Let V 0 and T 0 are the volume of the gas and
temperature initially in each part. After displacing
the adiabatic separator the new volumes are V 1
and V 2 and temperatures are T 1 and T 2
Given that
1
2
7
3
V
V
V V V 1 2 20
0 0
1 2
14 6
&
10 10
V V
V V
1
1 0
0 0 1
14
10
V
T V T
(i)
1
(^10)
0 0 2
6
10
V
T V T
(ii)
From (i) & (ii) we get
1
2
3
7
T
T
Number of fissions per second
Power output
Energy released per fission
6
17
6 19
3.2 10
1 10
200 10 1.6 10
Number of fission per minute
60 1 10^17 6 10^18
5
6
0.5
5 10
10
V V
E m
d
The value of Rs should be such that the current
through the zener diode is much larger than the
load current as five times the load current i.e.,
Iz20 mA. The total current through Rs is
therefore, 24 mA. The voltage drop across Rs is
10 6 4 V. This gives
s 3
4 V
R 167
24 10 A
Note Slight variation in the value of the resistor
does not matter, what is important is that the current
Iz should be sufficiently larger than IL.
(^) rad (1 )
I
P
c
where
coefficient of reflection
(1 )
I
F A
C
6
8
200
(1 0.6) 1.07 10
3 10
F A N
A
0.6 100 60%
Wavelength increases in the sequence
VIBGYOR. Refractve index decreases as
wavelength increases. Therefore, decreases in
the sequence VIBGYOR.
As
C sin^11 ,
therefore, critical angle C
increases in the sequence VIBGYOR. For green
colour, i C.
For yellow, orange and red, critical angle is greater.
Therefore, i is less than critical angle for YOR.
These colours will not suffer total internal
reflection. They will emerge from glass-air interface.
No light is emitted from the second polaroid,
so P and P 1 2 are perpendicular to each other
Let the initial intensity of light is I 0. So Intensity
of light after transmission from first polaroid is^0
2
I
.
Intensity of light emitted from P 3 is 1 0 2
2
I
I cos
Intensity of light transmitted from last polaroid i.e.,
from 2 1 2 (^90) ^022
2
I
P I cos cos .sin
0 2 0 2
2 2
8 8
I I
sin cos sin
As, asin n
19.Sol:
20.Sol:
21.Sol:
22.Sol:
23.Sol:
24.Sol:
25.Sol:
26.Sol: ay 3
D
or
0.3 10^3 5 10^3
( )
3 3 1
ay
D F
D
5 10 m 5000 A^7