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Theory of Machines Test 3

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Theory of Machines Test 3
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  • Question 1
    1 / -0
    In a rim type flywheel, mass is distributed uniformly throughout. On a second rim type flywheel, mass is concentrated at 1/2 of the initial radius. If both wheels are rotating at the same angular velocity, what is the ratio of energy stored in the first flywheel to the second flywheel?
    Solution

    Concept:

    \(E = \frac{1}{2}I{\omega ^2}\)

    Calculation:

    For first flywheel,

    \({E_1} = \frac{1}{2}\left( {m{r^2}} \right){\omega ^2}\)

    For second flywheel,

    \({E_2} = \frac{1}{2}\left[ {m{{\left( {\frac{r}{2}} \right)}^2}} \right]{\omega ^2}\)

    \({E_2} = \frac{1}{8}m{r^2}{\omega ^2}\)

    Now,

    \(\frac{{{E_1}}}{{{E_2}}} = \frac{{\frac{1}{2}\;m{r^2}{\omega ^2}}}{{\frac{1}{8}\;m{r^2}{\omega ^2}}}\)

    \(\frac{{{E_1}}}{{{E_2}}} = 4\)

  • Question 2
    1 / -0
    A flywheel is fitted to the crank shaft of an engine having W amount of indicated work per revolution. Permissible limits of coefficient of fluctuation of energy and speed are CE and CS respectively. The kinetic energy of the flywheel is given by
    Solution

    Concept:

    Coefficient of fluctuation of energy:

    \({C_E} = \frac{{Maximum\;fluctuation\;of\;energy}}{{Work\;done\;per\;cycle}}\)

    \({C_E} = \frac{\Delta E}{W} \Rightarrow \Delta E=C_E.W\)

    Coefficient of fluctuation of speed:

    \(\begin{array}{l} {C_S} = \frac{{Maximum\;fluctuation\;of\;speed}}{{Mean\;speed}}\\ {C_S} = \frac{{{ω _1} - {ω _2}}}{ω } = \frac{{2\left( {{ω _1} - {ω _2}} \right)}}{{\left( {{ω _1} + {ω _2}} \right)}} \end{array}\)

    ω = mean angular speed during the cycle (rad/s)

    \(ω = \frac{{{ω _1} + {ω _2}}}{2}\)

    Maximum fluctuation of energy: ΔE = CE. W

    \(\begin{array}{l} {\rm{\Delta }}E = \frac{1}{2}Iω _1^2 - \frac{1}{2}Iω _2^2 = \frac{1}{2}I\left( {{ω _1} + {ω _2}} \right)\left( {{ω _1} - {ω _2}} \right)\\ {\rm{\Delta }}E = Iω \left( {{ω _1} - {ω _2}} \right) = I{ω ^2}\frac{{\left( {{ω _1} - {ω _2}} \right)}}{ω } = I{ω ^2}{C_S}\\ K.E = \frac{1}{2}I{ω ^2} = \frac{1}{2}.\frac{{{\rm{\Delta }}E}}{{{C_S}}} = \frac{{{C_E}W}}{{2{C_S}}} \end{array}\)

  • Question 3
    1 / -0
    If maximum and minimum equilibrium speed of governor are 700 rpm and 300 rpm respectively. What is the sensitivity of governor?
    Solution

    Concept:

    \({\rm{Sensitivity\;of\;governor\;}} = \frac{{{\omega _{max}} - {\omega _{min}}}}{{{\omega _{mean}}}}\)

    Calculation:

    Given: ωmax = 700 rpm, ωmin = 300 rpm

    Now,

    \({\omega _{mean}} = \frac{{700 + 300}}{2} = 500\;rpm\)

    \(\therefore {\rm{Sensitivity}} = \frac{{700 - 300}}{{500}}\)

    Sensitivity = 0.8

  • Question 4
    1 / -0

    For a porter governor the following data is obtained.

    Mass of fly balls = 4 kg each, Mass of sleeve = 20 kg, Power = 4 J, Maximum rise of sleeve = 250 mm

    For the information given above, calculate the fraction change in speed. (round up to two decimal places)
    Solution

    Concept:

    Power of generator is given as

    \(P = \left( {m + M} \right)gh\;\left( {\frac{{4{c^2}}}{{1\; + \;2c}}} \right)\)

    Calculation:

    Given:

    Mass of fly balls (m) = 4 kg, Mass of sleeve (M) = 20 kg, Maximum rise of sleeve (h) = 250 mm = 0.25 m, Power = 4 J

    \(P = \left( {m + M} \right)gh\;\left( {\frac{{4{c^2}}}{{1\; + \;2c}}} \right)\)

    \(4 = \left( {4 + 20} \right)9.81 \times 0.25 \times \frac{{4{c^2}}}{{1\; + \;2c}}\)

    \( \Rightarrow 4 + 8c = 24 \times 9.81 \times \frac{1}{4} \times 4{c^2}\)

    4 + 8c = 24 × 9.81 c2

    ⇒ 58.86c2 – 2c – 1 = 0

    ∴ c = 0.1484

  • Question 5
    1 / -0
    Torque requirement of a punching machine is given as T= 200 + 30sinθ, where θ is a crank angle. A flywheel with 15 kg.m2 moment of inertia is attached. If power is supplied at a uniform rate, what is the maximum acceleration of flywheel possible (rad/s2)?
    Solution

    Concept:

    Tmax = Iαmax

    Calculation:

    T = 200 + 30 sin θ

    \({T_{mean}} = \frac{1}{{2\pi }}\mathop \smallint \nolimits_0^{2\pi } \left( {200 + 30\sin \theta } \right)d\theta \)

    \({T_{mean}} = \frac{1}{{2\pi }}\left[ {200\;\theta + 30\;\left( { - \cos \theta } \right)} \right]_0^{2\pi }\)

    Tmean = 200 N.m

    Now,

    Tflywheel = T - Tmean

    Tflywheel = 200 + 30 sin θ – 200

    Tflywheel = 30 sin θ

    We know that, maximum value of sin θ = 1

    ∴ Tmax = Tflywheel = 30 N.m

    Tmax = Iαmax

    \(\therefore {\alpha _{max}} = \frac{{30}}{{15}}\)

    αmax = 2 rad/s

  • Question 6
    1 / -0

    A steam engine develops 300 kW power at 9.5 rad/s. The coefficient of fluctuation of energy is found to be 0.1 and fluctuation of speed is kept within ± 0.5% of mean speed. Find the mass of the flywheel (in kg) required if the radius of gyration is 2 m.

    Solution

    Concept:

    Coefficient of fluctuation of energy:

    \({C_E} = \frac{{Maximum\;Fluctuation\;of\;energy}}{{Work\;done\;per\;cycle}}\)

    Work done per cycle:

    W = Tmean × θ

    \({T_{mean}} = \frac{{P \times 60}}{{2\pi N}} = \frac{P}{\omega }\)

    Work done per cycle:

    \(W = \frac{{P \times 60}}{n}\)

    θ = 2π (in case of steam engine and two stroke IC engine)

    θ = 4π (in case of four stroke IC engine)

    Coefficient of fluctuation of speed:

    \({C_s} = \frac{{{\omega _{max}} - {\omega _{min}}}}{{{\omega _{mean}}}} = \frac{{2\left( {{\omega _1} - {\omega _2}} \right)}}{{{\omega _1} + {\omega _2}}}\)

    Mean kinetic energy of flywheel:

    \(E = \frac{1}{2}I{\omega ^2} = \frac{1}{2}m{k^2}{\omega ^2}\)

    As the speed of the flywheel changes from ω1 to ω2, the maximum fluctuation of energy:

    ΔE = 2ECs

    Calculation:

    \({C_s} = \frac{{1.005\;\omega - 0.995\;\omega }}{\omega } = 0.01\)

    \(W = \frac{{P \times 60}}{N} = \frac{P}{\omega } \times 2\pi \)

    \(W = \frac{{300}}{{9.5}} \times 2\pi = 198.42\;kN.m\)

    The maximum fluctuation of energy:

    ΔE = W × CE = 198.42 × 0.1 = 19.84 kN.m

    ΔE = 2ECs = mk2ω2Cs

    \(m = \frac{{{\rm{\Delta }}E}}{{{k^2}{\omega ^2}{C_s}}} = \frac{{19.84 \times {{10}^3}}}{{{{\left( 2 \right)}^2} \times {{\left( {9.5} \right)}^2} \times 0.01}}\)

    ∴ m = 5495.84 kg

  • Question 7
    1 / -0

    In a cam design, the rise motion is given by a simple harmonic motion (SHM) 

    \(s = \frac{h}{2}\left( {1 - cos\frac{{\pi \theta }}{\beta }} \right)\). Where, h is total rise, θ is camshaft angle, β is the total angle of the rise interval.

    For, h = 20 mm, speed = 300 rpm and β = 60˚, the maximum velocity (m/s) is given as ____
    Solution

    Concept:

    \(V = \omega \frac{{ds}}{{d\theta }}\)

    Calculation:

    Given: h = 20 mm, speed = 300 rpm and β = 60˚

    Now,

    \(s = \frac{h}{2}\left( {1 - \cos \frac{{\pi \theta }}{\beta }\;} \right)\)

    \(\therefore \frac{{ds}}{{d\theta }} = \frac{h}{2}(0 + \sin \frac{{\pi \theta }}{\beta })\frac{\pi }{\beta }\)

    \(\frac{{ds}}{{d\theta }} \Rightarrow \max ,{\rm{\;}}\;when{\rm{\;sin}}\frac{{\pi \theta }}{\beta } = 1\)

    \(\therefore {\left( {\frac{{ds}}{{d\theta }}} \right)_{max}} = \frac{{h\pi }}{{2\beta }}\)

    h = 20 mm = 0.02 m

    \(\omega = \frac{{2\pi \times 300}}{{60}} = 31.41\;rad/s\)

    \(\beta = 60^\circ = \frac{\pi }{3}\)

    \({V_{max}} = \frac{{0.02 \times 31.41 \times \pi }}{{2 \times \left( {\frac{\pi }{3}} \right)}}\)

    Vmax = 0.9423 m/s

  • Question 8
    1 / -0
    The cross-section of a flywheel is square and the rim has a mean radius of 0.50 m. The density of flywheel is 7000 kg/m3 and it is employed in a punching press which runs at 240 rpm. During punching operation which lasts one-quarter of a revolution energy requirement from flywheel is 3 kJ. If the coefficient of speed fluctuation is 0.18 and the rim contributes 85% of total moment of inertia then the cross section of the flywheel is _________×  10-3 m2.
    Solution

    Concept:

    The energy required by flywheel is \(\Delta E\)

    Contribution of rim to Moment Of Inertia = k

    Coefficient of speed fluctuation = Cs

    \({\rm{Angular\;velocity\;}}\left( {\rm{\omega }} \right){\rm{\;}} = \frac{{2\pi N}}{{60}}\;rad/s\)

    \(\therefore k\Delta E = I{\omega ^2}{C_s}\)

    Where, I = moment of inertia = mass × (mean radius)2

    Calculation:

    ΔE = 3000 J

    Contribution of rim, k = 85%

    k = 0.85, Cs = 0.18, N= 240 rpm, density (ρ) = 7000 kg/m2

    \(\omega = \frac{{2\pi N}}{{60}} = 8\pi \;rad/s\)

    kΔE = Iω2 Cs  

    \(I = \frac{{0.85\; × \; 3000}}{{64{\pi ^2}\; × \; 0.18}}\)

    I = 22.427 kg.m2

    \(m = \frac{I}{{{R^2}}} = \frac{{22.427}}{{0.25}}\)

    m = 89.711 kg

    Mass, m = (2πR) × bt × ρ (∵ mass = denity × volume)

    where bt = cross-sectional area

    \(bt = \frac{{89.711}}{{2\pi\; × \;0.5\; × \;7000}}\)

    bt = 4.079 × 10-3 m2

  • Question 9
    1 / -0
    In a spring controlled governor, controlling force varies linearly with radius of rotation. When controlling force is 1500 N, radius of rotation is 200 mm and when controlling force is 800 N, radius of rotation is 120 mm. By changing initial tension governor behaves as isochronous governor. What is the value of change in tension and isochronous speed? (mass of balls = 8 kg)
    Solution

    Explanation:

    F = ar + b, a and b are constants

    1500 = 200 a + b

    800 = 120 a + b

    Solving, we get

    a = 8.75 N/mm, b = -250 N

    for isochronous governor, b = 0

    ∴ F = ar

    F = mr ω2 = ar

    2 = a

    \(\omega = \sqrt {\frac{a}{m}} \)

    \(\omega = \sqrt {\frac{{8.75 \times 1000\left( {N/m} \right)}}{8}} \)

    ω = 33.07 rad/s

    \(N = \frac{{\omega \times 60}}{{2\pi }}\)

    N = 315.8 rpm ≈ 316 rpm

    Now,

    Change in tension = 0 – (-250)

    Change in tension = 250 N

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