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Ch 05: Applying Newton's Laws
Chapter 5, Problem 5

Two crates connected by a rope lie on a horizontal surface (Fig. E5.37). Crate A has mass mA, and crate B has mass mB. The coefficient of kinetic friction between each crate and the surface is μk. The crates are pulled to the right at constant velocity by a horizontal force F Draw one or more free-body diagrams to calculate the following in terms of mA, mB, and μk: (b) the tension in the rope connecting the blocks. Diagram showing two crates P and Q connected by a rope, with a force F pulling them to the right.

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Draw the free-body diagrams for both crates A and B. Identify all the forces acting on each crate: the applied force F, the tension T in the rope, the frictional forces, and the normal forces.
For crate A, write the equation of motion in the horizontal direction: F - T - fA = 0, where fA is the frictional force on crate A. Since the crates are moving at constant velocity, the net force is zero.
Express the frictional force fA in terms of the coefficient of kinetic friction and the normal force: fA = μk * mA * g.
For crate B, write the equation of motion in the horizontal direction: T - fB = 0, where fB is the frictional force on crate B. Again, since the crates are moving at constant velocity, the net force is zero.
Express the frictional force fB in terms of the coefficient of kinetic friction and the normal force: fB = μk * mB * g. Solve the equations to find the tension T in the rope connecting the blocks.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Free-Body Diagram

A free-body diagram is a graphical representation used to visualize the forces acting on an object. In this scenario, each crate (A and B) will have its own free-body diagram showing the applied force, tension in the rope, and frictional forces. This helps in analyzing the forces to determine the net force and subsequently the tension in the connecting rope.
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Kinetic Friction

Kinetic friction is the force that opposes the motion of two surfaces sliding past each other. It is quantified by the equation F_friction = μk * N, where μk is the coefficient of kinetic friction and N is the normal force. In this problem, the kinetic friction acts on both crates, affecting the net force and the tension in the rope as the crates are pulled at a constant velocity.
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Newton's Second Law

Newton's Second Law states that the acceleration of an object is directly proportional to the net force acting on it and inversely proportional to its mass, expressed as F = ma. In this case, since the crates are moving at constant velocity, the net force is zero, which means the applied force must equal the total frictional force acting on both crates. This principle is essential for calculating the tension in the rope.
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Related Practice
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In a laboratory experiment on friction, a 135-N block resting on a rough horizontal table is pulled by a horizontal wire. The pull gradually increases until the block begins to move and continues to increase thereafter. Figure E5.26 shows a graph of the friction force on this block as a function of the pull. (a) Identify the regions of the graph where static friction and kinetic friction occur.

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In another version of the 'Giant Swing' (see Exercise 5.50), the seat is connected to two cables, one of which is horizontal (Fig. E5.51). The seat swings in a horizontal circle at a rate of 28.0 rpm (rev/min). If the seat weighs 255 N and an 825-N person is sitting in it, find the tension in each cable.

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