip&lt;br /&gt;
 | date = 2 January 2008&lt;br /&gt;
 | url = http://ww1.microchip.com/downloads/en/AppNotes/01177a.pdf&lt;br /&gt;
 | archiveurl = http://www.webcitation.org/6Db011SaW&lt;br /&gt;
 | archivedate = 2013-01-11&lt;br /&gt;
 | deadurl = no&lt;br /&gt;
 | format = PDF&lt;br /&gt;
 | accessdate = 26 December 2012}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Analog circuits]]&lt;/div&gt;</summary>
		<author><name>en&gt;Headbomb</name></author>
	</entry>
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