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Basic Science Test 11

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Basic Science Test 11
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  • Question 1
    1 / -0
    Figure shows the graph of x-coordinate of a particle moving along x-axis as  function of time. Average velocity during t=0t=0 to 6s6s and instantaneous velocity at t=3st=3s respectively, will be 

    Solution
    Velocity= slope of x-t graph=0 (at t=35t=35)
    Net displacement from t=0t=0 to t=6s=0t=6s=0
    Ave. velocity=Netdisplacementtime=06=0=\cfrac{Net\quad displacement}{time}=\cfrac{0}{6}=0
  • Question 2
    1 / -0
    A bob of a simple pendulum of length 2m2m is moved sideways and whirled in horizontal circle of radius 1.732m1.732m. If the mass of the bob is 2kg2kg, then tension in the string is
    Solution
    sinθ=1.7322\sin\theta=\frac{1.732}{2}
    sinθ=32\sin\theta=\frac{\sqrt{3}}{2}
    θ=600\theta=60^0
    Tcosθ=mgT\cos\theta=mg
    T=mgcosθ=29.8cos600=19.612=39.8NT=\frac{mg}{\cos\theta}=\frac{2*9.8}{\cos60^0}=\frac{19.6}{\frac{1}{2}}=39.8N

  • Question 3
    1 / -0
    A particle is in uniform circular motion, then its velocity is perpendicular to
    Solution
    VacV\bot a_c
    if in uniform circular motion then only centripetal force occurs
    net force =centripetal force
    so netforce av\bot a_v
  • Question 4
    1 / -0
    A wheel of mass 40kg40kg and radius of gyration 0.5m0.5m comes to rest from a speed of 1800r±1800r\pm in 30s30s. Assuming that the retardation is uniform, the value of the retarding torque in NmNm, is
    Solution
    τ=Iα\tau =I\alpha
    =(mk2).α=(m{k}^{2}).\alpha
    =40×(0.5)2×2π=40\times {(0.5)}^{2}\times 2\pi
    =20π=20\pi rad/s
  • Question 5
    1 / -0
    What is the minimum coefficient of friction for a solid sphere to roll without slipping on an inclined plane of inclination θ\theta?
    Solution
    Here we are talking about minimum coefficient of friction this suggests that friction acting would be μmgcosθ\mu mg\cos\theta
    taking moment about centre,
    μmgcosθr=Iα\mu mg\cos\theta*r=I*\alpha
    or, =μmgcosθr2I=\frac{\mu mg\cos\theta_{r}^2}{I}
    now, from force balance,
    mgsinθμmgcosθ=mamg\sin\theta-\mu mg\cos\theta=ma
    a=gsinθμgcosθa=g\sin\theta-\mu g\cos\theta
    from condition of rolling we know that
    a=rαa=r\alpha
    μmgcosθr2I=gsinθμmgcosθ\frac{\mu mg\cos\theta_{r}^2}{I}=g\sin\theta-\mu mg\cos\theta
    simplifying this, we get
    μ=tanθ1+mr2I\mu=\frac{\tan\theta}{1+\frac{mr^2}{I}}
    I=25mr2I=\frac{2}{5}mr^2
    Putting the value of moment of ionertia in expression of coefficient of friction we get,
    μ=27tanθ\mu=\frac{2}{7}\tan\theta

  • Question 6
    1 / -0
    A body is started from rest with acceleration 2m/s22 m/s^{2} till it attains the maximum velocity then retards to rest with 3 m/s2m/s^{2} It total time taken is 10 second then maximum speed attained is
  • Question 7
    1 / -0
    A partice is at rest and it is at origin (0,0)(0,0) at t=0t=0. If velocity varies as v=kx2v=k{x}^{2} where vv is the velocity and xx is displacement. Find how much distance it will travel in 22 sec
    Solution
    V=kx2V=k{x}^{2}
    dxdt=kx2\cfrac{dx}{dt}=k{x}^{2}
    dx=kx2dtdx=k{x}^{2}dt
    0x1x2 =02xdt\int _{ 0 }^{ x }{ \cfrac { 1 }{ { x }^{ 2 } }  } =\int _{ 0 }^{ 2 }{ x } dt
    1x=[kt] 02-\cfrac{1}{x}={ \left[ kt \right]  }_{ 0 }^{ 2 }
    1x=k2-\cfrac{1}{x}=k2
    x=12kx=-\cfrac{1}{2k}
    1x=kt+k-\cfrac{1}{x}=kt+k
    at t=0t=0 and d=0d=0
    k=k=\infty
    x=12x=-\cfrac{1}{2\infty}
    k=0k=0
  • Question 8
    1 / -0
    Two identical rings each of  mass m  with their planes mutually  perpendicular , radius R are welded at their point of contact O . If the system is free to rotate about an axis passing through the point p perpendicular to the plane of the paper the moment  of inertia of the system about this axis equal to : 


    Solution
    Answer
    I = I1+I1 I  =  I_{1} + I_{1}
    I1 =mr22+M(2R+R)2  =9.5MR2 I_{1}  = \dfrac{mr^{2}}{2} + M (2R + R)^{2}   = 9.5MR^{2}
    I2=mr22+ MR2=2MR2 I_{2} = \dfrac{mr^{2}}{2} +  MR^{2} = 2 MR^{2}
    I=I1+I2 I = I_{1} + I_{2}
    I=9.5Mr2+MR2 I = 9.5Mr^{2} + M R^{2}
    I=11.5MR2 I= 11.5MR^{2}
  • Question 9
    1 / -0
    A body is thrown up with a velocity 29.23ms!29.23ms! VV distance travelled in last second of upward motion is 
    Solution
    Total time of motion:
    v=u+atv=u+at
    x0=29.239.8×6x_0=29.23-9.8\times 6
    xt=2.98 secxt=2.98\ sec
    distance total 
    v2=u2+2as\Rightarrow v^2=u^2+2as
    0=(29.23)2=2×9.8×s\Rightarrow 0=(29.23)^2=2\times 9.8 \times s
    s=43.59 m\Rightarrow s=43.59\ m
    Now in 1.96 sec1.96\ sec
    s=29.3×1.9812×9.8(1.98)2s=29.3\times 1.98-\dfrac{1}{2}\times 9.8 (1.98)^2
    s=36.6654s=36.6654
    in last s=43.5938.66s= 43.59-38.66
    =4.93m=4.93m
  • Question 10
    1 / -0
    A body is projected with velocity 'u' so that the maximum height is thrice the horizontal range. Then the maximum height is
    Solution
    Hmax=42sin2θ2gH_{max} = \dfrac{4^2sin^2\theta}{2g}
    Range =42sin2θg=42sinθcosθg= \dfrac{4^2sin2\theta}{g} = \dfrac{4^2sin\theta\,cos\theta}{g}
    H3=R=4sin2θ2×3g=4sinθcosθg\dfrac{H}{3} = R = \dfrac{4sin2\theta}{2 \times 3g} = \dfrac{4sin\theta\,cos\theta}{g}
    tanθ=121tan\theta = \dfrac{12}{1}
    sinθ=12122+12=1145sin\theta = \dfrac{12}{\sqrt{12^2 + 1^2}} = \dfrac{1}{\sqrt{145}}
    Hmax=42sin2θ2g=42(12145)22gH_{max} = \dfrac{4^2sin^2\theta}{2g} = \dfrac{4^2\left ( \dfrac{12}{\sqrt{145}} \right )^2}{2g}
    =42×144145×2×g=72u2145g= \dfrac{4^2 \times 144}{145 \times 2 \times g} = \dfrac{72u^2}{145\,g}
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