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New answer posted

6 months ago

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S
Syed Aquib Ur Rahman

Contributor-Level 10

An excellent example of pure rotational motion is the motion of the blades of a ceiling fan when it is switched on. In this type of motion, the object rotates about a fixed axis, and all particles of the object move in circles centred on that axis. Windmills and turbines also follow the same rotational mechanics. 

New answer posted

6 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

υ 0 = 3 2 0 H z . v t r a i n = 3 6 k m / h = 3 6 * 1 0 0 0 6 0 * 6 0 = 1 0 m / s

υ ( r e f l e c t e d S o u n d ) = υ 0 ( v v v t r a i n )

= 3 2 0 ( 3 3 0 3 3 0 1 0 ) = 3 3 0 H z

υ e c h o = υ r e f l e c t e d ( v + v t r a i n V )

= 3 3 0 ( 3 3 0 + 1 0 3 3 0 ) = 3 4 0 H z .

New answer posted

6 months ago

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V
Vishal Baghel

Contributor-Level 10

P 1 = 1 . 2 * 1 0 3 0 C . m P 2 = 2 . 4 * 1 0 3 0 C . m

E 1 = 5 * 1 0 4 N C 1 E 2 = 1 5 * 1 0 4 N C 1

So, τ 1 τ 2 = P 1 E 1 s i n 9 0 ° P 2 E 2 s i n 9 0 ° = ( 1 . 2 * 1 0 3 0 ) * ( 5 * 1 0 4 ) ( 2 . 4 * 1 0 3 0 ) * ( 1 5 * 1 0 4 )

= 1 2 * 1 3 = 1 6 x = 6

New answer posted

6 months ago

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V
Vishal Baghel

Contributor-Level 10

R A B = 2 0 Ω

L = 300 cm

Null point is at 60 cm from A, so

2 0 m V = 4 R + 2 0 * 2 0 * ( 6 0 3 0 0 ) * 1 0 3

2 0 = 1 6 R + 2 0 * 1 0 3

R = 1 5 6 0 0 2 0 = 7 8 0 Ω

New answer posted

6 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

  i = l 0 2  at ω 1  = 212 rad/s R = 5 Ω

  ω 2 = 232 rad/s Δ ω = ω 2 ω 1 = 2 0 r a d / s

P = P m a x 2 a t ω 1 a n d ω 2

So, Δ ω = ω 2 ω 1 = R L

L = R Δ ω = 5 2 0 = . 2 5 H

= 250 mH

New answer posted

6 months ago

0 Follower 3 Views

S
Syed Aquib Ur Rahman

Contributor-Level 10

The law of rotational motion follows Newton's second law. The net external torque acting on a rigid body is directly proportional to its angular acceleration. The constant of proportionality is the moment of inertia (I). That is a measure of an object's resistance to changes in its rotational motion. This relationship is mathematically expressed as  τ = I α  

Each component of the rotational law has a direct analogue in linear motion. Torque is analogous to force (F), moment of inertia (I) is analogous to mass (m), and angular acceleration is analogous to linear acceleration (a). 

All in all, you just need to remember that just as

...more

New answer posted

6 months ago

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S
Syed Aquib Ur Rahman

Contributor-Level 10

Rotational motion in Class 11 Physics is regarded as a challenging chapter, particularly due to the transition from point particles to extended bodies. Additionally, the concepts covered here are analogous to, yet distinct from, linear motion. Even vector calculations here can be difficult. But the key to mastering this chapter is to be conceptually clear with your previous chapters in Physics. You also need to be able to visualise rotational motion instead of memorising definitions, to be able to master it.  

New answer posted

6 months ago

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V
Vishal Baghel

Contributor-Level 10

λ 1 = 5 6 0 n m , fringe width, B = 7.2 mm

B 1 = D λ 1 d = 7 . 2 m m

For λ 2 B 2 = D λ 2 d = 8 . 1 m m

B 2 B 1 = λ 2 λ 1 = 8 . 1 7 . 2 λ 2 8 1 7 2 λ 1

= 9 8 * 5 6 0 n m

= 630 nm

New answer posted

6 months ago

0 Follower 4 Views

S
Syed Aquib Ur Rahman

Contributor-Level 10

Yes, rotational motion is important for the NEET exam. Expect and prepare for, at least, two to three questions on rotational motion as per the latest NEET Physics syllabus for Mechanics. Questions from this chapter are clubbed into the application of principles from other areas of mechanics, such as Laws of Motion, Work, Energy, and Power, and Conservation of Momentum

New answer posted

6 months ago

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V
Vishal Baghel

Contributor-Level 10

t1/2 = 2hr 30 min

Radiation intensity a disintegrations / sec (Activity)

As,   A = A 0 2 t t 2

For safe working, A = A 0 6 4 A 0 6 4 = A 0 2 t t 1 2  

t = 6 t 1 2 = 6 * 2 . 5 h r                            

= 15

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