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Concepts Of Physics MCQ Edition [Volume 1]
Exam
Concepts Of Physics MCQ Edition [Volume 1]
Subject
Physics
Chapter
Work and Energy

Concepts Of Physics MCQ Edition [Volume 1] · Physics · Work and Energy

Suspended by a 1.5 m long string, a heavy particle is given an...

Suspended by a 1.5 m1.5 \text{ m} long string, a heavy particle is given an initial horizontal velocity of 57 m/s\sqrt{57} \text{ m/s}. Determine the maximum height reached by the particle above the point of suspension. Take g=10 m/s2g = 10 \text{ m/s}^2.

Options

  1. A1.5 m1.5 \text{ m}
  2. B1.8 m1.8 \text{ m}
  3. C0.9 m0.9 \text{ m}
  4. D1.2 m1.2 \text{ m}

Correct answer

D. 1.2 m1.2 \text{ m}

Step-by-step solution

Given:
Initial velocity, u=57 m/su = \sqrt{57} \text{ m/s}
Length of the string, l=1.5 ml = 1.5 \text{ m}
Acceleration due to gravity, g=10 m/s2g = 10 \text{ m/s}^2

The minimum velocity required to complete the vertical circle is 5gl=5×10×1.5=75 m/s\sqrt{5gl} = \sqrt{5 \times 10 \times 1.5} = \sqrt{75} \text{ m/s}.
The minimum velocity required to reach the horizontal position is 2gl=2×10×1.5=30 m/s\sqrt{2gl} = \sqrt{2 \times 10 \times 1.5} = \sqrt{30} \text{ m/s}.

Since 30<57<75\sqrt{30} < \sqrt{57} < \sqrt{75}, the particle will cross the horizontal position but the string will become slack before reaching the highest point.

Let the string become slack at an angle θ\theta with the upward vertical. At this point, the tension in the string is zero (T=0T = 0).
The component of gravity provides the necessary centripetal force:
mgcos⁡θ=mv2l⇒v2=glcos⁡θmg \cos\theta = \dfrac{mv^2}{l} \Rightarrow v^2 = gl \cos\theta

Using conservation of mechanical energy from the lowest point to the point where the string becomes slack:
12mu2=12mv2+mgh\dfrac{1}{2}mu^2 = \dfrac{1}{2}mv^2 + mgh
Here, the height from the lowest point is h=l(1+cos⁡θ)h = l(1 + \cos\theta).
u2=v2+2gl(1+cos⁡θ)u^2 = v^2 + 2gl(1 + \cos\theta)

Substituting v2=glcos⁡θv^2 = gl \cos\theta and the given values:
57=15cos⁡θ+2(15)(1+cos⁡θ)57 = 15 \cos\theta + 2(15)(1 + \cos\theta)
57=15cos⁡θ+30+30cos⁡θ57 = 15 \cos\theta + 30 + 30 \cos\theta
27=45cos⁡θ⇒cos⁡θ=2745=3527 = 45 \cos\theta \Rightarrow \cos\theta = \dfrac{27}{45} = \dfrac{3}{5}

The velocity at this point is:
v=15×35=9=3 m/sv = \sqrt{15 \times \dfrac{3}{5}} = \sqrt{9} = 3 \text{ m/s}

The height of this point above the point of suspension is:
y=lcos⁡θ=1.5×35=0.9 my = l \cos\theta = 1.5 \times \dfrac{3}{5} = 0.9 \text{ m}

After the string becomes slack, the particle undergoes projectile motion. The velocity vector makes an angle θ\theta with the horizontal. The vertical component of velocity is:
vy=vsin⁡θv_y = v \sin\theta
Since cos⁡θ=35\cos\theta = \dfrac{3}{5}, we have sin⁡θ=45\sin\theta = \dfrac{4}{5}.
vy=3×45=2.4 m/sv_y = 3 \times \dfrac{4}{5} = 2.4 \text{ m/s}

The further maximum height reached during the projectile motion is:
H′=vy22g=(2.4)22×10=5.7620=0.288 mH' = \dfrac{v_y^2}{2g} = \dfrac{(2.4)^2}{2 \times 10} = \dfrac{5.76}{20} = 0.288 \text{ m}

The total maximum height reached by the particle above the point of suspension is:
H_{\text\max} = y + H' = 0.9 + 0.288 = 1.188 \text{ m}

Rounding to one decimal place, we get H_{\text\max} \approx 1.2 \text{ m}.

Answer: 1.2 m1.2 \text{ m}
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