24.06.2022 Views

33 Years NEET-AIPMT Chapterwise Solutions - Physics 2020

All previous year questions , and these are downloaded from the sources in the internet. I don't own these resources and these are copyrighted by MTG.

All previous year questions , and these are downloaded from the sources in the internet. I don't own these resources and these are copyrighted by MTG.

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Motion in a Plane

Telegram @unacademyplusdiscounts

23

2 2 2

u sin2θ u sin θ 2 2 2

∴ = or,

2u

sinθcosθ u sin θ

=

g 2g

g 2g

tanq = 4 or q = tan –1 (4)

28. (a) : Here, u = 20 m/s, g = 10 m/s 2

For maximum range, angle of projection is

q = 45°

u

2 sin90° u

2 ⎛

∴ R = = ⎜ R u 2 sin2θ

max

Q = ⎟

g g ⎝ g ⎠

2

( 20 m/s)

= = 40 m

2

( 10 m/s )

29. (c) : Let f be elevation

angle of the projectile at its

highest point as seen from

the point of projection O and

q be angle of projection with

the horizontal.

From figure,tanφ= H

...(i)

R / 2

In case of projectile motion

sin

Maximumheight, H u 2 2

θ

=

2g

sin

Horizontal range, R u 2

=

g

Substituting these values of H and R in (i), we get

2 2

u sin θ

2 2

2g

sin θ sin θ 1

tanφ

= = = = tanθ

2

u sin2θ

sin2θ

2sinθcosθ

2

2 g

Here, q = 45°

∴ tanφ = 1 1

tan 45°= ( Q tan 45°=

1)

2 2

− ⎛

φ= tan 1 1

⎞ 2 ⎠ ⎟

30. (a) : Let v be velocity of a projectile at maximum

height H.

v = ucosq

According to

given problem,

u

v = 2

u

1

∴ = u cosθ ⇒ cosθ= ⇒ θ = 60°

2

2

31. (a) :

The horizontal momentum does not change. The change

in vertical momentum is

1

mv sin θ−( − mv sin θ)

= 2mv = 2mv

2

32. (b) : Horizontal range, R u 2

sin2θ

=

g

For angle of projection (45° – q), the horizontal range is

2 2

2

u sin[ 245 ( °−θ)] u sin( 90°−2θ ) u cos2θ

∴ R1

=

=

=

g

g

g

For angle of projection (45° + q), the horizontal range is

2 2 2

u sin[ 245 ( °+ θ)] u sin( 90°+

2θ) u cos2θ

R2

=

=

=

g

g

g

2

R1

u cos 2θ

/ g 1

∴ = = .

R 2

2 u cos 2θ

/ g 1

33. (c) : Time required to reach the ground is dependent

on the vertical motion of the particle. Vertical motion of

both the particles A and B are exactly same. Although

particle B has an initial velocity, but that is in horizontal

direction and it has no component in vertical (component

of a vector at a direction of 90° = 0) direction. Hence they

will reach the ground simultaneously.

34. (b) : As q 2 = (90 – q 1 ),

So range of projectile,

v0 2 sin2θ v0 2 2sinθcosθ

R1

= =

g

g

v0 2 2sin( 90−θ1)cos( 90 −θ1)

R2

=

g

v0 2 2cosθ1sinθ1

R2

= = R1

g

35. (b) : For the given velocity of projection u, the

horizontal range is the same for the angle of projection

q and 90° – q.

Horizontal range, R u 2

sin2θ

=

g

2

u sin( 2× 30° ) 2

u sin60°

∴ Forbody A,

RA

=

=

g

g

2

u sin( 2× 60°

)

Forbody BR , B =

g

u

2 u

u

RB = sin120° 2 sin( 180°− 60° ) 2 sin60°

= =

g

g

g

The range is the same whether the angle is q or 90° – q.

\ The ratio of ranges is 1 : 1.

36. (c) : Horizontal range, R u 2

sin2θ

=

g

For maximum horizontal range, q = 45°

2

u

Rm = g

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!