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11. (a, d) : As, F 1 = k 1 x, F 2 = k 2 x.<br />

1 2<br />

1 2<br />

Work done W1 = k1x<br />

and W2 = k2x<br />

2<br />

2<br />

W1<br />

k1<br />

or α= =<br />

W2<br />

k2<br />

When the springs are stretched by the same force<br />

F, the extensions in springs A and B are x 1 and x 2<br />

respectively which are given by<br />

F = k 1 x 1 = k 2 x 2 or x 1<br />

k2<br />

= …(i)<br />

x2<br />

k1<br />

1 2<br />

1 2<br />

Work done W1′=<br />

k1x1<br />

and W2′ = k2x2<br />

2<br />

2<br />

2<br />

W1′<br />

<br />

W ′ = k1<br />

k<br />

⋅ x1<br />

…(ii)<br />

2<br />

2 2 x2<br />

Using (i) and (ii) we get<br />

2<br />

W1′<br />

β=<br />

W ′ = k1<br />

k<br />

⋅ k2<br />

k<br />

= k2<br />

2<br />

2 2<br />

k<br />

1 1<br />

800 − 80<br />

12. (a, b, c, d) : Rate of heat flow H =<br />

⎛ li<br />

⎞ lo<br />

⎝<br />

⎜ KA⎟ i ⎠<br />

+ ⎛ ⎞<br />

⎜ ⎝ KoA⎠<br />

⎟<br />

which is also equal to 800 − T<br />

. Using these two<br />

⎛ li<br />

⎞<br />

⎝<br />

⎜ KA⎠<br />

⎟<br />

i<br />

720<br />

relations we get, T = 800 −<br />

Ki<br />

lo<br />

+ ⎛ . Thus<br />

⎞ ⎛ ⎞<br />

1<br />

⎜ ⎝ Ko<br />

⎠<br />

⎟ ⎜<br />

⎝ li<br />

⎠<br />

⎟<br />

one can reduce the temperature at the interface by<br />

any of the four options given.<br />

13. (a, b, c, d) : Intensity, by definition, is the energy<br />

flowing per unit area per unit time.<br />

The intensity is related to the displacement<br />

amplitude A of the sound wave by<br />

2 2<br />

I = 1 ρω v A<br />

2<br />

The displacement amplitude is given by A = P ,<br />

Bk<br />

⎛ ω⎞<br />

where k =<br />

⎝<br />

⎜<br />

v ⎠<br />

⎟ is the propagation constant.<br />

B<br />

The speed is given by v = . ρ<br />

14. (2) :<br />

Use these relations to get the required expressions.<br />

A<br />

d/2 x<br />

B 2D<br />

Optic axis<br />

O x d/4<br />

1<br />

C<br />

3f<br />

From similar triangles AOB and BDC<br />

OB AO<br />

= or x 1 d 2<br />

= ( / )<br />

BD CD x (<br />

2<br />

d / 4)<br />

or x 1 = 2x 2<br />

As x 1 + x 2 = 3f, 2x 2 + x 2 = 3f or x 2 = f<br />

i.e. x 1 = 2f<br />

n = 2.<br />

15. (7)<br />

16. (4) : Let the velocities of car 1 and car 2 be<br />

v 1 m s –1 and v 2 m s –1 .<br />

∴ Apparent frequencies of sound emitted by car 1<br />

and car 2 as detected at end point are<br />

υ0v<br />

υ0v<br />

υ1<br />

= and υ −<br />

2<br />

=<br />

v v1<br />

v − v2<br />

300 × 330<br />

−1<br />

∴ 330 =<br />

or v1<br />

= 30 ms<br />

330 − v1<br />

300 × 330<br />

−1<br />

and 360 =<br />

or v2<br />

= 55 ms<br />

330 − v<br />

A<br />

2<br />

vt 1<br />

vt 2<br />

1 2<br />

B<br />

100 m<br />

The distance between both the cars just when the<br />

2 n d car reaches point B(as shown in figure) is<br />

100 m = v 2 t – v 1 t<br />

100 100<br />

t = = = 4 s<br />

v − v 55 − 30<br />

2 1<br />

17. (5) : The capacitance of a parallel plate capacitor in<br />

air is given by<br />

A<br />

C = ε 0<br />

...(i)<br />

d<br />

By introducing a slab of thickness t, the new<br />

capacitance C′ be<strong>com</strong>es<br />

ε<br />

C′ = 0<br />

A<br />

⎛ 1 ⎞<br />

...(ii)<br />

d′ −t⎜1<br />

−<br />

⎝ ⎠<br />

⎟<br />

K<br />

The charge (Q = CV) remains the same in both the<br />

cases.<br />

Hence<br />

ε0A<br />

ε0A<br />

=<br />

d ⎛ 1 ⎞<br />

d′ −t⎜1<br />

−<br />

⎝ K ⎠<br />

⎟<br />

⎛ 1 ⎞<br />

or d= d′ −t<br />

−<br />

⎝<br />

⎜1<br />

K ⎠ ⎟<br />

80 CHEMISTRY TODAY | APRIL ‘17

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