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A rigid body is rotating with an angular velocity ω = a - bt, where a and b are constants and t is the time. Then the total angle subtended by the body before coming to rest is:
1. \(\frac{(a-b)a}{2}\)
2. \(\frac{a^2}{2b}\)
3. \(\frac{a^2 -b^2}{2b}\)
4. \(\frac{a^2 -b^2}{2a}\)

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Correct Answer - Option 2 : \(\frac{a^2}{2b}\)

The correct answer is option 2) i.e. \(\frac{a^2}{2b}\)

CONCEPT:

  • Angular velocity is the rate of change of angular displacement with time for motion on a curved path.
    • While moving on a curved path, displacement is the change in angle about the point of rotation or curved motion.

Angular velocity, \(ω =\frac{angle}{time} =\frac{dθ}{dt}\)

CALCULATION:
Given that:
Angular velocity, ω = a - bt
When the body comes to rest, ω = 0
⇒ a - bt = 0
⇒ t = a/b      
Therefore, the body comes to rest at t = a/b
We know, \(ω =\frac{dθ}{dt}\)
\(⇒ a-bt =\frac{dθ}{dt}\)
\(⇒ (a-bt)dt=dθ\)
Total angle subtended, θ = ∫dθ 
\(⇒∫dθ = \int_{0}^{a/b} (a-bt)dt\)
\(⇒∫dθ = [at - \frac{bt^2}{2}]_0 ^{a/b}\)
\(⇒∫dθ = a(\frac{a}{b}) - \frac{b(\frac{a}{b})^2}{2}\)
\(⇒∫dθ = \frac{a^2}{2b}\)
\(∴ θ =\frac{a^2}{2b}\)

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