Theory of Machines Miscellaneous


Theory of Machines Miscellaneous

  1. For an under damped harmonic oscillator, resonance









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    For underdamped harmonic oscillator,
    ωd = ωn

    Correct Option: C

    For underdamped harmonic oscillator,
    ωd = ωn


  1. A uniform stiff rod of length 300 mm and having a weight of 300 N is pivoted at one end and connected to a spring at the other end. For keeping the rod vertical in a stable position the minimum value of spring constant K needed is










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    NA

    Correct Option: C

    NA



  1. The assembly shown in the figure is composed of two massless rods of length l with two particles, each of mass m. The natural frequency of this assembly for small oscillations is










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    Net restoring torque when displaced by a small angle θ
    τ = mg cos (α – θ) l – mg (α + θ)l
    = 2 mgl cos α sin θ
    For very small θ, sin θ ≈ θ
    ∴ τ = 2mgl cos α . θ (restorative)

    Now , I
    d2θ
    + 2mgl cosα . θ = 0
    dt2

    But I = 2ml2
    ∴ 2ml2
    d2θ
    + 2mgl cosα . θ = 0
    dt2

    or
    d2θ
    +
    g cosα
    θ = 0
    dt2l

    ∴ ωn = √
    g cosα
    l

    Correct Option: D

    Net restoring torque when displaced by a small angle θ
    τ = mg cos (α – θ) l – mg (α + θ)l
    = 2 mgl cos α sin θ
    For very small θ, sin θ ≈ θ
    ∴ τ = 2mgl cos α . θ (restorative)

    Now , I
    d2θ
    + 2mgl cosα . θ = 0
    dt2

    But I = 2ml2
    ∴ 2ml2
    d2θ
    + 2mgl cosα . θ = 0
    dt2

    or
    d2θ
    +
    g cosα
    θ = 0
    dt2l

    ∴ ωn = √
    g cosα
    l


  1. In the figure shown, the spring deflects by δ to position A (the equilibrium position) when a mass m is kept on it. During free vibration, the mass is at position B at some instant. The change in potential energy of the spring mass system from position A to position B is










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    Potential energy at A = mg (l – δ)

    Total energy at B = mg [l – (δ + x)] +
    1
    kx2
    2

    ∴ Change in energy = mgl – mg(δ + x) +
    1
    kx2 - mgl + mgδ
    2

    =
    1
    kx2 - mgx . δ
    2

    Correct Option: A

    Potential energy at A = mg (l – δ)

    Total energy at B = mg [l – (δ + x)] +
    1
    kx2
    2

    ∴ Change in energy = mgl – mg(δ + x) +
    1
    kx2 - mgl + mgδ
    2

    =
    1
    kx2 - mgx . δ
    2



  1. As shown in figure, a mass of 100 kg is held between two springs. The natural frequency of vibration of the system in cycle/s, is










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    S = S1 + S2 = 20 + 20 = 40 kN/m = 40,000 N/m
    ∴ Natural frequency of vibration of the system,

    fn =
    1
    S / m

    fn =
    1
    (400 × 1000)/ 100 =
    20

    fn =
    10
    π

    Correct Option: C

    S = S1 + S2 = 20 + 20 = 40 kN/m = 40,000 N/m
    ∴ Natural frequency of vibration of the system,

    fn =
    1
    S / m

    fn =
    1
    (400 × 1000)/ 100 =
    20

    fn =
    10
    π