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1. Xtra Edge February 2012 - Career Point

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2. A plane spiral coil is made on a thin insulated wire and<br />

has N = 100 turns. Radii of inside and outside turns are<br />

a = 10 cm and b = 20 cm respectively. A magnetic field<br />

normal to the plane of spiral exists in the space. The<br />

magnetic field increases at a constant rate α = 0.3<br />

tesla/second. Calculate potential difference between the<br />

ends of the spiral.<br />

Sol. Since, magnetic field is increasing, therefore flux<br />

linked with the coil is also increasing. Due to<br />

increase in flux an emf is induced in it. Potential<br />

difference between ends of the spiral coil is equal to<br />

magnitude of emf induced in it.<br />

Since there are N turns in a radial width (b – a),<br />

therefore number of turns in the spiral coil per unit<br />

radial width is<br />

N<br />

n =<br />

( b – a)<br />

Consider a concentric circular ring of radius x and<br />

radial thickness dx<br />

Number of turns in this ring = n dx.<br />

Let at some instant magnetic field strength be B,<br />

Flux linked with the ring, φ = πx 2 B<br />

dφ<br />

Emf induced in this ring = (n . dx)<br />

dt<br />

⎛ dB ⎞<br />

= (n . dx) ⎜πx<br />

⎟<br />

⎝ dt ⎠<br />

2<br />

∴ Total emf induced in the spiral coil,<br />

x=<br />

b<br />

2<br />

e = ∫ ( πnαx<br />

dx)<br />

=<br />

3<br />

x=<br />

a<br />

1 πn α (b 3 – a 3 )<br />

= πnα x 2 dx<br />

Substituting value of n,<br />

1 2 2<br />

e = πN α(a + b + ab) = 2.2 volt Ans.<br />

3<br />

3. A spherical shell of radius R is filled with water.<br />

Temperature of atmosphere is (– θ) ºC. The shell is<br />

exposed to atmosphere and all water comes down to<br />

0ºC and then it starts freezing from outer surface<br />

towards the centre of the shell. Assuming shell to be<br />

highly conducting, calculate time for whole mass of<br />

water to freeze. Thermal conductivity of ice is K and<br />

latent heat of its fusion is L. Density of water is ρ.<br />

Neglect expansion during freezing.<br />

Sol. Heat flows from water to atmosphere because<br />

atmospheric temperature is below 0ºC. Water is<br />

filled in spherical shell, therefore heat flows in radial<br />

direction.<br />

Let at some instant t, thickness of ice layer be x.<br />

Then a concentric sphere of radius (R – x) is in<br />

liquid form as shown in figure. Heat flows from this<br />

sphere to atmosphere through ice layer.<br />

To calculate rate of heat flow, first we have to<br />

calculate thermal resistance of this ice layer.<br />

Considering a concentric spherical shell of radius r<br />

[(R – x) < r < R] and radial thickness dr as shown in<br />

figure.<br />

<strong>Xtra</strong><strong>Edge</strong> for IIT-JEE 18 FEBRUARY <strong>2012</strong><br />

r<br />

(R–x)<br />

dr<br />

Its thermal resistance =<br />

2<br />

4πr<br />

K<br />

∴ Total thermal resistance of ice layer<br />

R<br />

dr<br />

∫ 4πKr<br />

( R – x)<br />

2<br />

=<br />

R<br />

x<br />

4πKR(<br />

R – x)<br />

Temperature just inside and outside the ice layer is<br />

0ºC and (– θ)ºC, respectively.<br />

∴ Temperature difference = 0 – (– q) = θº C<br />

θ<br />

Hence, rate of heat flow, H =<br />

⎛ x ⎞<br />

⎜<br />

⎟<br />

⎝ 4πKR(<br />

R – x)<br />

⎠<br />

4πKRθ( R – x)<br />

=<br />

x<br />

H<br />

rate of freezing of mass =<br />

L<br />

H<br />

∴ Rate of freezing of volume =<br />

Lρ<br />

But it is equal to 4π(R – x) 2 dx<br />

.<br />

dt<br />

∴<br />

4πKRθ(<br />

R – x)<br />

Lρx<br />

= 4p (R – x) 2 dx<br />

.<br />

dt<br />

Lρx(<br />

R – x)<br />

or<br />

. dx = dt<br />

KRθ<br />

At instant t = 0, thickness of ice layer was equal to<br />

x = 0 and we have to calculate time t when whole<br />

mass has frozen or when x = R<br />

Substituting these limits,<br />

or t =<br />

t<br />

Lρ<br />

KRθ<br />

∫dt = ∫<br />

0<br />

ρ<br />

6Kθ<br />

LR 2<br />

R<br />

0<br />

x(<br />

R – x)<br />

dx<br />

Ans.

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