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Laws of Motion Test - 35

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Laws of Motion Test - 35
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  • Question 1
    1 / -0
    What is the value of $$p_1$$ and $$m_2$$ ?
    m (kg)v (m/s)p = mv (kgm/s)
    8560$$p_1$$
    $$m_2$$2.56.25
    Solution
    m (kg)v (m/s)p = mv (kgm/s)
    85605100
    2.5
    2.56.25
    In first case:
    $$ m=85kg $$
    $$v =60 m/s$$
    $$ p =mv = 85 \times 60 = 5100\ kg m/s$$
    In second  case:
    $$ m=? $$
    $$v =2.5 m/s$$
    $$ p =mv = 6.25 $$
    $$\therefore m = \dfrac{p}{v} = \dfrac{6.25}{2.5} = 2.5\ kg$$
  • Question 2
    1 / -0
    A stone tied to a string of length $$L$$ is swired in a verticle circle with the other end of the string at the centre. At a certain instant of time the stone is at it lowest position and has a speed $$u$$. Find the magnitude of the change in its velocity as it reaches a position, where the string is horizontal.
    Solution
    By using conservation of energy,
    $$\frac { 1 }{ 2 } m{ u }^{ 2 }=mgL+\frac { 1 }{ 2 } m{ v }^{ 2 }$$
    $$\Rightarrow v=\sqrt { { u }^{ 2 }-2gL }$$
    Change in velocity = $$\sqrt { { u }^{ 2 }-2gL } \hat { i } -u\hat { j }$$
    Magnitude of change in velocity = $$\sqrt { { u }^{ 2 }-2gL+{ u }^{ 2 } } =\sqrt { 2\left( { u }^{ 2 }-gL \right)  } $$

  • Question 3
    1 / -0
    A bob is suspended from a crane by a cable of length $$5m$$. The crane and load are moving at a constant speed $$v_{0}$$. The crane is stopped by a bumper and the bob on the cable swings out an angle of $$60^{\circ}$$. Find the initial speed $$v_{0}.(g=9.8 m/s^{2})$$

    Solution
    By using conservation of energy, from the initial point to the highest point
    $$\frac { 1 }{ 2 } m{ { v }_{ 0 } }^{ 2 }=mgl(1-cos{ 60 }^{ 0 })$$ 
    $$\Rightarrow { v }_{ 0 }=\sqrt { 2gl(1-cos{ 60 }^{ 0 }) } =\sqrt { gl } =\sqrt { 50 } =7m/s$$
  • Question 4
    1 / -0
    A simple pendulum is vibrating with angular amplitude of $$\theta=90^{o}$$ as shown in figure.
    For what value of $$\theta$$ is the acceleration directed
    $$(i)$$ Vertically upwards
    $$(ii)$$ Horizontally
    $$(iii)$$ Vertically downwards

    Solution
    Acceleration of a simple pendulum is $$a = -ω^{2}\times A\times cos  (ωt + θ)$$, where ω is angular velocity, $$A$$ is amplitude, $$t$$ is time and θ is angle.
    If θ is $$0$$, then $$a = -ω^{2}\times A\times cos (ωt)$$ so direction is vertically upwards, when θ is $$cos^{-1} (1/3^{1/2})$$ then direction is horizontally, when θ is $$90^o$$, then $$a = ω^{2}\times A\times sin (ωt)$$ so direction is vertically downwards.
  • Question 5
    1 / -0
    A pendulum bob is raised to a height, $$h$$, and released from rest. At what height will it attain half of its maximum speed?
    Solution
    By energy conservation, $$\dfrac{1}{2}mv^2_{max} = mgh$$
    Let at height $$h'$$, it attain velocity $$v'=\dfrac{v_{max}}{2} = \sqrt{gh/2}$$
    Now, $$mgh = \dfrac{1}{2}mv'^2 + mgh'$$

    or $$mgh = \dfrac{mgh}{4} + mgh'$$

    or $$mgh'=\dfrac{3}{4}mgh$$

    $$\therefore h' = \dfrac{3h}{4}$$
  • Question 6
    1 / -0

    Directions For Questions

    A small particle of mass $$m$$ attached with a light inextensible thread of length $$L$$ is moving in a vertical circle. In the given case particle is moving in complete vertical circle and ratio of its maximum to minimum velocity is $$2:1$$.

    ...view full instructions

    The kinetic energy of particle at the lower most position is

    Solution
    As  $$v= 2\sqrt{\dfrac{gL}{3}}$$
    Also,  $$u= 2v          \implies  u= 4\sqrt{\dfrac{gL}{3}}$$
    Thus      $$K.E_ A= \dfrac{1}{2}mu^2=  \dfrac{8mgL}{3}$$
  • Question 7
    1 / -0

    Directions For Questions

    Bob B of the pendulum AB is given an initial velocity $$\displaystyle \sqrt{3Lg}$$ in horizontal direction. Find the maximum height of the bob from the starting point:

    ...view full instructions

    if AB is a massless string.

    Solution

    When the string has traversed an angle $$\theta$$ , then

    $$T-mgcos\theta =\dfrac { m{ v }^{ 2 } }{ l }$$ , and conservation of energy gives

    $$\dfrac { m{ u }^{ 2 } }{ 2 } =\dfrac { m{ v }^{ 2 } }{ 2 } +mgl(1-cos\theta ).$$ then the string becomes slacked tension in the string becomes zero. Solving the above two equations to get the value of $$\theta$$

    $$\Rightarrow cos\theta =\dfrac { -1 }{ 3 }  and { v }^{ 2 }={ u }^{ 2 }-2gl(1-cos\theta )=\dfrac { gl }{ 3 } $$ from that point the maximum height reached is $$\dfrac { { v }^{ 2 }{ sin }^{ 2 }\left( \pi -\theta  \right)  }{ 2g }$$ maximum height $$= l(1-cos\theta )+\dfrac { { v }^{ 2 }{ sin }^{ 2 }\left( \pi -\theta  \right)  }{ 2g } =\dfrac { 4l }{ 3 } +\dfrac { 4l }{ 27 } =\dfrac { 40l }{ 27 } $$

  • Question 8
    1 / -0
    A simple pendulum of length $$l$$ has maximum angular displacement $$\displaystyle \theta .$$ Then maximum kinetic energy of a bob of mass $$m$$ is
    Solution
    At point B,  $$v=0$$ and $$P.E$$ is maximum.
    At point A,  $$P.E= 0$$ and $$K.E$$ is maximum.
    Height of bob at B,  $$AP= l-lcos\theta= l(1-cos\theta)$$
    Thus $$P.E= mgl(1-cos\theta)$$
    Applying conservation of energy at A and B,    $$K.E_m +0 = 0 + P.E$$
    $$\implies K.E_m=mgl (1-cos\theta) $$

  • Question 9
    1 / -0
    A car is travelling along a circular curve that has a radius of $$50 m$$. If its speed is $$16 m/s$$ and is increasing uniformly at $$8 m/s$$ $$^{2}$$. Determine the magnitude of its acceleration at this instant.
    Solution
    Given:    $$r  =50  $$ m            $$v  = 16$$  m/s            $$a_t  =8  m/s^2$$
    Radial acceleration of the car at that instant, $$a_r  = \dfrac{v^2}{r}  = \dfrac{16^2}{50}  = 5.12$$  $$m/s^2$$

    $$\therefore$$ Net acceleration of the car  $$a  = \sqrt{a_r^2 + a_t^2}  = \sqrt{(5.12)^2 + 8^2}  = 9.5  m/s^2$$
  • Question 10
    1 / -0

    Directions For Questions

    A small particle of mass $$m$$ attached with a light inextensible thread of length $$L$$ is moving in a vertical circle. In the given case particle is moving in complete vertical circle and ratio of its maximum to minimum velocity is $$2:1$$.

    ...view full instructions

    Velocity of particle when it is moving vertically downward is

    Solution
    Work-energy theorem  for A to C,   $$-mgL= \dfrac{1}{2}m(v')^2- \dfrac{1}{2}mu^2$$     where $$u= 4\sqrt{\dfrac{gL}{3}}$$
    $$-mgL= \dfrac{1}{2}m(v')^2- \dfrac{8mgL}{3}$$
    $$\implies v'= \sqrt{\dfrac{10 gL}{3}}$$ 

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