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Motion in a Plane

Motion in a PlaneNEET Physics · Class 11 · NCERT Chapter 3

21 NEET previous-year questions on Motion in a Plane, each with the correct answer and a step-by-step solution. Sourced directly from official NEET papers across every booklet code.

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All (21)
Motion in a Plane (21)

A

3.5

B

5.9

C

16.3

D

110.8

Solution

The range of a projectile is given by . For identical trajectories, the ranges are equal, so . Therefore, option (a) is correct.

A

t= π 4ω

B

t= π 2ω

C

t= π ω

D

t=0

Solution

A⃗⃗ =coswt î+sinwt ĵ B⃗⃗ =coswt 2 î+sinwt 2 ĵ for A⃗⃗ .B⃗⃗ =0 A⃗⃗ .B⃗⃗ =0=cos wt.coswt 2 +sinwt.sinwt 2 =cos(wt−wt 2)=cos( wt 2) So wt 2 = π 2 ⇒ t= π w

A

Acceleration vector is along −R⃗⃗ .

B

Magnitude of acceleration vector is v2 R , where v is the velocity of particle.

C

Magnitude of the velocity of particle is 8 meter/second

D

Patch of the particle is a circle of radius 4 meter.

Solution

www.vedantu.com 33 x= 45 m 2πt, y=4c os(2πt) Squiring and adding ⇒ Circular motion V=ω= (2π)(4)=8π

A

r⃗ 1−r⃗ 2 |r⃗ 1−r⃗ 2|= v⃗⃗ 2−v⃗⃗ 1 |v⃗⃗ 2−v⃗⃗ 1|

B

r 1∙v⃗ 1=r 2∙v⃗ 2

C

r 1×v⃗ 1=r 2×v⃗ 2

D

r 1−r 2=v⃗ 1−v⃗ 2

Solution

For two particles to collide, the direction of the relative velocity of one with respect to other should be directed towards the relative position of the other particle i.e. r⃗ 1−r⃗ 2 |r⃗ 1−r⃗ 2| → direction of relative position of 1 w.r.t..2. & v⃗⃗ 2−v⃗⃗ 1 |v⃗⃗ 2|−v⃗⃗ 1 → direction of velocity of 2 w.r.t.1 www.vedantu.com 32 So for collision of A & B r 1−r 2 |r 1−r 2|= v⃗ 2−v⃗ 1 |v⃗ 2−v⃗ 1|

A

0.1 m/s2

B

0.15 m/s2

C

0.18 m/ s2

D

0.2m s2

Solution

Tangential acceleration at = rα = constant = K α = K r At the end of second revoluation angular velocity is w then w2 − w0 2 = 2 ∝ θ w2 − O2 = 2(K r)(4π) w2 = 8πK r K.E. of the particle is = K.E.= 1 2mv2 K.E.= 1 2mr2w2 K.E.= 1 2 m(r2)(8πK r ) 8 ×10−4 = 1 2 × 10× 10−3 × 6.4 ×10−2 × 3.14× K 𝐾 = 2 6.4 × 3.14= 0.1 𝑚 𝑠𝑠𝑒𝑐2

A

Velocity and acceleration both are perpendicular to r .

B

Velocity and acceleration both are parallel to r .

C

Velocity is perpendicular to r and acceleration is directed towards the origin.

D

Velocity is perpendicular to r and acceleration is directed away from the origin.

Solution

Position vector is r = cosω + x ̂ +sinω + y ̂ Velocity of particle is v⃗ = dr⃗ dt v⃗ = sinωt.ωx ̂ + cosωt.ωy ̂ v⃗ = ω(−sinωtx ̂ + cosωty ̂) Acceleration of the particle is a⃗ = dv⃗ dt a⃗ = −ω2(cosωtx ̂ +sinωty ̂) a⃗ = −ω2r , So direction of r and a⃗ are opposite. v⃗ .a⃗ = 0 ⇒ v⃗ ⊥ a⃗ v⃗ .r = 0 ⇒ v⃗ ⊥ r So, ans is (Velocity is perpendicular to r and acceleration is directed towards the origin.)

A

0𝑜

B

90𝑜

C

45𝑜

D

180𝑜

Solution

www.vedantu.com 24 |A⃗⃗ + B⃗⃗ | = |A⃗⃗ − B⃗⃗ | A2 + B2 + 2ABcosθ = A2 + B2 = 2ABcosθ 4ABcosθ = 0 cosθ = 0 θ =90o

A

√gR2 μs+tanθ 1−μs tanθ

B

√gR μs+tanθ 1−μs tanθ

C

√ g R μs+tanθ 1−μstanθ

D

√ g R2 μs+tanθ 1−μstanθ

Solution

www.vedantu.com 28 N =mgcosθ +mv2 r sinθ fmax = μmgcosθ +μmv2 r sinθ mgsinθ + μmgcosθ +μmv2 r sinθ =mv2 r cosθ gsinθ + gcosθ =V2 r (cosθ − μsinθ) gr[ tanθ + μ 1 + μtanθ] = V2 www.vedantu.com 29 CHEMISTRY

A

T

B

2mvT l+

C

2mvT l-

D

Zero

Solution

Centripetal force 2mv l ⎛⎞ ⎜⎟⎜⎟⎝⎠ is provided by tension so the net force will be equal to tension i.e., T.

A

inclined at an angle of 60° from vertical

B

the mass is at the highest point

C

the wire is horizontal

D

the mass is at the lowest point

Solution

Tension is maximum at bottom ⇒ Mass is at the lowest point

A

1 : 4

B

2 : 1

C

1: 2

D

4 : 1

Solution

𝑅= 𝑚𝑣 𝑞𝐵 𝑅𝐻 𝑅∝ = 𝑚𝑣 𝑒𝐵 ×2𝑒𝐵 𝑚𝑣=2∶1

A

electric heater

B

induction furnace

C

magnetic braking in train

D

electromagnet

Solution

Conceptual.

A

3 : 1

B

2 : 1

C

1 : 2

D

2 : 3

Solution

1 𝐹1 = 1 𝑓+ 1 𝑓= 2 𝑓 𝐹1=𝑓/2 1 𝐹2 = 1 𝑓− 1 𝑓+1 𝑓= 1 𝑓 𝐹2=𝑓 𝐹1∶ 𝐹2=1 ∶2

A

45° west

B

30° west

C

D

60° west

Solution

2 1 20 10 mv Rvcos −= − =−= θ θ =120° ∴ angle with north = 30° west

A

1 2 2 1 2 gT cos R         − θ= π

B

1 2 2 1 2 R cos gT         − π θ=

C

1 2 2 1 2 R sin gT         − π θ=

D

1 2 2 1 2 2gT sin R         − θ= π

Solution

The maximum height for a projectile is given by . For a particle moving in a circle with radius and period , the speed . Given , substituting gives . Taking the inverse sine, . Simplifying, . However, the correct form is , which matches option (b).

A

B

C

12π

D

104π

Solution

Angular acceleration ω −ωα= fi t 23120 rad/s60 πω= ×f 21200 rad/s60 πω= ×i ⇒ (3120 1200) 2 416 60 −πα= × = π

A

Zero

B

15 3 ms −

C

5 ms–1

D

10 ms–1

Solution

At highest point vertical component of velocity become zero. At highest point speed of object = 10cos30° 5 3 m/s= - 16 - NEET (UG)-2022 (Code-Q1)

A

along the axis of rotation

B

along the radius, away from centre

C

along the radius towards the centre

D

along the tangent to its position

Solution

Angular acceleration is a vector quantity directed along the axis of rotation, perpendicular to the plane of motion. This aligns with the definition in NCERT XI chapter Motion in a Plane, so option (a) is correct.

A

3000 m

B

2800 m

C

2000 m

D

1000 m

Solution

The maximum height is given by . Substituting, , so option (d) is correct.

A

Constant velocity

B

Constant acceleration

C

Constant velocity but varying acceleration

D

Varying velocity and varying acceleration

Solution

A particle moving with uniform speed in a circular path maintains varying velocity and varying acceleration. It is because direction of both velocity as well as acceleration will change continuously.

A

T

B

4T

C

4 T

D

2T

Solution

2=ω Tm 2(2 )′ = ω Tm 4′=TT SECTION-B

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