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Work Energy and Power Test - 30

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Work Energy and Power Test - 30
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  • Question 1
    1 / -0
    In a vertical circle of radius $$(r)$$, at what point in its path a particle may have tension equal to zero:
    Solution
    Let the tension in the string at the highest point be  $$T$$
    Minimum speed required by the particle at the highest point to complete the vertical circular motion is  $$\sqrt{gr}$$
    $$\therefore$$         $$\dfrac{mv^2}{r}   =T + mg$$

    OR        $$\dfrac{m (gr)}{r}   = T+mg$$                 $$\implies T =0$$
    Thus tension can be zero at the highest point.

  • Question 2
    1 / -0
    A stone attached to one end of a string is whirled in a vertical circle. The tension in the string is maximum when
    Solution
    $$Answer:-$$ C
    When the stone is at the bottom position forces acting on stone are:
    Upward force tension (T), Downward forces are weight (mg) and also $$\dfrac{mv^2}{R}$$ centrifugal force 
    So balancing forces we get :
    $$T=mg+\dfrac{mv^2}{R}$$
    And minimum tension is obtained at highest point which will be:
    $$T=mg-$$ $$\dfrac{mv^2}{R}$$
  • Question 3
    1 / -0
    A position dependent force $$F=7-2x+3x^{2}$$N acts on a small object of mass 2kg to displace it from $$x=0$$ to $$x=5m$$. The work done in joules is-
    Solution
    $$W=\int F\mathrm{d} x$$
    $$\displaystyle \int_{0}^{5}(7-2x+3x^{2})\mathrm{d} x=\left ( 7x-\frac{2x^{2}}{2}+\frac{3x^{3}}{3} \right )_{0}^{5}=135J$$
  • Question 4
    1 / -0
    A particle is moving in a vertical circle, the tension in the string when passing through two position at angle $$30^{\circ}$$ and $$60^{\circ}$$ from vertical from lowest position are $$T_1$$ and $$T_2$$ respectively, then 
    Solution
    In equilibrium, $$T=mv^2/r+mg\cos\theta$$
    Since, $$\theta$$ increases $$\cos\theta$$ and $$v$$ both will decrease.
    Hence, for $$\theta=60^o$$, the tension will be less.
    Thus, $$T_1>T_2$$.

  • Question 5
    1 / -0
    A pendulum bob has a speed $$3\;m/s$$ while passing through its lowest position, length of the pendulum is $$0.5\;m$$ then its speed when it makes an angle of $$60^{\circ}$$ with the vertical is
    Solution

    $$\textbf{Step 1: Apply energy conservation}$$
                    In $$\Delta ABD$$,

                  $$AB = AD \cos \theta$$

           $$\Rightarrow AB = l \cos \dfrac{\pi}{3} = \dfrac{l}{2}$$

             $$\Rightarrow h  = l - \dfrac{l}{2} = \dfrac{l}{2}$$

    As there are no dissipative force energy will be conserved.
            $$\Rightarrow (E)_i = E_f$$

            $$\Rightarrow K_1 + U_1 = K_2 + U_2$$
    Taking point $$C$$ is zero potential level

            $$\Rightarrow \dfrac{1}{2} mu^2 = \dfrac{1}{2} mv^2 + (mgh)$$

    $$\textbf{Step 2: Calculations}$$

           $$\Rightarrow v  = \sqrt{u^2 - 2gh}$$

    Putting given values
           $$v = \sqrt{(3)^2(m/s)^2 - 2 \times 9.8(m/s^2) \times \dfrac{0.5}{2}(m)} = 2 m/s$$

    Hence $$A$$ is the correct option.

  • Question 6
    1 / -0
    A particle slides from rest from the topmost point of a vertical circle of radius ($$r$$) along a smooth chord making an angle $$(\theta)$$ with the vertical the time of decent is 
    Solution

    Force on particle along the cord = $$mg\cos { \theta  }$$ 

    Distance travelled by the particle =$$\quad \dfrac { d }{ \cos { \theta  }  }$$, where $$d$$ is the diameter or the vertical circle.

    $$s = \dfrac { a{ t }^{ 2 } }{ 2 }$$

    $$\Rightarrow\  t =\sqrt { \dfrac { 2s }{ a }  }$$.

     Hence,$$\ t$$ is independent of $$\theta$$.

  • Question 7
    1 / -0
    A particle of mass $$m_{1}$$ moving with a velocity of $$5m/s$$ collides head on with a stationary particle of mass $$m_{2}$$. After collision both the particle move with a common velocity of $$4m/s$$, then the value $$m_
    {1}/m_{2}$$ is:
    Solution
    Conservation of Momentum principle,
    Initial momentum is $$M_i=5m_1$$
    Final momentum is $$M_f=4(m_1+m_2)$$
    By the above stated principle $$M_i=M_f=5m_1=4(m_1+m_2)$$
    $$\implies m_1=4m_2$$
    $$\therefore m_1:m_2=4:1$$
  • Question 8
    1 / -0
    Under the action of a force, a 2kg mass moves such that its position x as a function of time t is given by $$x=t^3/3$$ where x is in meters and t in second. The work done by the force in first two seconds is:
    Solution
    $$x=\dfrac{t^3}{3}$$
    $$ a=\dfrac{d^2x}{dt^2}=2t$$
    Thus force acting on the particle=$$ma=2mt$$
    Work done$$=\int Fdx$$
    $$=\int_0^2 (2mt)t^2dt$$
    $$=2m\int_0^2 t^3dt$$
    $$=16J$$
  • Question 9
    1 / -0
    Force shown acts for $$2$$ seconds. Find out work done by force $$F$$ on $$10$$ kg in $$3$$ seconds.

    Solution
    Work done,
    $$W=Fd$$
    Displacement $$d$$ is given by,
    $$d=\dfrac{1}{2}a{t}^{2}$$
    $$F=ma$$
    $$10=10a$$, $$a=1m/s^2$$
    $$d=\dfrac{1}{2}(1){(2)}^{2}=2m$$
    $$W=10\times2=20J$$
  • Question 10
    1 / -0
    A time dependent force F = 10 t is applied on 10 kg block. Find out the work done by F in 2 seconds.
    Solution
    $$10\, \times\, \displaystyle \dfrac{dv}{dt}\, =\, 10\, t$$

    $$\int_0^v \ dv =\int_{0}^{t} tdt$$

    $$\Rightarrow\, v\, =\, \displaystyle \dfrac{t^2}{2}$$ ..........(1)

    $$dW\, =\, \vec{F}\, .\, \vec{ds}$$
    $$dW\, =\, 10 t. dx$$
    $$dW\, =\, 10 t. v. dt$$ .......... (2) $$\because\, dx\, =\, vdt$$

    from (1) & (2) 

    $$dW\, =\, 10\, t\, .\, \left ( \displaystyle \dfrac{t^2}{2} \right )dt\, \quad\, dW\, =\, 5t^3dt$$

    $$W\, =\, \displaystyle \dfrac{5}{4}\, [t^4]_0^2\, =\, 20\, J$$ 
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