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Concepts Of Physics MCQ Edition [Volume 1]
Exam
Concepts Of Physics MCQ Edition [Volume 1]
Subject
Physics
Chapter
Newton's Laws of Motion

Concepts Of Physics MCQ Edition [Volume 1] · Physics · Newton's Laws of Motion

In the arrangement depicted in the figure, let m_1 = 1 kg , m_2 = 2...

In the arrangement depicted in the figure, let m1=1 kgm_1 = 1 \text{ kg}, m2=2 kgm_2 = 2 \text{ kg} and m3=3 kgm_3 = 3 \text{ kg}. Determine the accelerations of the masses m1m_1, m2m_2, and m3m_3. When the system is released from rest, the string segment from the upper pulley to m1m_1 measures 20 cm20 \text{ cm}. How much time will elapse before m1m_1 strikes the upper pulley?
In the arrangement depicted in the figure, let m_1 = 1 kg , m_2 = 2 kg and m_3 = 3 kg . Determine the accelerations of

Options

  1. A19g29\dfrac{19g}{29} (up), 21g29\dfrac{21g}{29} (down), 17g29\dfrac{17g}{29} (down), 0.25 s0.25 \text{ s}
  2. B21g29\dfrac{21g}{29} (up), 17g29\dfrac{17g}{29} (down), 19g29\dfrac{19g}{29} (down), 0.18 s0.18 \text{ s}
  3. C17g29\dfrac{17g}{29} (up), 19g29\dfrac{19g}{29} (down), 21g29\dfrac{21g}{29} (down), 0.35 s0.35 \text{ s}
  4. D19g29\dfrac{19g}{29} (up), 17g29\dfrac{17g}{29} (down), 21g29\dfrac{21g}{29} (down), 0.25 s0.25 \text{ s}

Correct answer

D. 19g29\dfrac{19g}{29} (up), 17g29\dfrac{17g}{29} (down), 21g29\dfrac{21g}{29} (down), 0.25 s0.25 \text{ s}

Step-by-step solution

Let T1T_1 be the tension in the string connected to m1m_1 and T2T_2 be the tension in the string connecting m2m_2 and m3m_3. Since the lower pulley is massless, T1=2T2T_1 = 2T_2.

Let a1a_1 be the upward acceleration of m1m_1. The lower pulley will have a downward acceleration of a1a_1.
Let a′a' be the downward acceleration of m3m_3 relative to the lower pulley. Then m2m_2 has an upward acceleration a′a' relative to the lower pulley.
The absolute downward accelerations of m2m_2 and m3m_3 are a2=a1−a′a_2 = a_1 - a' and a3=a1+a′a_3 = a_1 + a'.

Writing the equations of motion for each mass:
For m1m_1: T1−m1g=m1a1T_1 - m_1 g = m_1 a_1
⇒2T2−g=a1⇒T2=a1+g2\Rightarrow 2T_2 - g = a_1 \Rightarrow T_2 = \dfrac{a_1 + g}{2}

For m2m_2: m2g−T2=m2a2m_2 g - T_2 = m_2 a_2
⇒2g−T2=2(a1−a′)⇒g−T22=a1−a′\Rightarrow 2g - T_2 = 2(a_1 - a') \Rightarrow g - \dfrac{T_2}{2} = a_1 - a'

For m3m_3: m3g−T2=m3a3m_3 g - T_2 = m_3 a_3
⇒3g−T2=3(a1+a′)⇒g−T23=a1+a′\Rightarrow 3g - T_2 = 3(a_1 + a') \Rightarrow g - \dfrac{T_2}{3} = a_1 + a'

Adding the equations for m2m_2 and m3m_3 to eliminate a′a':
2g−T2(12+13)=2a12g - T_2\left(\dfrac{1}{2} + \dfrac{1}{3}\right) = 2a_1
2g−56T2=2a12g - \dfrac{5}{6}T_2 = 2a_1

Substituting T2=a1+g2T_2 = \dfrac{a_1 + g}{2} into the above equation:
2g−56(a1+g2)=2a12g - \dfrac{5}{6}\left(\dfrac{a_1 + g}{2}\right) = 2a_1
2g−512g=2a1+512a12g - \dfrac{5}{12}g = 2a_1 + \dfrac{5}{12}a_1
1912g=2912a1⇒a1=19g29\dfrac{19}{12}g = \dfrac{29}{12}a_1 \Rightarrow a_1 = \dfrac{19g}{29} (upwards)

Now, finding T2T_2:
T2=19g29+g2=24g29T_2 = \dfrac{\dfrac{19g}{29} + g}{2} = \dfrac{24g}{29}

Finding the accelerations a2a_2 and a3a_3:
a2=g−T22=g−12g29=17g29a_2 = g - \dfrac{T_2}{2} = g - \dfrac{12g}{29} = \dfrac{17g}{29} (downwards)
a3=g−T23=g−8g29=21g29a_3 = g - \dfrac{T_2}{3} = g - \dfrac{8g}{29} = \dfrac{21g}{29} (downwards)

To find the time elapsed before m1m_1 strikes the upper pulley, we use the kinematic equation s=ut+12at2s = ut + \dfrac{1}{2}at^2.
Given s=20 cm=0.2 ms = 20 \text{ cm} = 0.2 \text{ m}, u=0u = 0, and a1=19g29a_1 = \dfrac{19g}{29}.
0.2=12×(19×9.829)×t20.2 = \dfrac{1}{2} \times \left(\dfrac{19 \times 9.8}{29}\right) \times t^2
0.4=186.229t20.4 = \dfrac{186.2}{29} t^2
t2=0.4×29186.2≈0.0623t^2 = \dfrac{0.4 \times 29}{186.2} \approx 0.0623
t≈0.25 st \approx 0.25 \text{ s}

Answer: 19g29\dfrac{19g}{29} (up), 17g29\dfrac{17g}{29} (down), 21g29\dfrac{21g}{29} (down), 0.25 s0.25 \text{ s}
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