{"id":12694,"date":"2025-09-20T12:24:57","date_gmt":"2025-09-20T11:24:57","guid":{"rendered":"https:\/\/mcqsadda.com\/?p=12694"},"modified":"2025-10-22T10:09:22","modified_gmt":"2025-10-22T09:09:22","slug":"magnetic-effect-of-electric-current-top-100-mcqs-with-answer-and-explanation","status":"publish","type":"post","link":"https:\/\/mcqsadda.com\/index.php\/2025\/09\/20\/magnetic-effect-of-electric-current-top-100-mcqs-with-answer-and-explanation\/","title":{"rendered":"Magnetic effect of electric current Top 100 MCQs With Answer and Explanation"},"content":{"rendered":"\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">1. A magnetic field is produced by:<\/mark><\/strong><br>A) Electric charges at rest<br>B) Moving electric charges<br>C) Gravitational forces<br>D) Heat energy<br><strong>Answer:<\/strong> B) Moving electric charges<br><strong>Explanation:<\/strong> Magnetic fields arise from motion of charges (current) or changing electric fields.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\"><strong>2. The SI unit of magnetic field (magnetic flux density, B) is:<br><\/strong><\/mark>A) Tesla (T)<br>B) Weber (Wb)<br>C) Ampere (A)<br>D) Gauss<br><strong>Answer<\/strong>: A) Tesla (T)<br><strong>Explanation<\/strong>: 1 T = 1 N\/(A\u00b7m).<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">3. The direction of the magnetic field around a straight current-carrying wire is given by:<br><\/mark><\/strong>A) Fleming\u2019s left-hand rule<br>B) Right-hand thumb rule<br>C) Ampere\u2019s law<br>D) Coulomb\u2019s law<br><strong>Answer<\/strong>: B) Right-hand thumb rule<br><strong>Explanation<\/strong>: Thumb points along current, fingers curl along magnetic field direction.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">4. Magnetic field lines:<br><\/mark><\/strong>A) Start from south pole and end at north pole<br>B) Start from north pole and end at south pole<br>C) Are straight only<br>D) Are imaginary and random<br><strong>Answer<\/strong>: B) Start from north pole and end at south pole<br><strong>Explanation<\/strong>: Magnetic field lines always form closed loops outside and inside the magnet.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">5. The strength of magnetic field around a long straight wire at distance r is:<br><\/mark><\/strong>A) B=\u03bc_0 I\/2\u03c0r<br>B) B=\u03bc_0 I\/4\u03c0r^2<br>C) B=\u03bc_0 I\/r<br>D) B=I\/r^2<br><strong>Answer<\/strong>: A) B=\u03bc_0 I\/2\u03c0r<br><strong>Explanation<\/strong>: Biot\u2013Savart law for a long straight wire.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">6. Unit of magnetic flux (\u03a6) is:<br><\/mark><\/strong>A) Tesla (T)<br>B) Weber (Wb)<br>C) Ampere (A)<br>D) Henry (H)<br><strong>Answer<\/strong>: B) Weber (Wb)<br><strong>Explanation<\/strong>: Magnetic flux = B\u00b7A, unit is Wb.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">7. Fleming\u2019s left-hand rule is used to find:<br><\/mark><\/strong>A) Direction of induced current<br>B) Force on current-carrying conductor in magnetic field<br>C) Magnetic field around wire<br>D) Electric field direction<br><strong>Answer<\/strong>: B) Force on current-carrying conductor in magnetic field<br><strong>Explanation<\/strong>: Thumb = force, forefinger = field, middle finger = current.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">8. Magnitude of magnetic force on a charge q moving with velocity v in magnetic field B at angle \u03b8 is:<br><\/mark><\/strong>A) F=qvB<br>B) F=qvBsin\u2061\u03b8<br>C) F=qvBcos\u2061\u03b8<br>D) F=qv^2 B<br><strong>Answer<\/strong>: B) F=qvBsin\u2061\u03b8<br><strong>Explanation<\/strong>: Force is maximum when velocity is perpendicular to field.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">9. A charge moving parallel to magnetic field experiences:<br><\/mark><\/strong>A) Maximum force<br>B) Zero force<br>C) Half force<br>D) Depends on speed<br><strong>Answer<\/strong>: B) Zero force<br><strong>Explanation<\/strong>: F = qvB sin \u03b8 \u2192 \u03b8 = 0\u00b0 \u2192 F = 0.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">10. Unit of magnetic moment (\u03bc) is:<br><\/mark><\/strong>A) A\u00b7m\u00b2<br>B) N\u00b7m<br>C) Tesla<br>D) Weber<br><strong>Answer<\/strong>: A) A\u00b7m\u00b2<br><strong>Explanation<\/strong>: \u03bc = I\u00b7A, current \u00d7 area.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">11. Torque on a current-carrying loop in uniform magnetic field is:<br><\/mark><\/strong>A) \u03c4 = B I A sin \u03b8<br>B) \u03c4 = B I A cos \u03b8<br>C) \u03c4 = B I A<br>D) \u03c4 = 0<br><strong>Answer<\/strong>: A) \u03c4 = B I A sin \u03b8<br><strong>Explanation<\/strong>: \u03b8 = angle between plane of loop and field.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">12. A compass needle aligns along:<br><\/mark><\/strong>A) Electric field<br>B) Magnetic field<br>C) Current direction<br>D) Gravity<br><strong>Answer<\/strong>: B) Magnetic field<br><strong>Explanation<\/strong>: Needle aligns along local magnetic field lines.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">13. A solenoid behaves like:<br><\/mark><\/strong>A) Permanent magnet<br>B) Electromagnet<br>C) Capacitor<br>D) Resistor<br><strong>Answer<\/strong>: B) Electromagnet<br><strong>Explanation<\/strong>: Current through coil produces magnetic field similar to bar magnet.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">14. Magnetic field at the center of a circular current loop of radius R is:<br><\/mark><\/strong>A) B=\u03bc_0 I\/2R<br>B) B=\u03bc_0 I\/2\u03c0R<br>C) B=\u03bc_0 I\/4\u03c0R^2<br>D) B=\u03bc_0 I\/R^2<br><strong>Answer<\/strong>: A) B=\u03bc_0 I\/2R<br><strong>Explanation<\/strong>: From Biot\u2013Savart law for a circular loop.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">15. Magnetic lines of force are:<br><\/mark><\/strong>A) Closed curves<br>B) Open curves<br>C) Straight only<br>D) Random<br><strong>Answer<\/strong>: A) Closed curves<br><strong>Explanation<\/strong>: They start from N pole and end at S pole outside magnet, forming loops inside.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">16. Magnetic field inside a long solenoid of n turns\/m and current I is:<br><\/mark><\/strong>A) B = \u03bc\u2080 n I<br>B) B = \u03bc\u2080 I \/ 2\u03c0 r<br>C) B = \u03bc\u2080 I n\u00b2<br>D) B = \u03bc\u2080 I \/ L<br><strong>Answer<\/strong>: A) B = \u03bc\u2080 n I<br><strong>Explanation<\/strong>: Field inside solenoid is uniform.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">17. Direction of magnetic field inside solenoid is determined by:<br><\/mark><\/strong>A) Fleming\u2019s left-hand rule<br>B) Right-hand screw rule<br>C) Biot\u2013Savart law<br>D) Coulomb\u2019s law<br><strong>Answer<\/strong>: B) Right-hand screw rule<br><strong>Explanation<\/strong>: Curl fingers along current, thumb gives field direction.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">18. Two parallel wires carrying current in same direction:<br><\/mark><\/strong>A) Repel<br>B) Attract<br>C) No force<br>D) Depends on current<br><strong>Answer<\/strong>: B) Attract<br><strong>Explanation<\/strong>: Magnetic field produced by each wire exerts force on the other.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">19. Two parallel wires carrying current in opposite direction:<br><\/mark><\/strong>A) Attract<br>B) Repel<br>C) Neutral<br>D) None<br><strong>Answer<\/strong>: B) Repel<br><strong>Explanation<\/strong>: Currents in opposite direction produce opposing fields \u2192 repulsion.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">20. Ampere\u2019s force between two parallel wires:<br><\/mark><\/strong>A) F\/L=(\u03bc_0 I_1 I_2)\/2\u03c0d<br>B) F\/L=(\u03bc_0 I_1 I_2)\/d^2<br>C) F\/L=\u03bc_0 I_1 I_2<br>D) F = 0<br><strong>Answer<\/strong>: A) F\/L=(\u03bc_0 I_1 I_2)\/2\u03c0d<br><strong>Explanation<\/strong>: Standard formula for force per unit length.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">21. Magnetic field at point due to infinite straight wire decreases with:<br><\/mark><\/strong>A) 1\/r<br>B) 1\/r\u00b2<br>C) r\u00b2<br>D) r<br><strong>Answer<\/strong>: A) 1\/r<br><strong>Explanation<\/strong>: Biot\u2013Savart law for straight wire: B \u221d 1\/r.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">22. SI unit of magnetic dipole moment:<br><\/mark><\/strong>A) A\u00b7m\u00b2<br>B) N\u00b7m<br>C) J\/T<br>D) Both A &amp; C<br><strong>Answer<\/strong>: D) Both A &amp; C<br><strong>Explanation<\/strong>: \u03bc = I\u00b7A = torque\/field, both units equivalent.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">23. A charge moving in a magnetic field in circular path has:<br><\/mark><\/strong>A) Constant speed<br>B) Zero acceleration<br>C) Zero force<br>D) Increasing speed<br><strong>Answer<\/strong>: A) Constant speed<br><strong>Explanation<\/strong>: Magnetic force is perpendicular to velocity \u2192 centripetal motion, speed constant.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">24. Radius of circular path of charge q, mass m, velocity v in perpendicular B:<br><\/mark><\/strong>A) r = mv\/qB<br>B) r = qB\/mv<br>C) r = mv\u00b2\/qB<br>D) r = qBv\/m<br><strong>Answer<\/strong>: A) r = mv\/qB<br><strong>Explanation<\/strong>: Centripetal force mv\u00b2\/r = qvB \u2192 r = mv\/qB.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">25. Time period of circular motion of charge in uniform magnetic field:<br><\/mark><\/strong>A) T=2\u03c0m\/qB<br>B) T=2\u03c0q\/mB<br>C) T=2\u03c0m\/q<br>D) T=q\/mB<br><strong>Answer<\/strong>: A) T=2\u03c0m\/qB<br><strong>Explanation:<\/strong> T = 2\u03c0r\/v = 2\u03c0 m\/qB.<br><\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">26. The magnetic field at a point due to a small current element I&#8221;\u2009&#8221; dlis given by:<br><\/mark><\/strong>A) Ampere\u2019s law<br>B) Biot\u2013Savart law<br>C) Faraday\u2019s law<br>D) Coulomb\u2019s law<br><strong>Answer<\/strong>: B) Biot\u2013Savart law<br><strong>Explanation:<\/strong> Biot\u2013Savart law relates a small current element to the magnetic field it produces at a point.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">27. Magnetic field due to a small current element Idlat distance r is:<br><\/mark><\/strong>A) dB\u221dIdl\/r<br>B) dB\u221dIdl\/r^2<br>C) dB\u221dIdl\/r^3<br>D) dB\u221dIdl<br><strong>Answer:<\/strong> B) dB\u221dIdl\/r^2<br><strong>Explanation<\/strong>: Biot\u2013Savart law: dB \u20d7=(\u03bc_0\/4\u03c0)(I&#8221;\u2009&#8221; dl \u20d7\u00d7r \u0302)\/r^2.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">28. Direction of magnetic field due to current element is:<br><\/mark><\/strong>A) Along current<br>B) Along radius<br>C) Perpendicular to plane of current element and radius vector<br>D) Opposite to current<br><strong>Answer<\/strong>: C) Perpendicular to plane of current element and radius vector<br><strong>Explanation<\/strong>: Cross product in Biot\u2013Savart law gives direction.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">29. Magnetic field at center of circular loop of radius R carrying current I:<br><\/mark><\/strong>A) B=\u03bc_0 I\/2\u03c0R<br>B) B=\u03bc_0 I\/2R<br>C) B=\u03bc_0 I\/4\u03c0R^2<br>D) B=\u03bc_0 I\/R^2<br><strong>Answer:<\/strong> B) B=\u03bc_0 I\/2R<br><strong>Explanation:<\/strong> Biot\u2013Savart integration over circular loop.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">30. Field at the center of a semicircular wire of radius R carrying current I:<br><\/mark><\/strong>A) B=\u03bc_0 I\/4R<br>B) B=\u03bc_0 I\/2R<br>C) B=\u03bc_0 I\/4\u03c0R<br>D) B=\u03bc_0 I\/8R<br><strong>Answer:<\/strong> A) B=\u03bc_0 I\/4R<br><strong>Explanation<\/strong>: B = (\u03bc\u2080 I \/ 4R) for semicircle (half of full circle).<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">31. Magnetic field at the axis of a solenoid (length L >> radius) with n turns\/m and current I:<br><\/mark><\/strong>A) B=\u03bc_0 nI<br>B) B=\u03bc_0 I\/2R<br>C) B=\u03bc_0 In^2<br>D) B=\u03bc_0 IL<br><strong>Answer<\/strong>: A) B=\u03bc_0 nI<br><strong>Explanation<\/strong>: Field inside long solenoid uniform.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">32. Magnetic field inside a toroid of mean radius R and N turns carrying current I:<br><\/mark><\/strong>A) B=\u03bc_0 NI\/2\u03c0R<br>B) B=\u03bc_0 NI\/R<br>C) B=\u03bc_0 I\/2R<br>D) B=\u03bc_0 I\/2\u03c0R^2<br><strong>Answer<\/strong>: A) B=\u03bc_0 NI\/2\u03c0R<br><strong>Explanation<\/strong>: Field confined inside toroid, derived via Ampere\u2019s law.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">33. Ampere\u2019s circuital law states:<br><\/mark><\/strong>A) Magnetic field along path = \u03bc\u2080 \u00d7 total current enclosed<br>B) \u222eB \u20d7\u22c5dl \u20d7=\u03bc_0 I_enclosed<br>C) Magnetic field due to charges only<br>D) Both A &amp; B<br><strong>Answer<\/strong>: D) Both A &amp; B<br><strong>Explanation<\/strong>: Ampere\u2019s law relates line integral of B to current enclosed.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">34. For a straight wire, Ampere\u2019s law gives:<br><\/mark><\/strong>A) B=\u03bc_0 I\/2\u03c0r<br>B) B=\u03bc_0 I\/2R<br>C) B=\u03bc_0 I\/R^2<br>D) B=\u03bc_0 I\/4\u03c0R^2<br><strong>Answer<\/strong>: A) B=\u03bc_0 I\/2\u03c0r<br><strong>Explanation<\/strong>: Same as Biot\u2013Savart for long straight wire.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">35. Magnetic field inside an ideal solenoid is:<br><\/mark><\/strong>A) Non-uniform<br>B) Uniform and along axis<br>C) Zero<br>D) Radial<br><strong>Answer<\/strong>: B) Uniform and along axis<br><strong>Explanation<\/strong>: Superposition of fields from all turns produces uniform field.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">36. For circular current loop, magnetic moment \u03bc =<br><\/mark><\/strong>A) I \u00d7 circumference<br>B) I \u00d7 area of loop<br>C) B \u00d7 area<br>D) I\u00b2 \u00d7 area<br><strong>Answer<\/strong>: B) I \u00d7 area of loop<br><strong>Explanation<\/strong>: \u03bc = I\u00b7A, defines strength of current loop.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">37. Unit of magnetic moment in SI:<br><\/mark><\/strong>A) Tesla<br>B) Ampere\u00b7m\u00b2<br>C) Weber<br>D) Henry<br><strong>Answer: <\/strong>B) Ampere\u00b7m\u00b2<br><strong>Explanation<\/strong>: \u03bc = I \u00d7 A \u2192 unit A\u00b7m\u00b2.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">38. Torque on current-carrying loop in uniform B field:<br><\/mark><\/strong>A) \u03c4 = \u03bc B sin \u03b8<br>B) \u03c4 = \u03bc B cos \u03b8<br>C) \u03c4 = \u03bc B<br>D) \u03c4 = 0<br><strong>Answer<\/strong>: A) \u03c4 = \u03bc B sin \u03b8<br><strong>Explanation:<\/strong> \u03b8 = angle between \u03bc and B.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">39. Potential energy of magnetic dipole in magnetic field:<br><\/mark><\/strong>A) U = \u2013 \u03bc \u00b7 B<br>B) U = \u03bc \u00b7 B<br>C) U = \u03bc \/ B<br>D) U = 0<br><strong>Answer<\/strong>: A) U = \u2013 \u03bc \u00b7 B<br><strong>Explanation<\/strong>: Minimum energy when \u03bc aligns with B.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">40. Right-hand screw rule determines:<br><\/mark><\/strong>A) Current direction from B<br>B) B direction around current<br>C) Force on conductor<br>D) Magnetic flux<br><strong>Answer<\/strong>: B) B direction around current<br><strong>Explanation<\/strong>: Curl fingers along rotation, thumb shows current.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">41. Two parallel wires carrying currents in same direction experience:<br><\/mark><\/strong>A) Repulsion<br>B) Attraction<br>C) No force<br>D) Varies with distance<br><strong>Answer<\/strong>: B) Attraction<br><strong>Explanation<\/strong>: Like currents attract; basis of defining ampere.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">42. Unit force per unit length between parallel wires:<br><\/mark><\/strong>A) 2\u00d710\u207b\u2077 N\/m per 1 A current separated by 1 m<br>B) 10\u207b\u2077 N\/m<br>C) 1 N\/m<br>D) 10\u207b\u00b3 N\/m<br><strong>Answer<\/strong>: A) 2\u00d710\u207b\u2077 N\/m per 1 A current separated by 1 m<br><strong>Explanation<\/strong>: Defines 1 Ampere.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">43. Magnetic field at distance r from infinite wire decreases as:<br><\/mark><\/strong>A) 1\/r\u00b2<br>B) 1\/r<br>C) r\u00b2<br>D) r<br><strong>Answer<\/strong>: B) 1\/r<br><strong>Explanation<\/strong>: Biot\u2013Savart law: B \u221d 1\/r.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">44. Magnetic field outside a very long solenoid is:<br><\/mark><\/strong>A) Uniform<br>B) Zero<br>C) Maximum<br>D) Same as inside<br><strong>Answer<\/strong>: B) Zero<br><strong>Explanation<\/strong>: Fields from turns cancel outside.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">45. Magnetic field inside toroid:<br><\/mark><\/strong>A) Uniform along circular path<br>B) Radial<br>C) Zero<br>D) Tangential but varying<br><strong>Answer<\/strong>: A) Uniform along circular path<br><strong>Explanation<\/strong>: Symmetry \u2192 B constant along each circular loop.<br><\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">46. A current-carrying loop produces field:<br><\/mark><\/strong>A) Only at center<br>B) Along axis<br>C) Uniform everywhere<br>D) None<br><strong>Answer<\/strong>: B) Along axis<br><strong>Explanation<\/strong>: B strongest at center, decreases along axis.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">47. Magnetic field at axis of circular coil of N turns:<br><\/mark><\/strong>A) B=\u03bc_0 NI\/2R<br>B) B=\u03bc_0 I\/2R<br>C) B=\u03bc_0 I\/R<br>D) B=\u03bc_0 NI\/R<br><strong>Answer<\/strong>: A) B=\u03bc_0 NI\/2R<br><strong>Explanation<\/strong>: Multiply single loop field by N turns.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">48. Magnetic field at point on axis of short solenoid:<br><\/mark><\/strong>A) Uniform<br>B) Non-uniform<br>C) Zero<br>D) Radial<br><strong>Answer<\/strong>: B) Non-uniform<br><strong>Explanation<\/strong>: Only long solenoid approximates uniform field.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">49. For long straight wire, magnetic field at 1 m from 1 A current:<br><\/mark><\/strong>A) 2\u00d710^(-7) T<br>B) 10^(-7) T<br>C) 4\u00d710^(-7) T<br>D) 8\u00d710^(-7) T<br><strong>Answer<\/strong>: A) 2\u00d710^(-7) T<br><strong>Explanation<\/strong>: B = \u03bc\u2080 I \/ 2\u03c0r \u2192 \u03bc\u2080 = 4\u03c0\u00d710\u207b\u2077.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">50. Magnetic field of coil increases by:<br><\/mark><\/strong>A) Increasing current<br>B) Increasing number of turns<br>C) Reducing coil radius<br>D) All of above<br><strong>Answer<\/strong>: D) All of above<br><strong>Explanation<\/strong>: B \u221d N I \/ R.<br><\/p>\n\n\n\n<p class=\"has-large-font-size\"><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\"><strong>51. Electromagnetic induction is the phenomenon of:<\/strong><br><\/mark>A) Generation of magnetic field by current<br>B) Induction of current in a conductor due to changing magnetic field<br>C) Attraction between magnets<br>D) Magnetic field due to moving charges<br><strong>Answer<\/strong>: B) Induction of current in a conductor due to changing magnetic field<br><strong>Explanation<\/strong>: Faraday\u2019s experiments showed changing flux induces current.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">52. Faraday\u2019s law states:<br><\/mark><\/strong>A) Induced emf \u221d magnetic field<br>B) Induced emf \u221d rate of change of magnetic flux<br>C) Induced emf \u221d current<br>D) Induced emf \u221d resistance<br><strong>Answer<\/strong>: B) Induced emf \u221d rate of change of magnetic flux<br><strong>Explanation<\/strong>: E=-d\u03a6_B\/dt<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">53. Lenz\u2019s law gives:<br><\/mark><\/strong>A) Direction of induced current<br>B) Magnitude of induced current<br>C) Both direction and magnitude<br>D) None<br><strong>Answer<\/strong>: A) Direction of induced current<br><strong>Explanation<\/strong>: Induced current opposes change in flux (conservation of energy).<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">54. Unit of magnetic flux (\u03a6) is:<br><\/mark><\/strong>A) Tesla<br>B) Weber<br>C) Ampere\u00b7turn<br>D) Henry<br><strong>Answer<\/strong>: B) Weber (Wb)<br><strong>Explanation<\/strong>: Flux = B\u00b7A, 1 Wb = 1 T\u00b7m\u00b2.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">55. Unit of induced emf is:<br><\/mark><\/strong>A) Tesla<br>B) Volt<br>C) Weber<br>D) Ampere<br><strong>Answer<\/strong>: B) Volt<br><strong>Explanation<\/strong>: EMF is potential difference induced.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">56. A conductor moving in uniform magnetic field experiences:<br><\/mark><\/strong>A) Constant magnetic flux<br>B) Induced emf<br>C) Zero current<br>D) Zero voltage<br><strong>Answer<\/strong>: B) Induced emf<br><strong>Explanation<\/strong>: Motion changes flux through conductor \u2192 Faraday\u2019s law.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">57. Induced emf in a coil rotating in uniform B-field is maximum when:<br><\/mark><\/strong>A) Plane of coil parallel to field<br>B) Plane of coil perpendicular to field<br>C) Coil stationary<br>D) Coil axis perpendicular to field<br><strong>Answer<\/strong>: B) Plane of coil perpendicular to field<br><strong>Explanation<\/strong>: Flux changes fastest \u2192 max emf.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">58. Induced emf in coil:<br><\/mark><\/strong>A) Zero if flux constant<br>B) Max if flux changes fastest<br>C) Always constant<br>D) Depends on coil material<br><strong>Answer<\/strong>: A) Zero if flux constant<br><strong>Explanation<\/strong>: No change in flux \u2192 no induced emf.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">59. EMF induced in a coil of N turns:<br><\/mark><\/strong>A) E=Nd\u03a6\/dt<br>B) E=d\u03a6\/dt<br>C) E=N\u03a6<br>D) E=NI<br><strong>Answer<\/strong>: A) E=Nd\u03a6\/dt<br><strong>Explanation<\/strong>: Faraday\u2019s law generalized for N turns.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">60. A bar magnet moving toward a coil induces:<br><\/mark><\/strong>A) Current in same direction as flux change<br>B) Current opposing flux change<br>C) Zero current<br>D) Infinite current<br><strong>Answer<\/strong>: B) Current opposing flux change<br><strong>Explanation<\/strong>: Lenz\u2019s law ensures induced current opposes motion.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">61. Magnetic flux through coil of area A in uniform B:<br><\/mark><\/strong>A) \u03a6=B\/A<br>B) \u03a6=B\u22c5Acos\u2061\u03b8<br>C) \u03a6=B+A<br>D) \u03a6=BA\/\u03b8<br><strong>Answer<\/strong>: B) \u03a6=B\u22c5Acos\u2061\u03b8<br><strong>Explanation<\/strong>: \u03b8 = angle between B and normal to plane of coil.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">62. Motional emf is generated due to:<br><\/mark><\/strong>A) Changing B-field<br>B) Motion of conductor in B-field<br>C) Resistance<br>D) Temperature<br><strong>Answer<\/strong>: B) Motion of conductor in B-field<br><strong>Explanation<\/strong>: Conductor cuts magnetic lines \u2192 induced emf.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">63. EMF induced in rod of length l moving with velocity v perpendicular to B:<br><\/mark><\/strong>A) E=Blv<br>B) E=Bl\/v<br>C) E=Blv^2<br>D) E=B\/lv<br><strong>Answer<\/strong>: A) E=Blv<br><strong>Explanation<\/strong>: Motional emf formula: \u03b5 = B l v.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">64. Eddy currents are induced in:<br><\/mark><\/strong>A) Insulators<br>B) Conductors<br>C) Non-conductors<br>D) Vacuum<br><strong>Answer<\/strong>: B) Conductors<br><strong>Explanation<\/strong>: Loop currents induced in bulk of conducting material.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">65. Lenz\u2019s law ensures:<br><\/mark><\/strong>A) Energy conservation<br>B) Maximum current<br>C) Minimum resistance<br>D) None<br><strong>Answer<\/strong>: A) Energy conservation<br><strong>Explanation<\/strong>: Induced current always opposes change \u2192 work done = energy.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">66. Direction of induced current in moving magnet-coil system given by:<br><\/mark><\/strong>A) Right-hand rule<br>B) Left-hand rule<br>C) Fleming\u2019s right-hand rule<br>D) Fleming\u2019s left-hand rule<br><strong>Answer<\/strong>: C) Fleming\u2019s right-hand rule<br><strong>Explanation<\/strong>: Right-hand rule for generators \u2192 direction of induced current.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">67. Changing area of loop in uniform B produces:<br><\/mark><\/strong>A) No EMF<br>B) Induced EMF<br>C) Only flux<br>D) Only torque<br><strong>Answer<\/strong>: B) Induced EMF<br><strong>Explanation<\/strong>: Change in flux (B\u00b7A) \u2192 EMF induced.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">68. Self-induction occurs due to:<br><\/mark><\/strong>A) Mutual induction<br>B) Changing current in same coil<br>C) Static magnetic field<br>D) Electrostatics<br><strong>Answer:<\/strong> B) Changing current in same coil<br><strong>Explanation<\/strong>: Time-varying current induces EMF in same coil \u2192 Lenz\u2019s law.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">69. Inductance unit:<\/mark><\/strong><br>A) Weber<br>B) Henry<br>C) Tesla<br>D) Volt<br><strong>Answe<\/strong>r: B) Henry (H)<br><strong>Explanation:<\/strong> L = EMF \/ (dI\/dt).<br><\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">70. Mutual induction occurs when:<br><\/mark><\/strong>A) EMF induced in one coil due to current change in another coil<br>B) EMF induced in same coil<br>C) Magnetic field is uniform<br>D) Current constant<br><strong>Answer:<\/strong> A) EMF induced in one coil due to current change in another coil<br><strong>Explanation<\/strong>: Basis for transformers.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">71. Transformer works on principle of:<br><\/mark><\/strong>A) Self-induction only<br>B) Mutual induction<br>C) Static electricity<br>D) Magnetic monopoles<br><strong>Answer<\/strong>: B) Mutual induction<br><strong>Explanation<\/strong>: Changing current in primary \u2192 changing flux \u2192 induces EMF in secondary.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">72. Induced EMF in secondary coil:<br><\/mark><\/strong>A) Directly proportional to turns of secondary<br>B) Inversely proportional to primary turns<br>C) Independent of turns<br>D) Zero<br><strong>Answer<\/strong>: A) Directly proportional to turns of secondary<br><strong>Explanation<\/strong>: Faraday\u2019s law: \u03b5 \u221d N d\u03a6\/dt.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">73. Energy stored in inductor L carrying current I:<br><\/mark><\/strong>A) U=1\/2 LI^2<br>B) U=LI<br>C) U=1\/2 I^2\/L<br>D) U=I\/L<br><strong>Answer<\/strong>: A) U=1\/2 LI^2<br><strong>Explanation<\/strong>: Energy stored in magnetic field of inductor.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">74. Back EMF in motor opposes:<br><\/mark><\/strong>A) Applied voltage<br>B) Magnetic field<br>C) Current flow<br>D) Resistance<br><strong>Answer<\/strong>: C) Current flow<br><strong>Explanation<\/strong>: Lenz\u2019s law: induced EMF opposes cause (current) in coil.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">75. EMF induced is maximum when:<br><\/mark><\/strong>A) Magnetic flux changes fastest<br>B) Flux constant<br>C) Coil stationary<br>D) Coil parallel to field<br><strong>Answer<\/strong>: A) Magnetic flux changes fastest<br><strong>Explanation<\/strong>: Rate of change of flux determines EMF magnitude.<br><\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">76. The device which converts electrical energy into mechanical energy is:<br><\/mark><\/strong>A) Generator<br>B) Motor<br>C) Transformer<br>D) Dynamo<br><strong>Answer<\/strong>: B) Motor<br><strong>Explanation<\/strong>: Electric motor works on principle of force on current-carrying conductor in magnetic field.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">77. The device which converts mechanical energy into electrical energy is:<br><\/mark><\/strong>A) Motor<br>B) Generator<br>C) Transformer<br>D) Battery<br><strong>Answer<\/strong>: B) Generator<br><strong>Explanation<\/strong>: Electromagnetic induction principle: rotating coil in B-field produces EMF.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">78. The principle of DC motor is:<br><\/mark><\/strong>A) Electromagnetic induction<br>B) Force on current-carrying conductor in magnetic field<br>C) Mutual induction<br>D) Self-induction<br><strong>Answer<\/strong>: B) Force on current-carrying conductor in magnetic field<br><strong>Explanation<\/strong>: Torque on loop \u2192 rotation.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">79. Torque on rectangular coil in motor is maximum when plane of coil is:<br><\/mark><\/strong>A) Parallel to magnetic field<br>B) Perpendicular to magnetic field<br>C) At 45\u00b0 to field<br>D) Any orientation<br><strong>Answer<\/strong>: B) Perpendicular to magnetic field<br><strong>Explanation<\/strong>: Torque \u03c4 = \u03bcB sin \u03b8 \u2192 maximum at \u03b8 = 90\u00b0.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">80. Back EMF in motor is produced due to:<br><\/mark><\/strong>A) Motion of coil in magnetic field<br>B) Resistance of coil<br>C) Supply voltage<br>D) Magnetic flux<br><strong>Answer<\/strong>: A) Motion of coil in magnetic field<br><strong>Explanation<\/strong>: EMF induced opposes applied voltage, limiting current.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">81. Transformer operates on:<br><\/mark><\/strong>A) DC supply<br>B) AC supply<br>C) Constant current<br>D) None<br><strong>Answer<\/strong>: B) AC supply<br><strong>Explanation<\/strong>: Only changing flux (AC) induces EMF in secondary.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">82. Step-up transformer increases:<br><\/mark><\/strong>A) Current<br>B) Voltage<br>C) Resistance<br>D) Power<br><strong>Answer<\/strong>: B) Voltage<br><strong>Explanation<\/strong>: V\u2082\/V\u2081 = N\u2082\/N\u2081 \u2192 N\u2082 > N\u2081 \u2192 voltage increases.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">83. Step-down transformer decreases:<br><\/mark><\/strong>A) Voltage<br>B) Current<br>C) Resistance<br>D) Power<br><strong>Answer<\/strong>: A) Voltage<br><strong>Explanation<\/strong>: N\u2082 &lt; N\u2081 \u2192 V\u2082 &lt; V\u2081.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">84. Efficiency of ideal transformer:<br><\/mark><\/strong>A) 50%<br>B) 75%<br>C) 100%<br>D) 0%<br><strong>Answer<\/strong>: C) 100%<br><strong>Explanation<\/strong>: Ideal \u2192 negligible losses, power in = power out.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">85. Energy loss in transformer occurs due to:<br><\/mark><\/strong>A) Eddy currents<br>B) Hysteresis<br>C) Resistance of coil<br>D) All of the above<br><strong>Answer<\/strong>: D) All of the above<br><strong>Explanation<\/strong>: Real transformers have losses due to these factors.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">86. Induced EMF in rotating coil of generator is maximum when plane of coil is:<br><\/mark><\/strong>A) Parallel to B-field<br>B) Perpendicular to B-field<br>C) Stationary<br>D) At 45\u00b0<br><strong>Answer<\/strong>: A) Parallel to B-field<br><strong>Explanation<\/strong>: Rate of change of flux maximum when plane parallel (axis perpendicular).<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">87. Frequency of AC induced in generator depends on:<br><\/mark><\/strong>A) Number of turns only<br>B) Speed of rotation only<br>C) Both speed and number of poles<br>D) Voltage applied<br><strong>Answer<\/strong>: C) Both speed and number of poles<br><strong>Explanation<\/strong>: f = (np)\/120 for n rpm, p poles.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">88. In AC generator, slip rings:<br><\/mark><\/strong>A) Connect coil to external circuit continuously<br>B) Reverse current direction<br>C) Act as brushes<br>D) None<br><strong>Answer<\/strong>: A) Connect coil to external circuit continuously<br><strong>Explanation<\/strong>: Allow AC output; contrast with commutator in DC.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">89. In DC generator, commutator:<br><\/mark><\/strong>A) Produces AC<br>B) Converts AC to DC<br>C) Increases voltage<br>D) Reduces resistance<br><strong>Answer<\/strong>: B) Converts AC to DC<br><strong>Explanation<\/strong>: Segmented commutator reverses current direction in coil \u2192 DC output.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">90. RMS value of AC:<br><\/mark><\/strong>A) Maximum value<br>B) Average value<br>C) V_rms=V_0\/\u221a2<br>D) Twice max value<br><strong>Answer<\/strong>: C) V_rms=V_0\/\u221a2<br><strong>Explanation<\/strong>: Standard relation for sinusoidal AC.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">91. Peak value of AC current I\u2080 related to RMS I:<br><\/mark><\/strong>A) I_0=I_rms<br>B) I_0=\u221a2 I_rms<br>C) I_0=I_rms\/2<br>D) I_0=2I_rms<br><strong>Answer<\/strong>: B) I_0=\u221a2 I_rms<br><strong>Explanation<\/strong>: RMS is effective value: I_rms=I_0\/\u221a2.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">92. Induced EMF in rod moving in uniform B-field:<br><\/mark><\/strong>A) E=Blv<br>B) E=B\/lv<br>C) E=Bv\/l<br>D) E=Bv^2 l<br><strong>Answer<\/strong>: A) E=Blv<br><strong>Explanation<\/strong>: Motional EMF formula.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">93. Induced current in short-circuited coil opposes:<br><\/mark><\/strong>A) Change in flux<br>B) Voltage supply<br>C) Resistance<br>D) None<br><strong>Answer<\/strong>: A) Change in flux<br><strong>Explanation<\/strong>: Lenz\u2019s law.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">94. A loop rotating in B-field experiences torque:<br><\/mark><\/strong>A) \u03c4 = \u03bcB sin \u03b8<br>B) \u03c4 = \u03bcB cos \u03b8<br>C) \u03c4 = \u03bcB<br>D) \u03c4 = 0<br><strong>Answer<\/strong>: A) \u03c4 = \u03bcB sin \u03b8<br><strong>Explanation<\/strong>: Standard torque formula for magnetic dipole.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">95. Hall effect helps measure:<br><\/mark><\/strong>A) Magnetic field<br>B) Charge carrier density<br>C) Current type (electrons\/holes)<br>D) All of the above<br><strong>Answer<\/strong>: D) All of the above<br><strong>Explanation<\/strong>: Hall voltage depends on B, carrier density, and charge sign.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">96. Direction of Hall voltage determined by:<br><\/mark><\/strong>A) Fleming\u2019s left-hand rule<br>B) Right-hand rule<br>C) Lenz\u2019s law<br>D) Biot\u2013Savart law<br><strong>Answer<\/strong>: B) Right-hand rule<br><strong>Explanation<\/strong>: For conventional current and magnetic field, right-hand gives sign.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">97. In magnetic braking, eddy currents:<br><\/mark><\/strong>A) Slow motion of conductor<br>B) Accelerate motion<br>C) Generate power only<br>D) Heat nothing<br><strong>Answer<\/strong>: A) Slow motion of conductor<br><strong>Explanation<\/strong>: Lenz\u2019s law \u2192 currents oppose motion \u2192 braking effect.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">98. Magnetic flux linkage in coil:<br><\/mark><\/strong>A) \u03a6 \u00d7 N<br>B) B \u00d7 A<br>C) \u03bc\u2080 I<br>D) None<br><strong>Answer<\/strong>: A) \u03a6 \u00d7 N<br><strong>Explanation<\/strong>: Flux through N turns \u2192 total flux linkage.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">99. Energy stored in inductor:<br><\/mark><\/strong>A) U = \u00bd L I\u00b2<br>B) U = L I<br>C) U = LI\u00b2<br>D) U = \u00bd I\u00b2\/L<br><strong>Answer<\/strong>: A) U = \u00bd L I\u00b2<br><strong>Explanation<\/strong>: Magnetic energy stored in inductor field.<\/p>\n\n\n\n<p class=\"has-large-font-size\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">100. Which of the following is NOT an application of electromagnetic induction?<br><\/mark><\/strong>A) Transformer<br>B) AC generator<br>C) Electric motor<br>D) Electric heater<br><strong>Answer<\/strong>: D) Electric heater<br><strong>Explanation<\/strong>: Heater works by resistive heating, not induction.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>1. A magnetic field is produced by:A) Electric charges at restB) Moving electric chargesC) Gravitational forcesD) Heat energyAnswer: B) Moving electric chargesExplanation: Magnetic fields arise from motion of charges (current) or changing electric fields. 2. The SI unit of magnetic field (magnetic flux density, B) is:A) Tesla (T)B) Weber (Wb)C) Ampere (A)D) GaussAnswer: A) Tesla<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[8],"tags":[15737,15481,15857,15821,15720,15819,15859,15816,15727,15855,15736,15854,10964,15858,15729,15853,15738,4029,5649,15465,5623,15856,15536,15479,15474,15467,15483,15472,15592,15456,15478,15735,15469,15480],"class_list":{"0":"post-12694","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-physics","7":"tag-amperes-law","8":"tag-competitive-exam-physics","9":"tag-current-and-magnetism","10":"tag-electric-circuits","11":"tag-electric-current","12":"tag-electromagnet","13":"tag-electromagnetic-concepts","14":"tag-electromagnetic-induction","15":"tag-electromagnetism","16":"tag-flemings-left-hand-rule","17":"tag-lorentz-force","18":"tag-magnetic-effect-of-electric-current","19":"tag-magnetic-effect-of-electric-current-top-100-mcqs-with-answer-and-explanation","20":"tag-magnetic-effects","21":"tag-magnetic-field","22":"tag-magnetic-force-problems","23":"tag-magnetic-lines-of-force","24":"tag-mcqs-adda","25":"tag-mcqs-for-pc-psi-sda-fda-pdo-vao-banking-kas-ias-ssc-gd-ssc-chsl-ssc-cgl-for-all-compitative-exams","26":"tag-mcqs-for-physics-exam","27":"tag-mcqs-for-sda-fda-pdo-vao-banking-kas-ias-ssc-gd-ssc-chsl-ssc-cgl-for-all-compitative-exams","28":"tag-oersted-experiment","29":"tag-physics-formulas","30":"tag-physics-learning","31":"tag-physics-mcqs","32":"tag-physics-preparation-material","33":"tag-physics-questions-and-answers","34":"tag-physics-quiz","35":"tag-physics-revision","36":"tag-physics-study-material","37":"tag-psc-physics-mcqs","38":"tag-solenoid","39":"tag-ssc-physics-mcqs","40":"tag-upsc-physics-mcqs"},"_links":{"self":[{"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/posts\/12694","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/comments?post=12694"}],"version-history":[{"count":3,"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/posts\/12694\/revisions"}],"predecessor-version":[{"id":12725,"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/posts\/12694\/revisions\/12725"}],"wp:attachment":[{"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/media?parent=12694"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/categories?post=12694"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/mcqsadda.com\/index.php\/wp-json\/wp\/v2\/tags?post=12694"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}