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5.1 State the principle of conservation of mechanical energy in words.

Physics

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Answer

36.13∘\text{36.13}^\circ

90.35 W\text{90.35 W}

Step-by-step solution

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5.1 State the principle of conservation of mechanical energy in words.

The principle of conservation of mechanical energy states that the total mechanical energy (sum of kinetic and potential energy) of an isolated system remains constant if only conservative forces do work on the objects within the system.

5.2 Is the mechanical energy of the object CONSERVED or NOT CONSERVED while the object is moving from point P to point Q along the horizontal surface? Give a reason for the answer.

NOT CONSERVED.
This is because a non-conservative force (friction) does work on the object as it moves from P to Q.

5.3 Calculate the:

5.3.1 Magnitude of the angle θ\theta, shown in the diagram above, using energy principles ONLY.

  1. Identify the initial and final states and the forces doing work.

    Initial state (P): vP=0v_P = 0 m/s, hP=0h_P = 0 m.
    Final state (R): vR=0v_R = 0 m/s, hR=40h_R = 40 cm =0.4= 0.4 m.
    Forces doing work from P to R: applied force FF, frictional force fkf_k, and gravitational force FgF_g.

  2. Apply the Work-Energy Theorem from point P to point R.

    The Work-Energy Theorem states that the net work done on an object equals its change in kinetic energy: Wnet=ΔKW_{net} = \Delta K.
    Since the object starts from rest at P and stops at R, ΔK=KR−KP=0−0=0\Delta K = K_R - K_P = 0 - 0 = 0.
    Therefore, Wnet=0W_{net} = 0.

    The net work is the sum of the work done by all forces:

    Wnet=WF+Wfriction+WgW_{net} = W_F + W_{friction} + W_g WF=FΔxcos⁡θW_F = F \Delta x \cos \theta Wfriction=fkΔxcos⁡180∘=−fkΔxW_{friction} = f_k \Delta x \cos 180^\circ = -f_k \Delta x Wg=−mghRW_g = -mgh_R

    Note: The applied force FF and frictional force fkf_k only act from P to Q. The gravitational force FgF_g does work over the vertical displacement from Q to R.

  3. Substitute the known values into the Work-Energy Theorem equation.

    Given:
    F=80F = 80 N
    Δx=4\Delta x = 4 m (distance from P to Q)
    fk=45f_k = 45 N
    m=20m = 20 kg
    g=9.8g = 9.8 m/s2^2
    hR=0.4h_R = 0.4 m

    FΔxcos⁡θ−fkΔx−mghR=0F \Delta x \cos \theta - f_k \Delta x - mgh_R = 0 (80 N)(4 m)cos⁡θ−(45 N)(4 m)−(20 kg)(9.8 m/s2)(0.4 m)=0(80 \text{ N})(4 \text{ m}) \cos \theta - (45 \text{ N})(4 \text{ m}) - (20 \text{ kg})(9.8 \text{ m/s}^2)(0.4 \text{ m}) = 0 320cos⁡θ−180−78.4=0320 \cos \theta - 180 - 78.4 = 0 320cos⁡θ−258.4=0320 \cos \theta - 258.4 = 0 320cos⁡θ=258.4320 \cos \theta = 258.4 cos⁡θ=258.4320\cos \theta = \frac{258.4}{320} cos⁡θ=0.8075\cos \theta = 0.8075 θ=arccos⁡(0.8075)\theta = \arccos(0.8075) θ≈36.13∘\theta \approx 36.13^\circ

    The magnitude of the angle θ\theta is 36.13∘\boxed{\text{36.13}^\circ}.

    5.3.2 Power delivered by force F if the time taken for the object to move from point P to point Q is 2.86 seconds.

  4. Calculate the work done by force F from P to Q.

    WF=FΔxcos⁡θW_F = F \Delta x \cos \theta

    Using the value of θ\theta from 5.3.1:

    WF=(80 N)(4 m)cos⁡(36.13∘)W_F = (80 \text{ N})(4 \text{ m}) \cos(36.13^\circ) WF=320cos⁡(36.13∘)W_F = 320 \cos(36.13^\circ) WF=320×0.8075W_F = 320 \times 0.8075 WF=258.4 JW_F = 258.4 \text{ J}
  5. Calculate the power delivered by force F.

    Power PP is defined as the rate at which work is done:

    P=WFtP = \frac{W_F}{t}

    Given t=2.86t = 2.86 s:

    P=258.4 J2.86 sP = \frac{258.4 \text{ J}}{2.86 \text{ s}} P≈90.35 WP \approx 90.35 \text{ W}

    The power delivered by force F is 90.35 W\boxed{\text{90.35 W}}.

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