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JEE Main 201912 JanuaryEvening Shift
Exam
JEE Main
Year
2019
Date
12 January
Shift
Evening Shift
Subject
Physics
Chapter
Mechanical Properties of Fluids

JEE Main 2019 · 12 January · Evening Shift · Physics · Mechanical Properties of Fluids

A soap bubble, blown by a mechanical pump at the mouth of a tube...

A soap bubble, blown by a mechanical pump at the mouth of a tube increases in volume with time at a constant rate. The graph that correctly depicts the time dependence of pressure inside the bubble is given by:A soap bubble, blown by a mechanical pump at the mouth of a tube increases in volume with time at a constant rate. TheA soap bubble, blown by a mechanical pump at the mouth of a tube increases in volume with time at a constant rate. TheA soap bubble, blown by a mechanical pump at the mouth of a tube increases in volume with time at a constant rate. TheA soap bubble, blown by a mechanical pump at the mouth of a tube increases in volume with time at a constant rate. The

Options

  1. AMatch List-I with List-II List-I List-II (A) Moment of inertia of solid sphere of radius R about any tangent. (I)
  2. BMatch List-I with List-II List-I List-II (A) Moment of inertia of solid sphere of radius R about any tangent. (I)
  3. CMatch List-I with List-II List-I List-II (A) Moment of inertia of solid sphere of radius R about any tangent. (I)
  4. DMatch List-I with List-II List-I List-II (A) Moment of inertia of solid sphere of radius R about any tangent. (I)

Correct answer

D. Match List-I with List-II List-I List-II (A) Moment of inertia of solid sphere of radius R about any tangent. (I)

Step-by-step solution

dVdt=k\dfrac{dV}{dt} = k

⇒V=kt⇒ V = kt

⇒43πr3=kt⇒ \dfrac{4}{3}\pi{r}^{3} = kt

⇒r=(3k4π)13t13⇒ r = {\left(\dfrac{3k}{4\pi}\right)}^{\dfrac{1}{3}}{t}^{\dfrac{1}{3}}

P−P0=4TrP - {P}_{0} = \dfrac{4T}{r}

⇒P−P0=4T.(3k4π)13.1t13⇒ P - {P}_{0} = 4T . \left(\dfrac{3k}{4\pi}\right)\dfrac{1}{3} . \dfrac{1}{t\dfrac{1}{3}}⇒P=4T.(3k4π)13.1t13+P0⇒ P = 4T . \left(\dfrac{3k}{4\pi}\right)\dfrac{1}{3} . \dfrac{1}{t\dfrac{1}{3}} + {P}_{0}

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