Calculate the average angular acceleration and number of revolutions turned through in this time.

Physics

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2. Calculate the average angular acceleration and number of revolutions turned through in this time.

  • Initial angular velocity (ω0\omega_0): 1430 rev/min1430 \text{ rev/min}
  • Final angular velocity (ωf\omega_f): 1490 rev/min1490 \text{ rev/min}
  • Time interval (Δt\Delta t): 0.5 s0.5 \text{ s}
  1. Convert the initial and final angular velocities from revolutions per minute (rev/min) to radians per second (rad/s).

    We use the conversion factor: 1 rev/min=2π rad60 s=π30 rad/s1 \text{ rev/min} = \frac{2\pi \text{ rad}}{60 \text{ s}} = \frac{\pi}{30} \text{ rad/s}.

    ω0=1430 rev/min×π rad/s30 rev/min=143π3 rad/s\omega_0 = 1430 \text{ rev/min} \times \frac{\pi \text{ rad/s}}{30 \text{ rev/min}} = \frac{143\pi}{3} \text{ rad/s} ωf=1490 rev/min×π rad/s30 rev/min=149π3 rad/s\omega_f = 1490 \text{ rev/min} \times \frac{\pi \text{ rad/s}}{30 \text{ rev/min}} = \frac{149\pi}{3} \text{ rad/s}
  2. Calculate the average angular acceleration (αavg\alpha_{avg}).

    The formula for average angular acceleration is αavg=ωf−ω0Δt\alpha_{avg} = \frac{\omega_f - \omega_0}{\Delta t}.

    αavg=149π3 rad/s−143π3 rad/s0.5 s\alpha_{avg} = \frac{\frac{149\pi}{3} \text{ rad/s} - \frac{143\pi}{3} \text{ rad/s}}{0.5 \text{ s}} αavg=(149−143)π3 rad/s0.5 s\alpha_{avg} = \frac{\frac{(149-143)\pi}{3} \text{ rad/s}}{0.5 \text{ s}} αavg=6π3 rad/s0.5 s=2π rad/s0.5 s\alpha_{avg} = \frac{\frac{6\pi}{3} \text{ rad/s}}{0.5 \text{ s}} = \frac{2\pi \text{ rad/s}}{0.5 \text{ s}} αavg=4π rad/s2≈12.57 rad/s2\alpha_{avg} = 4\pi \text{ rad/s}^2 \approx 12.57 \text{ rad/s}^2

    The average angular acceleration is 4π rad/s2\boxed{4\pi \text{ rad/s}^2} or approximately 12.57 rad/s2\boxed{12.57 \text{ rad/s}^2}.

  3. Calculate the angular displacement (Δθ\Delta \theta) in radians.

    For uniform angular acceleration, the angular displacement can be found using Δθ=(ω0+ωf)2Δt\Delta \theta = \frac{(\omega_0 + \omega_f)}{2} \Delta t.

    Δθ=(143π3 rad/s+149π3 rad/s)2×0.5 s\Delta \theta = \frac{\left(\frac{143\pi}{3} \text{ rad/s} + \frac{149\pi}{3} \text{ rad/s}\right)}{2} \times 0.5 \text{ s} Δθ=(292π3 rad/s)2×0.5 s\Delta \theta = \frac{\left(\frac{292\pi}{3} \text{ rad/s}\right)}{2} \times 0.5 \text{ s} Δθ=146π3 rad/s×0.5 s\Delta \theta = \frac{146\pi}{3} \text{ rad/s} \times 0.5 \text{ s} Δθ=73π3 rad≈76.45 rad\Delta \theta = \frac{73\pi}{3} \text{ rad} \approx 76.45 \text{ rad}
  4. Convert the angular displacement from radians to revolutions.

    We use the conversion factor: 1 revolution=2π radians1 \text{ revolution} = 2\pi \text{ radians}.

    Number of revolutions=Δθ2π\text{Number of revolutions} = \frac{\Delta \theta}{2\pi} Number of revolutions=73π3 rad2π rad/rev\text{Number of revolutions} = \frac{\frac{73\pi}{3} \text{ rad}}{2\pi \text{ rad/rev}} Number of revolutions=736 revolutions≈12.17 revolutions\text{Number of revolutions} = \frac{73}{6} \text{ revolutions} \approx 12.17 \text{ revolutions}

    The number of revolutions turned through is 736 revolutions\boxed{\frac{73}{6} \text{ revolutions}} or approximately 12.17 revolutions\boxed{12.17 \text{ revolutions}}.

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