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Physics Test - 22

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Physics Test - 22
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  • Question 1
    4 / -1

    The excess pressure inside a spherical drop of water is four times that of another drop. Then, their mass ratio is

    Solution
    \(\frac{2 T}{r_{1}}=4 \times \frac{2 T}{r_{2}} \Rightarrow r_{2}=4 r_{1}\)
    Mass ratio \(=M_{1}: M_{2}=r_{1}^{3}: r_{2}^{3}=1: 64\)
  • Question 2
    4 / -1

    A balloon starts rising from the ground with an acceleration of 1.25 m/s2. After 8 s, a stone is released from the balloon. The stone will, after release from the balloon,

    Solution
    Velocity of the balloon after 8 sec
    \(\mathrm{v}=\mathrm{u}+\mathrm{at}=0+1.25 \mathrm{x} 8=10 \mathrm{m} / \mathrm{s}\)
    Height attained by the balloon after 8 sec \(\mathrm{H}=\mathrm{ut}+\frac{1}{2} \mathrm{at}^{2}=0+\frac{1}{2} \times 1.25 \times\left(8 \mathrm{s}^{2}=40 \mathrm{m}\right.\)
    Stone will have same velocity as that of balloon, after 8 sec, the stone will travel under acceleration due
    to gravity.
    Distance travelled by the stone before coming to rest \(\mathrm{v}^{2}-\mathrm{u}^{2}=2 \mathrm{as} \Rightarrow \mathrm{s}=\frac{10 \times 10}{2 \times 10}=5 \mathrm{m}\)
    Time taken by the stone to reach the ground
    Displacement \(=-40 \mathrm{m}, \mathrm{u}=+10 \mathrm{m} / \mathrm{s}\) and \(\mathrm{a}=-10 \mathrm{m} / \mathrm{s}^{2}\)
    \(-40=10 t-\frac{1}{2} \times 10 \times t^{2} \Rightarrow-8=2 t-t^{2}\)
    \(t^{2}-2 t-8=0\)
    \(\Rightarrow(t-4)(t+2)\)
    Neglecting the negative value, we get \(t=4\) sec
  • Question 3
    4 / -1

    A particle in SHM is described by the displacement equation x(t) = A cos (ωt + θ). If the initial (t = 0) position of the particle is 1 cm and its initial velocity is π cm/s, then what is its amplitude? (The angular frequency of the particle is πs-1.)

    Solution
    Rate of change of displacement gives velocity. Given, \(\quad x=A \cos (\omega t+\theta)\)
    Velocity \(v=\frac{d x}{d t}=A \frac{d}{d t} \cos (\omega t+\theta)\)
    \(v=-A \omega \sin (\omega t+\theta)\)
    Using \(\sin ^{2} \theta+\cos ^{2} \theta=1,\) we have
    \(v=-A \omega \sqrt{1-\cos ^{2}(\omega t+\theta)}\)
    \(\therefore\) From equation \(x=A \cos (\omega t+\theta),\) we have \(v=-A \omega \sqrt{1-x^{2} / A^{2}}\)
    \(\Rightarrow \quad v=-\omega \sqrt{A^{2}-x^{2}}\)
    Given, \(v=\pi \mathrm{cm} / \mathrm{s}, x=1 \mathrm{cm}, \omega=\pi \mathrm{s}^{-1}\)
    \(\therefore \quad \pi=-\pi \sqrt{A^{2}-1}\)
    \(\Rightarrow \quad 1=A^{2}-1\)
    \(\Rightarrow A=\sqrt{2} \mathrm{cm}\)
  • Question 4
    4 / -1

    From the top of a tower, a stone is thrown up and reaches the ground in time t1 = 9 s. A second stone is thrown down with the same speed and reaches the ground in time t2 = 4 s. A third stone is released from rest and reaches the ground in time t3, which is equal to

    Solution
    Taking the downward direction as positive Displacement of first stone,
    \[
    h=-u t_{1}+\frac{1}{2} g t_{1}^{2}
    \]
    Displacement of second stone,
    \[
    h=u t_{2}+\frac{1}{2} g t_{2}^{2}
    \]
    Displacement of third stone,
    \[
    h=\frac{1}{2} g t_{3}^{2}
    \]
    Multiplying Eq. (1) by \(t_{2}\) and Eq. (2) by \(t_{1}\) and adding, we get
    \[
    h\left(t_{1}+t_{2}\right)=\frac{1}{2} g t_{1} t_{2}\left(t_{1}+t_{2}\right)
    \]
    \(\Rightarrow \quad h=\frac{1}{2} g t_{1} t_{2}\)
    From Eqs. (3) and (4), \(t_{3}^{2}=t_{1} t_{2}\)
    or \(t_{3}=\sqrt{t_{1} t_{2}}=\sqrt{9 \times 4}=6 \mathrm{s}\)
  • Question 5
    4 / -1

    Two balls marked 1 and 2 of the same mass m and a third ball marked 3 of mass M are arranged over a smooth horizontal surface as shown in the figure. Ball 1 moves with a velocity v1toward balls 2 and 3. All collisions are assumed to be elastic. If M < m, the number of collisions between the balls will be

    Solution
    The first collision will be between balls 1 and \(2 .\) since both have the same mass, after the collision ball 1
    win come to rest and ball 2 win move with speed \(v_{1} .\) This ball will collide with the stationary ball 3 .
    Alter this second collision, let \(v_{2}\) and \(v_{3}\) be the speeds of balls 2 and 3 respectively. since the collisions
    are elastic, \(\mathrm{v}_{2}\) and \(\mathrm{v}_{3}\) are given by
    \[
    v_{2}=\left(\frac{m-M}{m+M}\right) v_{1}
    \]
    (i)
    and \(v_{3}=\left(\frac{2 m}{m+M}\right) v_{1}\)
    (ii)
    If \(\mathrm{M}<\mathrm{m},\) it follows from (i) and (ii) that \(\mathrm{v}_{2}<\mathrm{v}_{3}\) and both have the same direction. Therefore, ball 2
    cannot collide with ball 3 again. Hence there are only two collisions.
  • Question 6
    4 / -1

    A spring of force constant k is cut into two pieces such that one piece is double the length of the other. The force constant of the longer piece will be

    Solution
    The force constant of a spring is inversely propor. tional to its length. If a spring of length \(L\) is cut into two pieces of lengths \(x\) and \((L-x)\), such that
    \[
    x=2(L-x) \text { or } x=\frac{2 L}{3}
    \]
    then the force constant of the spring of length \(x\) is related to the force constant \(k\) of the complete spring of length \(L\) as
    \[
    \frac{k_{1}}{k}=\frac{L}{x}=\frac{L}{2 L / 3}=\frac{3}{2} \text { or } k_{1}=\frac{3}{2} k
    \]
  • Question 7
    4 / -1

    A particle has an initial velocity of 9 m/s due east and a constant acceleration of 2 m/s2 due west. The distance covered by the particle in the fifth second of its motion is

    Solution

    The displacement is indeed 0 but not the distance. the distance covered is 0.5 m.

    Actually, the car is changing the direction of motion at 4.5 seconds. As such displacement between 4 and 5 seconds is 0 but still the car covers some distance.

    The distance is the mod of displacement made by the car between 4 and 4.5 seconds + mod of the displacement between 4.5 and 5 seconds.

    Displacement b/w 4 to 4.5 seconds = (9)(0.5) - (4.52 - 42) = 4.5 - 4.25 = 0.25

    Displacement b/w 4.5 to 4 seconds = (9)(0.5) - (52 - 4.52) = 4.5 - 4.75 = -0.25

    Displacement = 0, Distance = 0.5 m

  • Question 8
    4 / -1

    A block released on a rough inclined plane of inclination = 30° slides down the plane with an acceleration g/4, where g is the acceleration due to gravity. What is the coefficient of friction between the block and the inclined plane?

    Solution

    Acceleration of an object down the incline is 'a
    ma \(=m g \sin \theta-f\)
    \(f=\mu N=\mu m g \cos \theta\)
    \(a=g \sin \theta-\mu g \cos \theta\)
    \(\theta=30^{\circ}\)
    \(\frac{9}{4}=g\left(\sin 30^{\circ}-\mu \cos 30^{\circ}\right)\)
    \(\frac{1}{2}-\mu \frac{\sqrt{3}}{2}=\frac{1}{4} \Rightarrow \mu \frac{\sqrt{3}}{2}=\frac{1}{4}\)
    \(\mu=\frac{1}{2 \sqrt{3}}\)
  • Question 9
    4 / -1

    A boy, while catching a ball, experiences an impulse of 6 Ns. If the mass of the ball is 200 g, then what was the speed of the ball before it was caught?

    Solution
    Impulse = Change in momentum
    Let v be the speed of the ball before it was caught and \(m\) be its mass.
    since the ball is brought to rest after it is caught, the change in momentum \(=\mathrm{mv}\). Now, \(m=0.2 \mathrm{kg} .\) Therefore, impulse is \(0.2 \mathrm{v}\). Given, impulse \(=6 \mathrm{Ns}\) Hence, \(v=\frac{6}{0.2}=30 \mathrm{ms}^{-1}\)
    Thus, the correct choice is (2) .
  • Question 10
    4 / -1

    The angular velocity of a planet revolving in an elliptical orbit around the sun __________ when it comes near the sun

    Solution
    If we consider planet and the sun as one system, then the force of gravitation between the sun and the
    planet is a central force hence no torque is generated about sun ..It means angular momentum of the planet is consereved \(L=I \omega=\) costant. As the planet comes near to the sun, Moment of I nertia
    decreases which means there will be increase in the angular veloicty of the planet.
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