brain storming comprehensions (physics)

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Page 1: Brain Storming Comprehensions (Physics)

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 

dt 

dF R 

  λ==⇒

 And   a = kt

kt dt 

dv =⇒

2

2kt v  =⇒

22

2t R 

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

⎟ ⎠

 ⎞⎜⎝ 

⎛    λ+=⇒   j 

ni 

kt v  ˆˆ

2

2

3. Answer (4)

Position vector of nth maxima relative to (n – 1)th maxima =  j 

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

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.

Page 2: Brain Storming Comprehensions (Physics)

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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  ...(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

Page 3: Brain Storming Comprehensions (Physics)

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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=

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 R 

 x 

 Also,θ

=  l 

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 

O

3a1. Answer (3)

dt 

dr v    −=30cos ⇒   vt ar 

2

3−=

2. Answer (1)

dt 

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

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

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

GMmmv 

3 –

)2( –

2

1 20   =

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.

GM 

R R 

GM 

hR 

GM v e   =

+=

+=

22