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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