{"id":28060,"date":"2019-10-30T15:28:04","date_gmt":"2019-10-30T09:58:04","guid":{"rendered":"http:\/\/mycbseguide.com\/blog\/?p=28060"},"modified":"2019-10-31T17:29:59","modified_gmt":"2019-10-31T11:59:59","slug":"cbse-class-12-physics-chapter-2-extra-questions","status":"publish","type":"post","link":"https:\/\/mycbseguide.com\/blog\/cbse-class-12-physics-chapter-2-extra-questions\/","title":{"rendered":"CBSE Class 12 Physics Chapter 2 Extra Questions"},"content":{"rendered":"<p><strong>CBSE Class 12 Physics Chapter 2 Extra Questions. <\/strong>We know Physics is tough subject within the consortium of science subjects physics is an important subject. But if you want to make career in these fields like IT Consultant, Lab Technician, Laser Engineer, Optical Engineer etc. You need to have strong fundamentals in physics to crack the exam<strong>.\u00a0<\/strong>myCBSEguide has just released Chapter Wise Question Answers for class 12 Physics. There chapter wise Extra Questions with complete solutions are available for download in\u00a0<strong><a href=\"https:\/\/mycbseguide.com\/\">myCBSEguide<\/a>\u00a0<\/strong>website and mobile app. These Questions with solution are prepared by our team of expert teachers who are teaching grade in CBSE schools for years. There are around 4-5 set of solved Physics Extra Questions from each and every chapter. The students will not miss any concept in these Chapter wise question that are specially designed to tackle Board Exam. We have taken care of every single concept given in\u00a0<strong><a href=\"https:\/\/mycbseguide.com\/course\/cbse-class-12-physics\/1251\/\">CBSE Class 12 Physics syllabus<\/a><\/strong>\u00a0and questions are framed as per the latest marking scheme and blue print issued by CBSE for class 12.<\/p>\n<div class=\"row\">\n<div class=\"col-md-12\">\n<div class=\"card\">\n<div class=\"row\">\n<div class=\"col-md-12\">\n<div class=\"card\">\n<p style=\"text-align: center;\"><strong>Class 12 Physics Extra Questions<\/strong><\/p>\n<p style=\"text-align: center;\"><strong><a class=\"button\" href=\"https:\/\/mycbseguide.com\/dashboard\/category\/1253\/type\/4\">Download as PDF<\/a><\/strong><\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<div class=\"toolbar-container\">\n<div class=\"toolbar-content\">\n<h2 class=\"toolbar-title\">Class 12 Physics Electrostatic Potential and Capacitance Practice Questions<\/h2>\n<\/div>\n<div class=\"icon-inner\">\n<ol style=\"padding-left: 20px;\">\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>Correct formula for capacitance in terms of area A and distance d, of a parallel plate capacitor in vacuum is<\/p>\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li><span class=\"mcq_option_text\"><span class=\"math-tex\">{tex}\\epsilon_0\\frac{A}{d^2}{\/tex}<\/span><\/span><\/li>\n<li><span class=\"mcq_option_text\"><span class=\"math-tex\">{tex}\\epsilon_0\\frac{A^2}{d}{\/tex}<\/span><\/span><\/li>\n<li><span class=\"mcq_option_text\"><span class=\"math-tex\">{tex}\\epsilon_0\\frac{d}{A}{\/tex}<\/span><\/span><\/li>\n<li><span class=\"mcq_option_text\"><span class=\"math-tex\">{tex}\\epsilon_0\\frac{A}{d}{\/tex}<\/span><\/span><\/li>\n<\/ol>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>Two parallel plate capacitors of capacitances C and 2C are connected in parallel and charged to a potential difference V by a battery. The battery is then disconnected and the space between the plates of capacitor C is completely filled with a material of dielectric constant K = 3. The potential difference across the capacitors now becomes<\/p>\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li><span class=\"mcq_option_text\"><span class=\"math-tex\">{tex}{2V \\over 5}{\/tex}<\/span><\/span><\/li>\n<li><span class=\"mcq_option_text\"><span class=\"math-tex\">{tex}{3V \\over 6}{\/tex}<\/span><\/span><\/li>\n<li><span class=\"mcq_option_text\"><span class=\"math-tex\">{tex}{V \\over 4}{\/tex}<\/span><\/span><\/li>\n<li><span class=\"mcq_option_text\"><span class=\"math-tex\">{tex}{3V \\over 5}{\/tex}<\/span><\/span><\/li>\n<\/ol>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-text\">A variable capacitor and an electroscope are connected in parallel to a battery. The reading of the electroscope would be decreased by<\/div>\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li>Decreasing the battery potential<\/li>\n<li>Increasing the area of overlapping of the plates<\/li>\n<li>Decreasing the distance between the plates<\/li>\n<li>Placing a dielectric between the plates<\/li>\n<\/ol>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">The capacity of a pure capacitor is 1 farad. In DC circuit its effective resistance will be\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li>infinite<\/li>\n<li>zero<\/li>\n<li>1 <span class=\"math-tex\">{tex}\\Omega {\/tex}<\/span><\/li>\n<li><span style=\"font-size: 0.9em;\">2 ohm<\/span><\/li>\n<\/ol>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-text\">In circuits, a difference in potential from one point to another is often called<\/div>\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li>volts<\/li>\n<li>AT<\/li>\n<li>field<\/li>\n<li>voltage<\/li>\n<\/ol>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>What is the geometrical shape of equipotential surfaces due to a single isolated charge?<\/p>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>Draw equipotential surfaces due to a single point charge.<\/p>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>Two charges 2 \u00b5C and -2 \u00b5C are placed at points A and B, 5 cm apart. Depict an equipotential surface of the system.<\/p>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>What are the dimensions of capacitance?<\/p>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>A slab of material of dielectric constant K has the same area as that of the plates of a parallel plate capacitor, but has the thickness d\/2, where d is the separation between the plates. Find out the expression for its capacitance when the slab is inserted between the plates of the capacitor.<\/p>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>Two capacitors of 1 \u00b5F capacitance are connected to a battery of 6 V. Initially switch S is closed. After sometime S is left open and dielectric slab of dielectric constant K = 3 are inserted to fill completely the space between the plates of the two capacitors.<br \/>\nHow will the (i) charge and (ii) potential difference between the plates of the capacitors be affected after the slabs are inserted?<br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone\" style=\"width: 168px; height: 73px;\" title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/JluPcFU.png\" alt=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" width=\"168\" height=\"73\" data-imgur-src=\"JluPcFU.png\" \/><\/p>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>Electric charge is distributed uniformly on the surface of a spherical rubber balloon. Show how the value of electric intensity and potential vary<\/p>\n<ol style=\"list-style-type: lower-roman;\" start=\"1\">\n<li>on the surface,<\/li>\n<li>inside and<\/li>\n<li>outside?<\/li>\n<\/ol>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<p>A <span class=\"math-tex\">{tex}5\\mu F{\/tex}<\/span> capacitor is charged by a 100 V supply. The supply is then disconnected and the charged capacitor is connected to another uncharged <span class=\"math-tex\">{tex}3\\mu F{\/tex}<\/span> capacitor. How much electrostatic energy of the first capacitor is lost in the process of attaining the steady situation?<\/p>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<ol style=\"list-style-type: lower-roman;\" start=\"1\">\n<li>Derive the expression for the capacitance of a parallel plate capacitor having plate area A and plate separation d.<\/li>\n<li>Two charged spherical conductors of radii R<sub>1<\/sub> and R<sub>2<\/sub> when connected by a conducting plate respectively. Find the ratio of their surface charge densities in terms of their radii.<\/li>\n<\/ol>\n<\/div>\n<\/div>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">\n<div class=\"question-container\">\n<div class=\"question-text\">\n<ol style=\"list-style-type: lower-roman;\" start=\"1\">\n<li>Explain using suitable diagrams, the difference in the behaviour of a\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li>conductor and<\/li>\n<li>dielectric in the presence of external electric field. Define the terms polarisation of a dielectric and write its relation with susceptibility.<\/li>\n<\/ol>\n<\/li>\n<li>A thin metallic spherical shell of radius R carries a charge Q on its surface. A point charge Q\/2 is placed at its centre C and another charge + 2Q is placed outside the shell at a distance x from the centre as shown in the figure. Find<br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone\" style=\"width: 100px; height: 84px;\" title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/4hkwTZd.png\" alt=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" width=\"138\" height=\"116\" data-imgur-src=\"4hkwTZd.png\" \/><\/li>\n<\/ol>\n<\/div>\n<\/div>\n<\/li>\n<\/ol>\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li>the force on the charge at the centre of shell and at the point A,<\/li>\n<li>the electric flux through the shell.<\/li>\n<\/ol>\n<\/div>\n<\/div>\n<p style=\"page-break-before: always; text-align: center;\"><strong>Class &#8211; 12 Physics (Electrostatics Potential and Capacitance)<\/strong><br \/>\n<strong>Answers<\/strong><\/p>\n<hr \/>\n<ol style=\"padding-left: 20px;\">\n<li class=\"question-list\" style=\"clear: both;\">\n<ol style=\"margin-top: 5px; padding-left: 15px; list-style-type: lower-alpha;\" start=\"4\" type=\"a\">\n<li><span class=\"math-tex\">{tex}\\epsilon_0\\frac{A}{d}{\/tex}<\/span><strong>Explanation:<\/strong>\u00a0The capacitance of a parallel plate capacitor is given by <span class=\"math-tex\">{tex}C = \\frac{{{\\varepsilon _0}A}}{d}{\/tex}<\/span><\/li>\n<\/ol>\n<ol style=\"margin-top: 5px; padding-left: 15px; list-style-type: lower-alpha;\" start=\"4\" type=\"a\">\n<li><span class=\"math-tex\">{tex}{3V \\over 5}{\/tex}<\/span><strong>Explanation:<\/strong>\u00a0The charges on the capacitors after being charged to a potential V are Q1 = CV; Q2 = 2CV.<br \/>\nAfter being filled with a material of dielectric K = 3 the capacitor which initially had a capacitance C has now the capacitance KC = 3C. The common potential<br \/>\n<span class=\"math-tex\">{tex}{V_1} = \\frac{{{\\text{Total charge}}}}{{{\\text{Total capacitance}}}} = \\frac{{{Q_1} + {Q_2}}}{{3C + 2C}}{\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex} = \\frac{{CV + 2CV}}{{5C}} = \\frac{3}{5}V{\/tex}<\/span><\/li>\n<\/ol>\n<ol style=\"margin-top: 5px; padding-left: 15px;\" type=\"a\">\n<li>Decreasing the battery potential<br \/>\n<strong>Explanation:<\/strong>\u00a0An electroscope is a device which measures the potential difference. If it is connected in parallel to the capacitor, the potential across it will be equal to the potential across the capacitor, which is equal to the potential across the battery. On decreasing the battery potential, the potential difference across the electroscope reduces and hence the reading reduces. While the capacitor is connected to the battery, Placing a dielectric between the plates, or decreasing the distance between the plates or increasing the area of the plates will not change the potential difference across it; since it will always remain equal to the potential difference maintained by the battery. In the cases B, C and D, The capacitance of the capacitor, however increases; but this increase happens due to increase in the charge stored in the capacitor while the potential remains constant.<\/li>\n<\/ol>\n<ol style=\"margin-top: 5px; padding-left: 15px;\" type=\"a\">\n<li>infinite<br \/>\n<strong>Explanation:<\/strong> Capacitor does not allow DC to pass through it. The effective capacitance or the capacitive reactance <span class=\"math-tex\">{tex}{X_C} = \\frac{1}{{C\\omega }}{\/tex}<\/span><span style=\"font-size: 0.9em;\">,<\/span><br \/>\nwhere \u03c9 is the frequency of voltage source.<br \/>\nSince DC current is a constant current, its frequency is zero.<br \/>\nThe capacitive reactance is therefore infinity.<\/li>\n<\/ol>\n<ol style=\"margin-top: 5px; padding-left: 15px; list-style-type: lower-alpha;\" start=\"4\" type=\"a\">\n<li>voltage<br \/>\n<strong>Explanation:<\/strong> Voltage is an electrical potential difference, the difference in electric potential between two places. The unit for electrical potential difference, or voltage, is the volt.<\/li>\n<\/ol>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">The equipotential surfaces produced by a single point charge are spherically symmetrical surfaces which are concentric.<br \/>\nIn concentric spheres which are as shown below in the figure, the lines of force point radially outwards, so they are perpendicular to the equipotential surfaces at all points.<br \/>\nIf we place another unit positive charge at any point on these surfaces, that will repelled along the the direction of the electric field intensity i.e. radially outwards to the surfaces.<br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone\" style=\"width: 212px; height: 180px;\" title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/jFAI0f3.png\" alt=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" width=\"205\" height=\"174\" data-imgur-src=\"jFAI0f3.png\" \/><\/li>\n<li class=\"question-list\" style=\"clear: both;\">Equipotential surfaces due to a single point charge are concentric sphere having charge at the centre. Electric field lines are always normally outwards from the spherical surfaces.<br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone\" style=\"width: 170px; height: 120px;\" title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/nX3Hpgi.png\" alt=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" width=\"181\" height=\"128\" data-imgur-src=\"nX3Hpgi.png\" \/><\/li>\n<li class=\"question-list\" style=\"clear: both;\">Given, <span class=\"math-tex\">{tex}q _ { A } = 2 \\mu C = 2 \\times 10 ^ { &#8211; 6 } C{\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex}q _ { g } = &#8211; 2 \\mu C = &#8211; 2 \\times 10 ^ { &#8211; 6 } C{\/tex}<\/span> and r = 5 cm<br \/>\n<img decoding=\"async\" style=\"width: 107px; height: 33px;\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/0zRHy6o.png\" alt=\"\" data-imgur-src=\"0zRHy6o.png\" \/><br \/>\nAs, potential at point O is zero.<br \/>\n<span class=\"math-tex\">{tex}V = \\frac { 2 \\times 10 ^ { &#8211; 6 } } { 4 \\pi \\varepsilon _ { 0 } x \\times 10 ^ { &#8211; 2 } } + \\frac { &#8211; 2 \\times 10 ^ { &#8211; 6 } } { 4 \\pi \\varepsilon _ { 0 } ( 5 &#8211; x ) \\times 10 ^ { &#8211; 2 } } = 0{\/tex}<\/span><br \/>\nor <span class=\"math-tex\">{tex}\\frac { 2 \\times 10 ^ { &#8211; 6 } } { 4 \\pi \\varepsilon _ { 0 } x \\times 10 ^ { &#8211; 2 } } = \\frac { 2 \\times 10 ^ { &#8211; 6 } } { 4 \\pi \\varepsilon _ { 0 } ( 5 &#8211; x ) \\times 10 ^ { &#8211; 2 } }{\/tex}<\/span><br \/>\nor x = 5 &#8211; x <span class=\"math-tex\">{tex}\\Rightarrow{\/tex}<\/span> x = 2.5 cm<br \/>\nHence equipotential surface is a plane normal to the axis of the dipole and lies at the mid point of the axis.<\/li>\n<li class=\"question-list\" style=\"clear: both;\"><span class=\"math-tex\">{tex}\\left[ {{M^{ &#8211; 1}}{L^{ &#8211; 2}}{A^2}{T^4}} \\right]{\/tex}<\/span><\/li>\n<li class=\"question-list\" style=\"clear: both;\">Initially, when there is vacuum between the two plates of the capacitor, then capacitance of the capacitor becomes <span class=\"math-tex\">{tex}C _ { 0 } = \\frac { \\varepsilon _ { 0 } A } { d }{\/tex}<\/span>,<br \/>\nwhere, A is the area of each plate of the capacitor.<br \/>\nSuppose that the capacitor is connected to a battery, an electric field E<sub>0<\/sub> is produced.<br \/>\nNow, if we insert the dielectric slab of dielectric constant K and of thickness t = d\/2, the electric field reduces to E = E<sub>0<\/sub>\/K.<br \/>\nNow, the gap between plates is divided in two parts, for distance t, there is electric field E and for the remaining distance (d &#8211; t) the electric field is E<sub>0<\/sub>.<br \/>\nIf V be the potential difference between the plates of the capacitor after inserting the dielectric slab, then V = Et + E<sub>0<\/sub>(d &#8211; t)<br \/>\n<span class=\"math-tex\">{tex}\\Rightarrow V = \\frac { E d } { 2 } + \\frac { E _ { 0 } d } { 2 } = \\frac { d } { 2 } \\left( E + E _ { 0 } \\right) \\quad \\left[ \\because t = \\frac { d } { 2 } \\right]{\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex}\\Rightarrow \\quad V = \\frac { d } { 2 } \\left( \\frac { E _ { 0 } } { K } + E _ { 0 } \\right){\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex}= \\frac { d E _ { 0 } } { 2 K } ( K + 1 ){\/tex}<\/span> <span class=\"math-tex\">{tex}\\left[ \\text { As, } \\frac { E _ { 0 } } { E } = K \\right]{\/tex}<\/span><br \/>\nNow, <span class=\"math-tex\">{tex}E _ { 0 } = \\frac { \\sigma } { \\varepsilon _ { 0 } } = \\frac { q } { \\varepsilon _ { 0 } A } {\/tex}<\/span>, Hence the potential becomes\u00a0<span class=\"math-tex\">{tex} V = \\frac { d } { 2 K } \\cdot \\frac { q } { \\varepsilon _ { 0 } A } ( K + 1 ){\/tex}<\/span><br \/>\nAgain we know that, <span class=\"math-tex\">{tex}C = \\frac { q } { V } = \\frac { 2 K \\varepsilon _ { 0 } A } { d ( K + 1 ) }{\/tex}<\/span>(substituting the value of V)<\/p>\n<ol style=\"list-style-type: lower-roman;\" start=\"1\">\n<li>According to the diagram, when the switch S is closed, the two capacitors C<sub>1<\/sub> and C<sub>2<\/sub> in parallel will be charged by the same potential difference V.<br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone\" style=\"width: 191px; height: 77px;\" title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/LfiZDrH.png\" alt=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" width=\"191\" height=\"77\" data-imgur-src=\"LfiZDrH.png\" \/><br \/>\nSo, charge on capacitor C<sub>1<\/sub><span class=\"math-tex\">{tex}q _ { 1 } = C _ { 1 } V = 1 \\times 6 = 6 \\mu \\mathrm { C }{\/tex}<\/span> &#8230;.(i)<br \/>\nand charge on capacitor C<sub>2<\/sub><br \/>\n<span class=\"math-tex\">{tex}q _ { 2 } = C _ { 2 } V = 1 \\times 6 = 6 \\mu C{\/tex}<\/span> &#8230;(ii)<br \/>\nHence total charge, q = q<sub>1<\/sub> + q<sub>2<\/sub> = 6 + 6 = 12\u00b5C (before the switch S is closed) Now when S is left open, there will be no change in the stored charge value of C<sub>2<\/sub>\u00a0and the change in charge value in C<sub>1<\/sub>\u00a0is given in the answer (ii).<\/li>\n<li>When switch S is opened and dielectric is introduced. Then<br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone\" style=\"width: 167px; height: 77px;\" title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/IQy8fvl.png\" alt=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" width=\"167\" height=\"77\" data-imgur-src=\"IQy8fvl.png\" \/><br \/>\nCapacity of both the capacitors becomes K times<br \/>\ni.e. <span class=\"math-tex\">{tex}C&#8217; _ { 1 } = C _ { 2 } ^ { \\prime } = K C = 3 \\times 1 = 3 \\mu F \\left( \\operatorname { as } C _ { 1 } ^ { \\prime } = C&#8217; _ { 2 } \\right){\/tex}<\/span><br \/>\nCapacitor A remains connected to battery<br \/>\n<span class=\"math-tex\">{tex}\\therefore \\quad V _ { 1 } ^ { \\prime } = V = 6 \\mathrm { V }{\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex}q _ { 1 } ^ { \\prime } = K q _ { 1 } = 3 \\times 6 \\mu C = 18 \\mu C{\/tex}<\/span>\u00a0(charge in C<sub>1<\/sub>\u00a0is increased to 3 times of the previous value)<br \/>\nCapacitor B becomes isolated, charge in it will remain same<br \/>\n<span class=\"math-tex\">{tex}\\therefore q&#8217; _ { 2 } = q _ { 2 } ~{ \\Rightarrow } ~C&#8217; _ { 2 } V&#8217; _ { 2 } = C _ { 2 } V _ { 2 }{\/tex}<\/span>\u00a0or <span class=\"math-tex\">{tex}( K C ) V&#8217; _ { 2 } = C V{\/tex}<\/span>\u00a0(C<sub>2<\/sub>\u00a0= C, C&#8217;<sub>2<\/sub> = KC)<br \/>\nor <span class=\"math-tex\">{tex}V _ { 2 } = \\left( \\frac { V } { K } \\right) = \\frac { 6 } { 3 } = 2 V{\/tex}<\/span>\u00a0(potential difference of the capacitor B is reduced to a factor of 3)<\/li>\n<\/ol>\n<\/li>\n<li class=\"question-list\" style=\"clear: both;\">On the surface E = constant, V = constant. Inside the surface, E = 0, V = constant = potential on surface. Outside the balloon.<br \/>\n<span class=\"math-tex\">{tex}E \\propto \\frac{1}{{{r^2}}}{\/tex}<\/span> and <span class=\"math-tex\">{tex}V \\propto \\frac{1}{r}{\/tex}<\/span><br \/>\nwhere r is the distance of the point from the centre of the balloon.<\/li>\n<li class=\"question-list\" style=\"clear: both;\">Initial energy stored in <span class=\"math-tex\">{tex}5\\mu F{\/tex}<\/span> capacitor,<br \/>\n<span class=\"math-tex\">{tex}{U_i} = \\frac{1}{2}C{V^2} = \\frac{1}{2} \\times 5 \\times {10^{ &#8211; 6}} \\times {(100)^2}{\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex} = 2.5 \\times {10^{ &#8211; 2}}J{\/tex}<\/span><br \/>\nCharge on 5 mF capacitor <span class=\"math-tex\">{tex} = 5 \\times {10^{ &#8211; 6}} \\times 100{\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex} = 5 \\times {10^{ &#8211; 4}}C\\left[ {\\because q = CV} \\right]{\/tex}<\/span><br \/>\nThe two capacitors attain a common potential V when they are connected together.<br \/>\n<span class=\"math-tex\">{tex}V = \\frac{{Total\\;ch\\arg e}}{{total\\;capacitor}} = \\frac{{5 \\times {{10}^{ &#8211; 4}}}}{{(5 + 3) \\times {{10}^{ &#8211; 6}}}} = \\frac{{125}}{2}V{\/tex}<\/span><br \/>\nFinal energy of the combination,<br \/>\n<span class=\"math-tex\">{tex}{U_f} = \\frac{1}{2} \\times (5 + 3) \\times {10^{ &#8211; 6}} \\times {\\left( {\\frac{{125}}{2}} \\right)^2} = 1.56 \\times {10^{ &#8211; 2}}J{\/tex}<\/span><br \/>\nElectrostatic energy lost in the process of attaining the steady state<br \/>\n<span class=\"math-tex\">{tex} = {U_i} &#8211; {U_f} = (2.5 &#8211; 1.56) \\times {10^{ &#8211; 2}}{\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex} = 0.94 \\times {10^{ &#8211; 2}}J{\/tex}<\/span><\/p>\n<ol style=\"list-style-type: lower-roman;\" start=\"1\">\n<li>Parallel plate capacitor consists of two thin conducting plates each of area A held parallel to each other at a suitable distance d. One of the plates is insulated and other is earthed. Say, there is vacuum or air between the plates. Structure of a parallel plate capacitor is shown below.<br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone\" style=\"width: 150px; height: 91px;\" title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/asdiC7e.png\" alt=\"\" width=\"348\" height=\"212\" data-imgur-src=\"asdiC7e.png\" \/><br \/>\nSuppose, the plate X is given a charge of +q coulomb. By induction, -q coulomb of charge is produced on the inner surface of the plate Y and +q coulomb on the outer surface. Since, the plate Y is connected to the earth, hence the relatively weak charge +q residing far away i.e. on the outer surface flows to the earth. Thus, the plates X and Y have equal and opposite charges +q and -q respectively<br \/>\nSuppose, the surface density of charge on each plate is <span class=\"math-tex\">{tex}\\sigma{\/tex}<\/span>, We know that the intensity of electric field at a point between two plane parallel sheets of equal and opposite charges is = <span class=\"math-tex\">{tex}\\frac {\\sigma }{2 \\epsilon _0} -(-\\frac {\\sigma }{2\\epsilon _0}) ={\/tex}<\/span> <span class=\"math-tex\">{tex}\\sigma\/\\varepsilon_0{\/tex}<\/span> [<span class=\"math-tex\">{tex}\\frac {+ \\sigma}{2\\epsilon _0} ~and ~ \\frac {- \\sigma}{2 \\epsilon_0}{\/tex}<\/span> are electric field intensities in between the two plates due to charges +q and -q on the two plates of the capacitor respectively], where <span class=\"math-tex\">{tex}\\varepsilon_0{\/tex}<\/span> is the permittivity of free space. The intensity of electric field between the plates will be given by, <span class=\"math-tex\">{tex}E = \\frac { \\sigma } { \\varepsilon _ { 0 } }{\/tex}<\/span><br \/>\nThe charge on each plate is q and the area of each plate is A. Thus,<br \/>\n<span class=\"math-tex\">{tex}\\sigma = \\frac { q } { A } \\text { and } E = \\frac { q } { \\varepsilon _ { 0 } A }{\/tex}<\/span>&#8230;&#8230;&#8230;&#8230;(i)<br \/>\nNow, let the potential difference between the two plates be V volt. Then, the electric field between the plates is given by<br \/>\n<span class=\"math-tex\">{tex}E = \\frac { V } { d } \\quad \\text { or } \\quad V = E d{\/tex}<\/span>&#8230;..(ii)<br \/>\nSubstituting the value of E from equation (i) into equation (ii), we get<br \/>\n<span class=\"math-tex\">{tex}V = \\frac { q d } { \\varepsilon _ { 0 } A }{\/tex}<\/span><br \/>\nNow capacitance of the parallel plate capacitor is<br \/>\n<span class=\"math-tex\">{tex}C = \\frac { q } { V } = \\frac { q } { q d \/ \\varepsilon _ { 0 } A } \\quad \\text { or } \\quad C = \\frac { \\varepsilon _ { 0 } A } { d }{\/tex}<\/span><br \/>\nWhere, <span class=\"math-tex\">{tex}\\varepsilon _ { 0 } = 8.85 \\times 10 ^ { &#8211; 12 } \\mathrm { C } ^ { 2 } &#8211; \\mathrm { Nm } ^ { &#8211; 2 }{\/tex}<\/span> is the permittivity of vacuum or air.<\/li>\n<li>Surface charge density of a spherically charged body is given by<br \/>\n<span class=\"math-tex\">{tex}\\sigma = \\frac { q } { 4 \\pi R ^ { 2 } }{\/tex}<\/span><br \/>\nAfter connecting both the conductors, their potentials will become equal.<br \/>\n<span class=\"math-tex\">{tex}\\Rightarrow \\frac { K q _ { 1 } } { R _ { \\mathrm { l } } } = \\frac { K q _ { 2 } } { R _ { 2 } }{\/tex}<\/span> [ For a spherically charged conductor with charge q potential is given by, <span class=\"math-tex\">{tex}V = \\frac { 1 } { 4 \\pi \\varepsilon _ { 0 } } \\frac { q } { R } \\text { or } V = \\frac { K q } { R }{\/tex}<\/span>]\n<span class=\"math-tex\">{tex}\\therefore \\frac { q _ { 1 } } { q _ { 2 } } = \\frac { R _ { 1 } } { R _ { 2 } } ~Hence~ \\frac { \\sigma _ { 1 } } { \\sigma _ { 2 } } = \\frac { q _ { 1 } \/ 4 \\pi R _ { 1 } ^ { 2 } } { q _ { 2 } \/ 4 \\pi R _ { 2 } ^ { 2 } }{\/tex}<\/span><br \/>\n<span class=\"math-tex\">{tex}= \\frac { q _ { 1 } } { q _ { 2 } } \\left( \\frac { R _ { 2 } } { R _ { 1 } } \\right) ^ { 2 } = \\frac {R_1}{R_2}\u00d7 \\left (\\frac {R_2}{R_1} \\right)^{2}= \\frac { R _ { 2 } } { R _ { 1 } }{\/tex}<\/span><\/li>\n<\/ol>\n<ol style=\"list-style-type: lower-roman;\" start=\"1\">\n<li style=\"list-style-type: none;\">\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li>When a conductor is placed in an external electric field, the free charges present inside the conductor redistribute themselves in such a manner that the electric field due to induced charges opposes the external field within the conductor. This happens until a static situation is achieved, i.e. when the two fields cancels each other, then the net electrostatic field in the conductor becomes zero.<\/li>\n<li>Dielectrics are non-conducting substances. i.e. they have no charge carriers. Thus, in a dielectric, free movement of charges is not possible. When a dielectric is placed in an external electric field, the molecules are re-oriented and thus induces a net dipole moment in the dielectric. This produces an electric field. The diagram clearly shows that the net electric field in case of a conductor becomes zero, whereas in case of a dielectric net electric field intensity becomes non zero.<br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone\" style=\"width: 200px; height: 144px;\" title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" src=\"https:\/\/media-mycbseguide.s3.amazonaws.com\/images\/imgur\/YSdjD02.png\" alt=\"\" width=\"257\" height=\"185\" data-imgur-src=\"YSdjD02.png\" \/><br \/>\nHowever, the opposing field is so induced that does not exactly cancel the external field. It only reduces it. And the resultant electric field reduces by some value.<br \/>\nBoth polar and non-polar dielectric develop net dipole moment in the presence of an external field. The dipole moment per unit volume of the substance is called polarisation and is denoted by P for linear isotropic dielectrics. <span class=\"math-tex\">{tex}P = \\chi E{\/tex}<\/span>, <span class=\"math-tex\">{tex}\\chi {\/tex}<\/span> is the susceptibility.<\/li>\n<\/ol>\n<ol style=\"list-style-type: lower-alpha;\" start=\"1\">\n<li>At point C, inside the shell. The electric field inside a spherical shell is zero. Thus, the force experienced by the charge Q\/2 kept at the centre C of the shell will also be zero.<br \/>\n<span class=\"math-tex\">{tex}\\because F _ { C } = q E \\quad \\left( E _ { \\text { nside the shell } } = 0\\right.{\/tex}<\/span>)<br \/>\n<span class=\"math-tex\">{tex}\\therefore F _ { C } = 0{\/tex}<\/span><br \/>\nAt point &#8216;A&#8217;, magnitude of the force experienced by charge +2Q there, IF<sub>A<\/sub>= 2Q \u00d7 <span class=\"math-tex\">{tex}\\left( \\frac { 1 } { 4 \\pi \\varepsilon _ { 0 } } \\frac { 3 Q \/ 2 } { x ^ { 2 } } \\right){\/tex}<\/span> (since 3Q\/2 is the net charge of the shell)<br \/>\n<span class=\"math-tex\">{tex}\\therefore F = \\frac { 3 Q ^ { 2 } } { 4 \\pi \\varepsilon _ { 0 } x ^ { 2 } }{\/tex}<\/span> , direction of this force is away from shell<\/li>\n<li>Electric flux through the shell, <span class=\"math-tex\">{tex}\\phi = \\frac { 1 } { \\varepsilon _ { 0 } } {\/tex}<\/span> \u00d7 magnitude of the net charge enclosed by the shell. (In this case there is no effect of the charge which lies above the shell)<br \/>\n<span class=\"math-tex\">{tex}\\Rightarrow \\quad \\phi = 1 \/ \\varepsilon _ { 0 } \\times Q \/ 2 = Q \/ 2 \\varepsilon _ { 0 }{\/tex}<\/span><\/li>\n<\/ol>\n<\/li>\n<\/ol>\n<\/li>\n<\/ol>\n<h2>Chapter Wise Extra Questions of Class 12 Physics Part I &amp; Part II<\/h2>\n<ol>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-important-questions-for-class-12-physics-chapter-1\/\">Electric Charges and Fields<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-physics-chapter-2-extra-questions\/\">Electrostatic Potential and Capacitance<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/current-electricity-chapter-1-extra-questions-for-class-12-physics\/\">Current Electricity<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-physics-chapter-4-important-questions\/\">Moving Charges and Magnetism<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-physics-magnetism-and-matter-important-questions\/\">Magnetism and Matter<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/electromagnetic-induction-class-12-physics-important-questions\/\">Electromagnetic Induction<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/alternating-current-class-12-physics-extra-questions\/\">Alternating Current<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-physics-electromagnetic-waves-important-questions\/\">Electromagnetic Waves<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-physics-chapter-9-extra-questions\/\">Ray Optics and Optical<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/important-questions-for-class-12-physics-chapter-10-wave-optics\/\">Wave Optics<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-chapter-11-physics-important-questions\/\">Dual Nature of Radiation and Matter<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-atoms-chapter-12-physics-extra-questions\/\">Atoms<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-physics-chapter-13-nuclei-important-questions\/\">Nuclei<\/a><\/li>\n<li><a href=\"https:\/\/mycbseguide.com\/blog\/extra-questions-for-class-12-physics-electronic-devices\/\">Electronic Devices<\/a><\/li>\n<\/ol>\n","protected":false},"excerpt":{"rendered":"<p>CBSE Class 12 Physics Chapter 2 Extra Questions. We know Physics is tough subject within the consortium of science subjects physics is an important subject. But if you want to make career in these fields like IT Consultant, Lab Technician, Laser Engineer, Optical Engineer etc. You need to have strong fundamentals in physics to crack &#8230; <a title=\"CBSE Class 12 Physics Chapter 2 Extra Questions\" class=\"read-more\" href=\"https:\/\/mycbseguide.com\/blog\/cbse-class-12-physics-chapter-2-extra-questions\/\" aria-label=\"More on CBSE Class 12 Physics Chapter 2 Extra Questions\">Read more<\/a><\/p>\n","protected":false},"author":2,"featured_media":0,"comment_status":"open","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1346,1433],"tags":[1869,1839,1838,1833,1832,1854],"class_list":["post-28060","post","type-post","status-publish","format-standard","hentry","category-cbse","category-physics-cbse-class-12","tag-cbse-class-12-physics","tag-extra-questions","tag-important-questions","tag-latest-exam-questions","tag-practice-questions","tag-practice-test"],"yoast_head":"<!-- This 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