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A 2 kg block attached to a spring with spring constant 8 N/m is displaced 2 m from equilibrium and released. What is the time it takes to reach 1 m from equilibrium?

Physics

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Step-by-step solution

9 steps
  1. Calculate the angular frequency ω\omega.

    The angular frequency for a mass-spring system is given by the formula:

    ω=km\omega = \sqrt{\frac{k}{m}}

    Given m=2 kgm = 2 \text{ kg} and k=8 N/mk = 8 \text{ N/m}:

    ω=8 N/m2 kg=4 rad2/s2=2 rad/s\omega = \sqrt{\frac{8 \text{ N/m}}{2 \text{ kg}}} = \sqrt{4 \text{ rad}^2/\text{s}^2} = 2 \text{ rad/s}
  2. Use the equation of motion for simple harmonic motion (SHM).

    Assuming the block is released from its maximum displacement A=2 mA = 2 \text{ m} at t=0t=0, the position x(t)x(t) is given by:

    x(t)=Acos⁡(ωt)x(t) = A \cos(\omega t)

    We want to find the time tt when x=1 mx = 1 \text{ m}.

    1 m=(2 m)cos⁡((2 rad/s)t)1 \text{ m} = (2 \text{ m}) \cos((2 \text{ rad/s}) t) 12=cos⁡((2 rad/s)t)\frac{1}{2} = \cos((2 \text{ rad/s}) t)
  3. Solve for tt.

    Take the inverse cosine of both sides:

    arccos⁡(12)=(2 rad/s)t\arccos\left(\frac{1}{2}\right) = (2 \text{ rad/s}) t

    We know that arccos⁡(12)=π3 rad\arccos\left(\frac{1}{2}\right) = \frac{\pi}{3} \text{ rad}.

    π3 rad=(2 rad/s)t\frac{\pi}{3} \text{ rad} = (2 \text{ rad/s}) t t=π/3 rad2 rad/s=π6 st = \frac{\pi/3 \text{ rad}}{2 \text{ rad/s}} = \frac{\pi}{6} \text{ s} t≈3.141596 s≈0.5236 st \approx \frac{3.14159}{6} \text{ s} \approx 0.5236 \text{ s}

    None of the options (A. 40 sec B. 60 sec C. 30 sec D. 20 sec) match this result. There might be an issue with the question's options or interpretation. However, based on the standard SHM model, this is the time taken. If the question implies traveling to x=1x=1 from x=2x=2 and then back to x=1x=1 or some other interpretation, it's not explicitly stated. Assuming the simplest interpretation of starting at x=2x=2 and moving towards x=0x=0.

    The final answer is 0.52 s\boxed{\text{0.52 s}}.

  4. Identify the given frequency.

    The frequency of the simple pendulum is f=1.5 Hzf = 1.5 \text{ Hz}.

  5. Calculate the angular frequency.

    The relationship between angular frequency ω\omega and frequency ff is:

    ω=2πf\omega = 2\pi f

    Substitute the given frequency:

    ω=2π(1.5 Hz)=3.0π rad/s\omega = 2\pi (1.5 \text{ Hz}) = 3.0\pi \text{ rad/s}

    The final answer is B. 3.0π\boxed{\text{B. } 3.0\pi}.

    Damping of periodic motion always results in a decrease in the amplitude of the oscillations over time due to energy dissipation.

    The final answer is B. decreasing amplitude\boxed{\text{B. decreasing amplitude}}.

  6. Calculate the total mass of the car and passengers.

    Total mass M=mcar+mpassengersM = m_{car} + m_{passengers}

    M=1300 kg+160 kg=1460 kgM = 1300 \text{ kg} + 160 \text{ kg} = 1460 \text{ kg}
  7. Calculate the total effective spring constant.

    Since there are four springs supporting the car, and they are in parallel, the total effective spring constant ktotalk_{total} is the sum of the individual spring constants.

    ktotal=4×kspringk_{total} = 4 \times k_{spring} ktotal=4×20,000 N/m=80,000 N/mk_{total} = 4 \times 20,000 \text{ N/m} = 80,000 \text{ N/m}
  8. Calculate the angular frequency ω\omega.

    The angular frequency for a mass-spring system is given by:

    ω=ktotalM\omega = \sqrt{\frac{k_{total}}{M}} ω=80,000 N/m1460 kg=54.7945 rad2/s2≈7.4023 rad/s\omega = \sqrt{\frac{80,000 \text{ N/m}}{1460 \text{ kg}}} = \sqrt{54.7945 \text{ rad}^2/\text{s}^2} \approx 7.4023 \text{ rad/s}
  9. Calculate the frequency ff.

    The frequency ff is related to the angular frequency ω\omega by:

    f=ω2πf = \frac{\omega}{2\pi} f=7.4023 rad/s2π≈7.40236.28318 Hz≈1.178 Hzf = \frac{7.4023 \text{ rad/s}}{2\pi} \approx \frac{7.4023}{6.28318} \text{ Hz} \approx 1.178 \text{ Hz}

    Comparing this to the given options:
    A. 2.31 Hz2.31 \text{ Hz}
    B. 1.42 Hz1.42 \text{ Hz}
    C. 5.36 Hz5.36 \text{ Hz}
    D. 1.18 Hz1.18 \text{ Hz}

    The calculated frequency is approximately 1.18 Hz1.18 \text{ Hz}.

    The final answer is D. 1.18 Hz\boxed{\text{D. } 1.18 \text{ Hz}}.

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