brain storming comprehensions (physics)
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8/10/2019 Brain Storming Comprehensions (Physics)
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Aakash Educational Services Ltd.-Regd. Office: Aakash Tower, Plot No.-4, Sector-11, Dwarka, New Delhi-75 Ph.011-47623456
Brain Storming
Comprehensions UNIT 4Linked Comprehension Type
C1. 1. Answer (3)
Fringe width = F =d
Dλ
d
v
dt
dF R
λ==⇒
And a = kt
kt dt
dv =⇒
2
2kt v =⇒
22
2t R
d
kt
dt
dF R α⇒
λ==⇒
2. Answer (1)
x component of velocity = velocity of screen =2
2kt
Also, y =d Dnλ
⇒ y component of velocity =dt
dy
=d
kt n
2
2λ
⎟ ⎠
⎞⎜⎝
⎛ λ+=⇒ j
d
ni
kt v ˆˆ
2
2
3. Answer (4)
Position vector of nth maxima relative to (n – 1)th maxima = j
d
D ˆλ
j d
kt j
dt
Dd
d a ˆˆ
2
2 λ=⋅
λ=⇒
C2. 1. Answer (1)
For minimum energy, j = 0 ⇒π
=2
hL . Use
I
Lk
2
2
=
2. Answer (1)
If KT < (KE)R, there will be no rotation.
3. Answer (2)For nitrogen, minimum KE of rotation is very low.
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330 Brain Storming Comprehensions Success Magnet-Solutions (Part-I)
Aakash Educational Services Ltd.-Regd. Office: Aakash Tower, Plot No.-4, Sector-11, Dwarka, New Delhi-75 Ph.011-47623456
C3. 1. Answer (1)
N
A B
4I I
N
For the disc A
NR Δt = 4Iω1
NR Δt = I (ω + ω2)
⇒ 4ω1 = ω + ω
2...(i)
21
12
uu
v v e
−
−=
ω=ω+ω⇒−ωω+ω
= 2121 2202
1
R
R R ...(ii)
4ω 1 – ω 2
= ω
2ω 1 + 2 ω2
= ω
1031 ω=ω⇒
52
ω=ω
If the next collision take place of n1 revolutions of the first disc and n
2 revolution of the second disc then
n1 ω2
= n2 ω1
2
3
2
1
n
n⇒
2. Answer (2)
So the time after which next collison will take place
= 32
1
×ωπ or 22
2×ωπ
= 3103
2××
ωπ
=ωπ
20
and T =ωπ
So = 20 T
3. Answer (2)
If I 1 = I
2 and e = 1 then
I ω 1 = I (ω + ω 2
)
10
21 =−ωω+ω
ω 1 – ω 2
= ω
ω1 + ω 2
= ω
⇒ ω1 = ω and ω2
= 0
So next collision will take place after
T 22 =ωπ
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331Success Magnet-Solutions (Part-I) Brain Storming Comprehensions
Aakash Educational Services Ltd.-Regd. Office: Aakash Tower, Plot No.-4, Sector-11, Dwarka, New Delhi-75 Ph.011-47623456
C4. 1. Answer (1)
(V – V ′)5 = V × 1 ⇒5
4=
′
V
V
2. Answer (2)
Acceleration = drag force / mass = 6πηr
m
V V ⎟ ⎠ ⎞⎜
⎝ ⎛ − 2
00
3. Answer (4)
Velocity increases exponentially from zero to V 0.
C5. 1 Answer (3)
For a horizontal axis through C , ∫ ⎟ ⎠
⎞⎜⎝
⎛ θ
===2
22 l mmR dmR I
2. Answer (1)
For the position of centre of mass, we have
θ
θ−=
θ
θθ
=
∫
∫
π
θ−π
π
θ−π
)cos1(
sin
2
2
2
20 R
d
d R
x
Also,θ
= l
R
3. Answer (3)
Mgd
I T π= 2
Here d = R – x 0, I = I cm + md 2 = (MR 2 – mx 02) + md 2
C6. The situation is shown in figure.
3 0 °
θr a
B′
C ′
A′
A
B C
v
v
v
O
3a1. Answer (3)
dt
dr v −=30cos ⇒ vt ar
2
3−=
2. Answer (1)
dt
d
r
v θ=
30sin⇒
⎟⎟ ⎠
⎞⎜⎜⎝
⎛
−=θ⇒
⎟⎟ ⎠
⎞⎜⎜⎝
⎛ −
=θt v a
a
vt a
vdt d
32
2ln
3
1
2
32
3. Answer (1)
All the sides of Δ ABC turn through same angle θ.
The particles converge, when r = 0
⇒v
at 3
2=
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332 Brain Storming Comprehensions Success Magnet-Solutions (Part-I)
Aakash Educational Services Ltd.-Regd. Office: Aakash Tower, Plot No.-4, Sector-11, Dwarka, New Delhi-75 Ph.011-47623456
C7. 1. Answer (3)
Relative to cart, velocity of small body will be at an angle 45° above horizontal.
Let V C be the speed of cart
V c
V 0
45°
Cart
By conservation of linear momentum along horizontal,
v mmv v v m c c ×=+−2
)( 0
22 0v
v v c −=
22
2 0v v v c
−=
2. Answer (2)
The vertical component of the small body is2
0v
So, height above the point of leaving is ( ) g v
g v
422
2
0
2
0 =
Above the cart surface, height =g
v R R
42
20+−
3. Answer (2)
Momentum along horizontal remains conserved,
So, mv = (m + m)V f
⇒ v f =
2
v
Loss = K i – K
f =
42)2(
2
1
2
1 222 mv v
mmv =⎟ ⎠
⎞⎜⎝
⎛ −
C8. 1. Answer (3)
The phase difference, if the wave travelled along x-axis is k Δ x . Now the phase difference will be )(·)( r k Δ
= ⎥⎦
⎤⎢⎣
⎡+
⎥⎥⎦
⎤
⎢⎢⎣
⎡++
λπ
k j i k j i ˆ2ˆ
2
1 –ˆ32·ˆ
2
1ˆ
2
1ˆ2
32
=λπ7
2. Answer (4)
For a point source, wave has spherical symmetry and the wave representation would be like
Displacement Y = Asin(ωt – kr )
So, Δφ = k Δr = ) –(2
12 r r λπ
= 002
=×λπ
∴ r 2 = r
1 =
222 132 ++
3. Answer (3)
]ˆcosˆcosˆcos[ j j i v
k γ+β+αω
=
v v
v v
v v z y x =γ=β=α cos,cos,cos
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333Success Magnet-Solutions (Part-I) Brain Storming Comprehensions
Aakash Educational Services Ltd.-Regd. Office: Aakash Tower, Plot No.-4, Sector-11, Dwarka, New Delhi-75 Ph.011-47623456
C9. 1. Answer (1)
For the object, not to hit the planet, its minimum distance ( i .e., when it is at perigee of its path) must
be slightly greater than the radius of planet.
2. Answer (3)
In the above case, semi-major axis of the orbit would be a =2
3R
Total mechanical energy =R
GMm
a
GMm
3 –
2 – =
So,R
GMm
R
GMmmv
3 –
)2( –
2
1 20 =
R
GM
v 30 =
3. Answer (1)
When v < v 0, object falls on planet, so it will not orbit. When v > v
escape object will not orbit.
R
GM
R R
GM
hR
GM v e =
+=
+=
22