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A force f = (4−v²) N is acting on a particle of mass 3kg where v is velocity in ms⁻¹ of the particle. Initially, the particle is at rest at the origin. Find, i. The time taken for the particle to reach a velocity of 0.5 ms⁻¹ ii. The displacement when the velocity is 0.5 ms⁻¹

Physics

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2 parts
i

0.383 s0.383 \, \text{s}

ii

0.0968 m0.0968 \, \text{m}

Step-by-step solution

6 steps

Here's the solution to the problem:

Given:
Force F=(4−v2) NF = (4-v^2) \, \text{N} (assuming '4' from the handwritten text, as '2x' from OCR would make the problem significantly more complex and likely beyond the scope of this type of question)
Mass m=3 kgm = 3 \, \text{kg}
Initial velocity v0=0 m/sv_0 = 0 \, \text{m/s} (at rest)
Initial position x0=0 mx_0 = 0 \, \text{m} (at the origin)

Part i· 3 steps

The time taken for the particle to reach a velocity of 0.5 m/s0.5 \, \text{m/s}

  1. Apply Newton's Second Law (F=maF=ma) and express acceleration as dvdt\frac{dv}{dt}.

    F=mdvdtF = m \frac{dv}{dt} 4−v2=3dvdt4-v^2 = 3 \frac{dv}{dt} dvdt=4−v23\frac{dv}{dt} = \frac{4-v^2}{3}
  2. Separate variables and integrate to find time.

    dt=34−v2dvdt = \frac{3}{4-v^2} dv

    Integrate from t=0t=0 to tt and v=0v=0 to v=0.5v=0.5:

    ∫0tdt=∫00.534−v2dv\int_{0}^{t} dt = \int_{0}^{0.5} \frac{3}{4-v^2} dv t=3∫00.5122−v2dvt = 3 \int_{0}^{0.5} \frac{1}{2^2-v^2} dv

    Using the standard integral ∫1a2−x2dx=12aln⁡∣a+xa−x∣\int \frac{1}{a^2-x^2} dx = \frac{1}{2a} \ln \left| \frac{a+x}{a-x} \right|, with a=2a=2:

    t=3[12(2)ln⁡∣2+v2−v∣]00.5t = 3 \left[ \frac{1}{2(2)} \ln \left| \frac{2+v}{2-v} \right| \right]_{0}^{0.5} t=34[ln⁡(2+v2−v)]00.5t = \frac{3}{4} \left[ \ln \left( \frac{2+v}{2-v} \right) \right]_{0}^{0.5}
  3. Evaluate the definite integral.

    t=34(ln⁡(2+0.52−0.5)−ln⁡(2+02−0))t = \frac{3}{4} \left( \ln \left( \frac{2+0.5}{2-0.5} \right) - \ln \left( \frac{2+0}{2-0} \right) \right) t=34(ln⁡(2.51.5)−ln⁡(1))t = \frac{3}{4} \left( \ln \left( \frac{2.5}{1.5} \right) - \ln(1) \right) t=34ln⁡(53)t = \frac{3}{4} \ln \left( \frac{5}{3} \right) t≈34×0.5108256t \approx \frac{3}{4} \times 0.5108256 t=0.383 st = \boxed{0.383 \, \text{s}}

Part ii

0.0968 m0.0968 \, \text{m}

The displacement when the velocity is 0.5 m/s0.5 \, \text{m/s}

  1. Apply Newton's Second Law (F=maF=ma) and express acceleration as vdvdxv \frac{dv}{dx}.

    F=mvdvdxF = m v \frac{dv}{dx} 4−v2=3vdvdx4-v^2 = 3 v \frac{dv}{dx}
  2. Separate variables and integrate to find displacement.

    dx=3v4−v2dvdx = \frac{3v}{4-v^2} dv

    Integrate from x=0x=0 to xx and v=0v=0 to v=0.5v=0.5:

    ∫0xdx=∫00.53v4−v2dv\int_{0}^{x} dx = \int_{0}^{0.5} \frac{3v}{4-v^2} dv x=∫00.53v4−v2dvx = \int_{0}^{0.5} \frac{3v}{4-v^2} dv

    Use substitution: Let u=4−v2u = 4-v^2. Then du=−2v dvdu = -2v \, dv, so v dv=−12duv \, dv = -\frac{1}{2} du.
    When v=0v=0, u=4u=4. When v=0.5v=0.5, u=4−(0.5)2=3.75u=4-(0.5)^2 = 3.75.

    x=∫43.753(−121u)dux = \int_{4}^{3.75} 3 \left( -\frac{1}{2} \frac{1}{u} \right) du x=−32∫43.751udux = -\frac{3}{2} \int_{4}^{3.75} \frac{1}{u} du
  3. Evaluate the definite integral.

    x=−32[ln⁡∣u∣]43.75x = -\frac{3}{2} [\ln|u|]_{4}^{3.75} x=−32(ln⁡(3.75)−ln⁡(4))x = -\frac{3}{2} (\ln(3.75) - \ln(4)) x=−32ln⁡(3.754)x = -\frac{3}{2} \ln \left( \frac{3.75}{4} \right) x=−32ln⁡(1516)x = -\frac{3}{2} \ln \left( \frac{15}{16} \right)

    Using the logarithm property ln⁡(a/b)=−ln⁡(b/a)\ln(a/b) = -\ln(b/a):

    x=32ln⁡(1615)x = \frac{3}{2} \ln \left( \frac{16}{15} \right) x≈32×0.0645385x \approx \frac{3}{2} \times 0.0645385 x=0.0968 mx = \boxed{0.0968 \, \text{m}}

    Dernière correction gratuite aujourd'hui — reviens demain, ou tape /upgrade pour l'illimité.

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