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State the work-energy theorem in words and apply it to calculate the kinetic energy of a crate. Also, draw a free-body diagram for the crate on an incline.

Physics

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2 parts
5.2

84 J\text{84 J}

5.4

pass point C\text{pass point C}

Step-by-step solution

4 steps

Here is the solution to your problem:

Part 5.1

State the work-energy theorem in words.

The work-energy theorem states that the net work done on an object is equal to the change in its kinetic energy.

Part 5.2

84 J\text{84 J}

Using ENERGY PRINCIPLES ONLY, calculate the kinetic energy of the crate at point B.

The crate starts at rest at point A, so its initial kinetic energy KA=0 JK_A = 0 \text{ J}.
A constant horizontal force F=12 NF = 12 \text{ N} acts on the crate over a distance dAB=7 md_{AB} = 7 \text{ m}.
The surface from A to B is frictionless.
The work done by the force FF is given by:

WF=F⋅dABW_F = F \cdot d_{AB}

According to the work-energy theorem, the net work done on the crate is equal to the change in its kinetic energy:

Wnet=ΔK=KB−KAW_{net} = \Delta K = K_B - K_A

Since KA=0 JK_A = 0 \text{ J} and the only force doing work is FF:

KB=WFK_B = W_F KB=(12 N)(7 m)K_B = (12 \text{ N})(7 \text{ m}) KB=84 JK_B = 84 \text{ J}

The kinetic energy of the crate at point B is 84 J\boxed{\text{84 J}}.

Part 5.3

Draw a free-body diagram showing ALL the forces acting on the crate as it moves down the incline.

As the crate moves down the incline, the forces acting on it are:

  • Gravitational force (Weight): Acts vertically downwards from the center of mass of the crate.
  • Normal force: Acts perpendicular to the inclined surface, pointing away from the surface.
  • Kinetic frictional force: Acts parallel to the inclined surface, pointing upwards along the incline (opposite to the direction of motion).

Part 5.4

pass point C\text{pass point C}

Using ENERGY PRINCIPLES ONLY, determine whether the crate will pass point C.

From point B to C, the crate moves down an incline.
Initial kinetic energy at B: KB=84 JK_B = 84 \text{ J}
Mass of the crate: m=3 kgm = 3 \text{ kg}
Distance from B to C: dBC=6.8 md_{BC} = 6.8 \text{ m}
Angle of inclination: θ=20∘\theta = 20^\circ
Constant frictional force: fk=21 Nf_k = 21 \text{ N}
Acceleration due to gravity: g=9.8 m/s2g = 9.8 \text{ m/s}^2

We use the work-energy theorem from B to C: Wnet,BC=KC−KBW_{net, BC} = K_C - K_B.
The forces doing work are gravity and friction.

  1. Calculate the work done by gravity (WgW_g).

    The component of gravity parallel to the incline is mgsin⁡θmg \sin\theta. This component acts in the direction of motion.

    Wg=(mgsin⁡θ)dBCW_g = (mg \sin\theta) d_{BC} Wg=(3 kg)(9.8 m/s2)sin⁡(20∘)(6.8 m)W_g = (3 \text{ kg})(9.8 \text{ m/s}^2) \sin(20^\circ) (6.8 \text{ m}) Wg=(29.4 N)(0.3420)(6.8 m)W_g = (29.4 \text{ N})(0.3420)(6.8 \text{ m}) Wg≈68.45 JW_g \approx 68.45 \text{ J}
  2. Calculate the work done by friction (WfW_f).

    Friction opposes the motion, so the work done by friction is negative.

    Wf=−fk⋅dBCW_f = -f_k \cdot d_{BC} Wf=−(21 N)(6.8 m)W_f = -(21 \text{ N})(6.8 \text{ m}) Wf=−142.8 JW_f = -142.8 \text{ J}
  3. Calculate the net work done from B to C (Wnet,BCW_{net, BC}).

    Wnet,BC=Wg+WfW_{net, BC} = W_g + W_f Wnet,BC=68.45 J−142.8 JW_{net, BC} = 68.45 \text{ J} - 142.8 \text{ J} Wnet,BC=−74.35 JW_{net, BC} = -74.35 \text{ J}
  4. Calculate the kinetic energy at C (KCK_C).

    Using the work-energy theorem:

    KC=KB+Wnet,BCK_C = K_B + W_{net, BC} KC=84 J+(−74.35 J)K_C = 84 \text{ J} + (-74.35 \text{ J}) KC=9.65 JK_C = 9.65 \text{ J}

    Since the kinetic energy at point C (KC=9.65 JK_C = 9.65 \text{ J}) is positive, the crate still has kinetic energy when it reaches point C. Therefore, the crate will pass point C.

    The crate will pass point C\boxed{\text{pass point C}}.

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