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NTA Abhyas 2020
Exam
NTA Abhyas
Year
2020
Subject
Physics
Chapter
Electromagnetic Induction

NTA Abhyas 2020 · Physics · Electromagnetic Induction

A long solenoid of cross-sectional radius R has a thin insulated...

A long solenoid of cross-sectional radius RR has a thin insulated wire ring of uniform cross-section tightly put on its winding. The ring is made out of two different material such that one half of the ring has a resistance 1010 times that of the other half. The magnetic induction produced by the solenoid varies with time as B=btB = bt, where bb is a constant. The magnitude of the electric field strength in the ring (other than the induced electric field) isA long solenoid of cross-sectional radius R has a thin insulated wire ring of uniform cross-section tightly put on its

Options

  1. A911Rb\dfrac{9}{11}Rb
  2. B922Rb\dfrac{9}{22}Rb
  3. C9Rb9Rb
  4. DRbRb

Correct answer

B. 922Rb\dfrac{9}{22}Rb

Step-by-step solution

Let us assume that the current in the ring is ii and the resistance of the two halves are rr and 10r10r, then by faraday's law

\left|\dfrac{dϕ}{dt}\right| = \pi{R}^{2}b = ir + i\left(10r\right)</p><p></p><p>⇒ i = \dfrac{\pi{R}^{2}b}{11r}</p><p>Theinducedelectricfieldinboththepartsoftheringis</p><p></p><p>The induced electric field in both the parts of the ring is</p><p>{E}_{ind} = \dfrac{R}{2}\dfrac{dB}{dt} = \dfrac{Rb}{2}</p><p><imgalt=""src="https://cdn−question−pool.getmarks.app/ntaabhyas/jeemain/images/13373sol1.JPG"style="width:130px;height:163px;"/><br/><br/>Let</p><p><img alt="" src="https://cdn-question-pool.Quantrex.app/nta_abhyas/jee_main/images/13373_sol_1.JPG" style="width: 130px; height: 163px;" /><br /><br />LetEbethefieldwhichisdevelopedineachpartduetochargeaccumulationatthejunctions,thenfortheupperhalf</p><p>be the field which is developed in each part due to charge accumulation at the junctions, then for the upper half</p><p>\left({E}_{ind} + E\right)\piR = i\left(10r\right)</p><p>andforthelowerhalf</p><p>(Eind−E)\piR=ir</p><p>and for the lower half</p><p>\left({E}_{ind} - E\right)\piR = ir

⇒2E\piR−9ir=0⇒ 2E\piR - 9ir = 0

E=9ir2\piRE = \dfrac{9ir}{2\piR}

⇒E=9r2\piR×πR2b11r=922Rb⇒ E = \dfrac{9r}{2\piR} \times \dfrac{\pi{R}^{2}b}{11r} = \dfrac{9}{22}Rb

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