Whan an elastic string of natural length 2m is fixed at one end and hangs vertically supporting a particle of mass 4Kg at the other end. It stretches to a length of 2.8m. A horizontal force of 28N is applied gradually to the mass until it is once again in equilibrium. Calculated the length and the inclination to the vertical of the string. If possible with a diagram.

Physics

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Answer

35.5∘35.5^\circ

2.983 m2.983 \text{ m}

Step-by-step solution

4 steps
  1. Calculate the spring constant (kk) of the elastic string.

    Given:
    Natural length L0=2 mL_0 = 2 \text{ m}
    Stretched length L1=2.8 mL_1 = 2.8 \text{ m}
    Mass m=4 kgm = 4 \text{ kg}
    Acceleration due to gravity g=9.8 m/s2g = 9.8 \text{ m/s}^2

    First, calculate the initial extension (x1x_1):

    x1=L1−L0=2.8 m−2 m=0.8 mx_1 = L_1 - L_0 = 2.8 \text{ m} - 2 \text{ m} = 0.8 \text{ m}

    Next, calculate the weight (WW) of the particle:

    W=mg=4 kg×9.8 m/s2=39.2 NW = mg = 4 \text{ kg} \times 9.8 \text{ m/s}^2 = 39.2 \text{ N}

    According to Hooke's Law, the tension in the string (which is equal to the weight in this vertical setup) is T=kxT = kx.
    So, W=kx1W = kx_1:

    k=Wx1=39.2 N0.8 m=49 N/mk = \frac{W}{x_1} = \frac{39.2 \text{ N}}{0.8 \text{ m}} = 49 \text{ N/m}
  2. Analyze the forces when the horizontal force is applied.

    When the horizontal force FH=28 NF_H = 28 \text{ N} is applied, the particle is in equilibrium under three forces:

    1. The weight W=39.2 NW = 39.2 \text{ N} acting vertically downwards.
    2. The horizontal force FH=28 NF_H = 28 \text{ N} acting horizontally.
    3. The tension TT in the string, acting along the string at an angle θ\theta to the vertical.

    Let x2x_2 be the new extension of the string and L2L_2 be the new stretched length.
    The tension in the string is T=kx2=49x2T = kx_2 = 49x_2.

    We resolve the forces into horizontal and vertical components.
    For vertical equilibrium:

    Tcos⁡θ=WT \cos \theta = W 49x2cos⁡θ=39.2(∗)49x_2 \cos \theta = 39.2 \quad (*)

    For horizontal equilibrium:

    Tsin⁡θ=FHT \sin \theta = F_H 49x2sin⁡θ=28(∗∗)49x_2 \sin \theta = 28 \quad (**)
  3. Calculate the inclination to the vertical (θ\theta).

    Divide equation (∗∗)(**) by equation (∗)(*):

    49x2sin⁡θ49x2cos⁡θ=2839.2\frac{49x_2 \sin \theta}{49x_2 \cos \theta} = \frac{28}{39.2} tan⁡θ=2839.2\tan \theta = \frac{28}{39.2} tan⁡θ=280392=57\tan \theta = \frac{280}{392} = \frac{5}{7} θ=arctan⁡(57)\theta = \arctan\left(\frac{5}{7}\right) θ≈35.537∘\theta \approx 35.537^\circ

    The inclination to the vertical of the string is 35.5∘\boxed{35.5^\circ}.

  4. Calculate the new length of the string (L2L_2).

    From tan⁡θ=57\tan \theta = \frac{5}{7}, we can construct a right-angled triangle with opposite side 5 and adjacent side 7. The hypotenuse is 52+72=25+49=74\sqrt{5^2 + 7^2} = \sqrt{25 + 49} = \sqrt{74}.
    So, cos⁡θ=774\cos \theta = \frac{7}{\sqrt{74}}.

    Substitute this value into equation (∗)(*):

    49x2(774)=39.249x_2 \left(\frac{7}{\sqrt{74}}\right) = 39.2 x2=39.27449×7x_2 = \frac{39.2 \sqrt{74}}{49 \times 7} x2=39.274343x_2 = \frac{39.2 \sqrt{74}}{343} x2≈39.2×8.6023343≈0.9831 mx_2 \approx \frac{39.2 \times 8.6023}{343} \approx 0.9831 \text{ m}

    The new stretched length L2L_2 is the natural length plus the extension:

    L2=L0+x2L_2 = L_0 + x_2 L2=2 m+0.9831 mL_2 = 2 \text{ m} + 0.9831 \text{ m} L2=2.9831 mL_2 = 2.9831 \text{ m}

    The length of the string is 2.983 m\boxed{2.983 \text{ m}}.

    Diagram:
    A diagram illustrating the forces and the inclination:

          Fixed point
              |
              |
              |  Tension (T)
              | /
              |/  θ (angle to vertical)
              O----- F_H (Horizontal force)
              |
              |
              | W (Weight)
              |
            Particle
    
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