More practice questions

  1. Q4. Assertion: Ampere’s circuital law cannot be used to find the field at the centre of a circular current loop. Reason: the law is true only for loops of high symmetry. Are both true, and does the reason explain the assertion?

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    The assertion is true but the reason is false. The law holds for every closed loop; at the centre of a circular loop there is simply no amperian loop on which B is tangential and constant, so the law does not give B there easily (NCERT page 120).

  2. Q5. Two long parallel wires 10 cm apart carry 4.0 A and 6.0 A in the same direction. Find the field midway between them.

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    Each gives B = μI/(2πr) at r = 0.050 m: 1.6 × 10−5 T and 2.4 × 10−5 T. With currents in the same direction the two fields at the midpoint point opposite ways, so the net field is 8.0 × 10−6 T, in the direction of the field of the 6.0 A wire (NCERT Eq. (4.14) and the right-hand rule, page 119).

  3. Q6. A long hollow metal pipe carries a current along its length, spread evenly round its wall. What is the field inside the pipe, and outside it?

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    In the hollow cavity (not in the conducting wall), with no other sources present, an amperian circle encloses no current and cylindrical symmetry makes B tangential and constant, so B = 0. Outside, at distance r from the axis, the whole current is enclosed and B = μI/(2πr), as for a thin wire (reasoned from NCERT Eq. [4.13(b)], page 118).

  4. Q7. In a thick wire of radius a carrying a uniform current, at what distance from the axis inside the wire is the field half its value at the surface?

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    Inside, B ∝ r, so B = B(a)/2 at r = a/2. Outside it falls as 1/r and is half the surface value again at r = 2a (NCERT Example 4.7, page 120).

  5. Q8. In a long wire of radius a, the current density rises in proportion to the distance from the axis, J = kr, and the total current is I. Find B inside the wire.

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    A thin ring of radius x and width dx carries kx × 2πx dx. Adding the rings from 0 to r gives 2πkr3/3, so the enclosed current grows as r3: Ie = Ir3/a3. Then B × 2πr = μ0Ir3/a3, so B = μ0Ir2/(2πa3). It rises as r2 and meets μ0I/(2πa) at the surface (beyond NCERT; reasoned from NCERT Eq. [4.13(b)], page 118).