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	<title><![CDATA[Mandakini Study Institute - Patna: NCERT Class 12 Physics Notes : Alternating Currents]]></title>
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	<pubDate>Sun, 24 Nov 2019 23:01:27 +0000</pubDate>
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	<title><![CDATA[NCERT Class 12 Physics Notes : Alternating Currents]]></title>
	<description><![CDATA[<p><strong>Transient Current</strong></p><p>An electric current which vary for a small finite time, while growing from zero to maximum or decaying from maximum to zero, is called a transient current.</p><p><strong>Growth of Current in an Inductor</strong></p><p>Growth of current in an inductor at any instant of time t is given by</p><p>I = I<sub>o</sub>(1 &ndash; e&nbsp;<sup>-Rt / L</sup>)</p><p>where, I<sub>o</sub>&nbsp;= maximum current, L = self inductance of the inductor and R = resistance of the circuit.</p><p>Here R / L = &tau;, is called time constant of a L &ndash; R circuit.</p><p><ins data-ad-client="ca-pub-6709000355577070" data-ad-format="auto" data-adsbygoogle-status="done" data-overlap-observer-io="false"><ins><ins></ins></ins></ins></p><p>Time constant of a L &ndash; R circuit is the time in which current in the circuit grows to 63.2% of the maximum value of current.</p><p>Decay of current in an inductor at any time t is given by</p><p>I = I<sub>o</sub>e&nbsp;<sup>-Rt / L</sup></p><p>Time constant of a L &ndash; R circuit is the time in which current decays to 36.8% of the maximum value of current.</p><p><strong>Charging and Discharging of a Capacitor</strong></p><p>The instantaneous charge on a capacitor on charging at any instant of time t is given by</p><p>q = q<sub>o</sub>(1 &ndash; e&nbsp;<sup>&ndash; t / RC</sup>)</p><p>where RC = &tau;, is called time constant of a R &ndash; C circuit.</p><p>The instantaneous charge on a capacitor in discharging at any instant of time t is given by q = q<sub>o</sub>e&nbsp;<sup>&ndash; t / RC</sup></p><p>Time constant of a R &ndash; C circuit is the time in which charge in the capacitor grows to 63.8% or decay to 36.8% of the maximum charge on capacitor.</p><p><strong>Alternating Current</strong></p><p>An electric current whose magnitude changes continuously with time and changes its direction periodically, is called an alternating current.</p><p>The instantaneous value of alternating current at any instant of time t is given by</p><p>I = I<sub>o</sub>&nbsp;sin &omega;t</p><p>where, 10 = peak value of alternating current.</p><p>The variation of alternating current with time is shown in graph given below</p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm3.staticflickr.com/2926/14620684229_629f18b2bd_o.jpg"></figure><p>Mean or average value of alternating current for first half cycle</p><p>I<sub>m</sub>&nbsp;= 2I<sub>o</sub>&nbsp;/ &pi; = 0.637 I<sub>o</sub></p><p>Mean or average value of alternating current for next half cycle</p><p>I&rsquo;<sub>m</sub>&nbsp;= &ndash; 2I<sub>o</sub>&nbsp;/ &pi; = &ndash; 0.637 I<sub>o</sub></p><p>Mean or average value of alternating current for one complete cycle = O.</p><p>Root mean square value of alternating current</p><p>I<sub>v</sub>&nbsp;= I<sub>rms</sub>&nbsp;= I<sub>o</sub>&nbsp;/ &radic;2 = 0.707 I<sub>o</sub></p><p>Where, I<sub>o</sub>&nbsp;= peak value of alternating current.</p><p>Root mean square value of alternating voltage</p><p>V<sub>rms</sub>&nbsp;= V<sub>o</sub>&nbsp;/ &radic;2 = 0.707 I<sub>o</sub>&nbsp;= 0.707 V<sub>o</sub></p><p>Reactance</p><p>The opposition offered by an inductor or by a capacitor in the path of flow of alternating current is called reactance.</p><p>Reactance is of two types</p><p>(i)&nbsp;<strong>Inductive Reactance</strong>&nbsp;(X<sub>L</sub>) Inductive reactance is the resistance offered by an inductor.</p><p>Inductive reactance (X<sub>L</sub>) = L&omega; = L2&pi;f = L2&pi; / T</p><p>Its unit is ohm. X<sub>L</sub>&nbsp;&prop; f</p><p>For direct current, X<sub>L</sub>&nbsp;= 0 (f = 0)</p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm4.staticflickr.com/3926/14620798997_77df336cf2_o.jpg"></figure><p>(ii)&nbsp;<strong>Capacitive Reactance</strong>&nbsp;(X<sub>c</sub>) Capacitive reactance is the resistance offered by an inductor</p><p>Capacitive reactance,</p><p>X<sub>c</sub>&nbsp;= 1 / C&omega; = 1 / C2&pi;f = T / C 2&pi;</p><p>Its unit is ohm X<sub>c</sub>&nbsp;&prop; 1 / f</p><p>For direct current, X<sub>c</sub>&nbsp;= &infin; (f = 0)</p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm4.staticflickr.com/3863/14806977092_c211fd9a09_o.jpg"></figure><p><strong>Impedance</strong></p><p>The opposition offered by an AC circuit containing more than one out of three components L, C and R, is called impedance (Z) of the circuit.</p><p>Impedance of an AC circuit, Z = &radic;R<sup>2</sup>&nbsp;+ (X<sub>L</sub>&nbsp;&ndash; X<sub>C</sub>)<sup>2</sup></p><p>Its SI unit is ohm.</p><p><strong>Power in an AC Circuit</strong></p><p>The power is defined as the rate at which work is being in the circuit.</p><p>The average power in an AC circuit,</p><p>P<sub>av</sub>&nbsp;= V<sub>rms</sub>&nbsp;i<sub>rms</sub>&nbsp;cos &theta;</p><p>= V / &radic;2 i / &radic;2 cos &theta; = Vi / &radic;2 cos &theta;</p><p>where, cos &theta; = Resistance(R) / Impedance (Z) is called the power factor 0f AC circuit.</p><p><strong>Current and Potential Relations</strong></p><p>Here, we will discuss current and potential relations for different AC circuits.</p><p>(i)&nbsp;<strong>Pure Resistive Circuit (R</strong>&nbsp;circuit)</p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm6.staticflickr.com/5556/14620798847_6ac6dc5c44_o.jpg"></figure><p>(a) Alternating emf, E = E<sub>o</sub>&nbsp;sin &omega;t</p><p>(b) Alternating current, I = I<sub>o</sub>&nbsp;sin &omega;t</p><p>(c) Alternating emf and alternating current both are in the same phase.</p><p>(d) Average power decay, (P) = E<sub>v</sub>&nbsp;. I<sub>v</sub></p><p>(e) Power factor, cos &theta; = 1</p><p><strong>(ii) Pure Inductive Circuit (L</strong>&nbsp;Circuit)</p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm3.staticflickr.com/2925/14804218031_28aeaaa04f_o.jpg"></figure><p>(a) Alternating emf, E = E<sub>o</sub>&nbsp;sin &omega;t</p><p>(b) Alternating current, I = I<sub>o</sub>&nbsp;sin (&omega;t &ndash; &pi; / 2)</p><p>(c) Alternating current lags behind alternating emf by &pi; / 2.</p><p>(d) Inductive reactance, X<sub>L</sub>&nbsp;= L&omega; = L2&pi;f</p><p>(e) Average power decay, (P) = 0</p><p>(f) Power factor, cos &theta; = cos 90&deg; = 0</p><p>(iii)<strong>&nbsp;Pure Capacitive Circuit</strong></p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm6.staticflickr.com/5553/14620615050_2d337c944d_o.jpg"></figure><p>(a) Alternating emf, E = E<sub>o</sub>&nbsp;sin &omega;t</p><p>(b) Alternating current, I = I<sub>o</sub>&nbsp;sin (&omega;t + &pi; / 2)</p><p>(c) Alternating current lags behind alternating emf by &pi; / 2.</p><p>(d) Inductive reactance, X<sub>L</sub>&nbsp;= C&omega; = C2&pi;f</p><p>(e) Average power decay, (P) = 0</p><p>(f) Power factor, cos &theta; = cos 90&deg; = 0</p><p>(iv)&nbsp;<strong>R &ndash; C Circuit</strong></p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm4.staticflickr.com/3871/14827161683_bfaedd01ee_o.jpg"></figure><p>E = E<sub>o</sub>&nbsp;sin &omega;t</p><p>I = E<sub>o</sub>&nbsp;/ 2 sin (&omega;t &ndash; &phi;)</p><p>Z = &radic;R<sup>2</sup>&nbsp;+ (1 / &omega;C)<sup>2</sup></p><p>tan &phi; = &ndash; 1 / &omega;C / R</p><p>Current leading the voltage by &phi;</p><p>V<sup>2</sup>&nbsp;= V<sup>2</sup><sub>R</sub>&nbsp;= V<sup>2</sup><sub>C</sub></p><p>(v)&nbsp;<strong>L &ndash; C Circuit</strong></p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm4.staticflickr.com/3865/14620684189_19ef03dbbc_o.jpg"></figure><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm4.staticflickr.com/3893/14804417711_c2e09d6f3e_o.jpg"></figure><p>(vi)&nbsp;<strong>L &ndash; C &ndash; R Circuit</strong></p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm6.staticflickr.com/5557/14620614890_f5ef4bb490_o.jpg"></figure><p>(a) Alternating emf, E = E<sub>o</sub>&nbsp;sin &Omega;t</p><p>(b) Alternating current, I = I<sub>o</sub>&nbsp;sin (&Omega;t &plusmn; &theta;)</p><p>(c) Alternating current lags leads behind alternating emf by &omega;.</p><p>(d) Resultant voltage, V = &radic;V<sup>2</sup><sub>R</sub>&nbsp;+ (V<sub>L</sub>&nbsp;&ndash; V<sub>C</sub>)<sup>2</sup></p><p>(e) Impedance, Z = &radic;R<sup>2</sup>&nbsp;+ (X<sub>L</sub>&nbsp;&ndash; X<sub>C</sub>)<sup>2</sup></p><p>(f) Power factor, cos &theta; = R / Z = R / &radic;&radic;R<sup>2</sup>&nbsp;+ (X<sub>L</sub>&nbsp;&ndash; X<sub>C</sub>)<sup>2</sup></p><p>(g) Average power decay, (P)= E<sub>V</sub>I<sub>V</sub>&nbsp;cos &theta;</p><p><strong>Resonance in AC Circuit</strong></p><p>The condition in which current is maximum or impedance is minimum in an AC circuit, is called resonance.</p><p>(i)&nbsp;<strong>Series Resonance Circuit</strong></p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm6.staticflickr.com/5551/14806976702_579bf93e11_o.jpg"></figure><p>In this circuit components L, C and R are connected in series.</p><p>At resonance = X<sub>L</sub>&nbsp;= X<sub>C</sub></p><p>Resonance frequency f = 1 / 2&pi;&radic;LC</p><p>A series resonance circuit is also known as acception circuit.</p><p>(ii)<strong>&nbsp;Parallel Resonance Circuit</strong></p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm6.staticflickr.com/5575/14804964504_00724bcb19_o.jpg"></figure><p>In this circuit L and C are connected in parallel with each other.</p><p>At resonance, X<sub>L</sub>&nbsp;= X<sub>C</sub></p><p>Impedance (Z) of the circuit is maximum.</p><p>Current in the circuit is minimum.</p><p><strong>Wattless Current</strong></p><p>Average power is given by</p><p>P<sub>av</sub>&nbsp;= E<sub>rms</sub>&nbsp;= I<sub>rms</sub>&nbsp;cos &theta;</p><p>Here the I<sub>rms</sub>&nbsp;cos &phi; contributes for power dissipation. Therefore, it is called wattless current.</p><p><strong>AC Generator or Dynamo</strong></p><p>It is a device which converts mechanical energy into alternating current energy.</p><p>Its working is based on electromagnetic induction.</p><p>The induced emf produced by the AC generator is given by</p><p>e = NBA&omega; sin &omega;t = e<sub>o</sub>&nbsp;= sin &omega;t</p><p>There are four main parts of an AC generator</p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm4.staticflickr.com/3868/14620683879_92e1b42c84_o.jpg"></figure><p>(i)&nbsp;<strong>Armature</strong>&nbsp;It is rectangular coil of insulated copper wire having a large number of turns.</p><p>(ii)&nbsp;<strong>Field Magnet</strong>s These are two pole pieces of a strong electromagnet.</p><p><ins data-ad-client="ca-pub-6709000355577070" data-ad-format="auto" data-adsbygoogle-status="done" data-overlap-observer-io="false"><ins><ins></ins></ins></ins></p><p>(iii)&nbsp;<strong>Slip Rings</strong>&nbsp;These are two hollow metallic rings.</p><p>(iv)&nbsp;<strong>Brushes</strong>&nbsp;These are two flexible metals or carbon rods, which remains slightly in contact with slip rings .</p><p><strong>Note</strong>&nbsp;An DC generator or dynamo contains split rings or commutator inspite of slip rings.</p><p><strong>DC Motor</strong></p><p>It is a device which converts electrical energy into mechanical energy.</p><p>Its working is based on the fact that when a current carrying coil is placed in uniform magnetic field a torque acts on it.</p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm4.staticflickr.com/3855/14620711678_cd542e400a_o.jpg"></figure><p>Torque acting on a current carrying coil placed in uniform magnetic field</p><p>&tau; = NBIA sin &theta;</p><p>When armature coil rotates a back emf is produced in the coil.</p><p>Efficiency of a motor,</p><p>&eta; = Back emf / Applied emf = E / V</p><p><strong>Transformer</strong></p><p>It is a device which can change a low voltage of high current into a high voltage of low current and vice-versa.</p><p>Its working is based on mutual induction.</p><p>There are two types of transformers.</p><p>(i)&nbsp;<strong>Step-up Transformers</strong>&nbsp;It converts a low voltage of high current into a high voltage of low current.</p><figure><img alt="CBSE Class 11 Physics Notes Alternating Currents" data-pin-no-hover="true" src="https://farm4.staticflickr.com/3917/14784331766_ea9be95efc_o.jpg"></figure><p>In this transformer,</p><p>N<sub>s</sub>&nbsp;&gt; N<sub>P</sub>, E<sub>s</sub>&nbsp;&gt; E<sub>P</sub></p><p>and I<sub>P</sub>&nbsp;&gt; I<sub>S</sub></p><p><strong>(ii) Step-down Transformer</strong>&nbsp;It converts a high voltage of low current into a low voltage of high current.</p><p>In this transformer,</p><p>N<sub>P</sub>&nbsp;&gt; N<sub>S</sub>, E<sub>P</sub>&nbsp;&gt; E<sub>S</sub>&nbsp;and I<sub>P</sub>&nbsp;&lt; I<sub>S</sub></p><p><strong>Transformation Ratio</strong></p><p>Transformation ratio,</p><p>K = N<sub>S</sub>&nbsp;/ N<sub>P</sub>&nbsp;= E<sub>S</sub>&nbsp;/ E<sub>P</sub>&nbsp;= I<sub>P</sub>&nbsp;/ I<sub>S</sub></p><p>For step-up transformer, K &gt; 1</p><p>For step-down transformer, K &lt; 1</p><p><strong>Energy Losses in a Transformer</strong></p><p>The main energy losses in a transformer are given below</p><ol>
	<li>Iron loss</li>
	<li>Copper loss</li>
	<li>Flux loss</li>
	<li>Hysteresis loss</li>
	<li>Humming loss</li>
</ol><p><strong>Important Points</strong></p><ul>
	<li>Transformer does not operate on direct current. It operates only on alternating voltages at input as well as at output.</li>
	<li>Transformer does not amplify power as vacuum tube.</li>
	<li>Transformer, a device based on mutual induction converts magnetic energy into electrical energy.</li>
	<li>Efficiency, &eta; = Output power / Input power</li>
</ul><p>Generally efficiency ranges from 70% to 90%.</p><ul>
	<li>A choke coil is a pure inductor. Average power consumed per cycle is zero in a choke coil.</li>
	<li>A DC motor connects DC energy from a battery into mechanical energy of rotation.</li>
	<li>An AC dynamo/generator produces are energy from mechanical energy of rotation of a coil.</li>
	<li>An induction coil generates high voltages of the order of 1OS V from a battery.</li>
</ul><p>It is based on the phenomenon of mutual induction.</p>]]></description>
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