Forces and Free-Body Diagrams
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AP Physics C: Mechanics › Forces and Free-Body Diagrams
A $12.0,\text{kg}$ box is pulled up a $30^\circ$ incline at constant speed by a rope parallel to the plane; $\mu_k=0.15$. Consider the scenario described above, with kinetic friction opposing the motion and $g=9.8,\text{m/s}^2$. The normal force is perpendicular to the incline and weight is vertical. No air resistance acts. Calculate the frictional force given the conditions.
$14.7,\text{N}$ down the plane
$15.3,\text{N}$ down the plane
$17.6,\text{N}$ down the plane
$18,\text{N}$ down the plane
$15.3,\text{N}$ up the plane
Explanation
This question tests AP Physics C: Mechanics skills, specifically understanding forces and free-body diagrams. Free-body diagrams help visualize all forces acting on an object, including weight, normal force, friction, and applied forces, which is essential for analyzing motion on inclined planes. In this scenario, a 12.0 kg box moves up a 30° incline at constant speed, meaning the net force is zero and all forces balance. The problem asks specifically for the frictional force, which opposes motion (pointing down the plane). Choice B is correct because the normal force equals mg cos(30°) = 101.8 N, and the kinetic friction force equals μₖN = 0.15 × 101.8 = 15.3 N down the plane. Choice A is incorrect because it has the right magnitude but wrong direction - friction must oppose motion, so it points down the plane, not up. To help students: Emphasize that friction always opposes relative motion between surfaces, and at constant velocity, the net force must be zero. Practice identifying the direction of friction based on the direction of motion or impending motion. Watch for: students confusing the direction of friction, mixing up static and kinetic friction, or forgetting that constant speed means zero acceleration.
Two masses $m_1=2.0,\text{kg}$ and $m_2=2.5,\text{kg}$ are connected by a light rope over a frictionless pulley. Consider the scenario described above, with $m_2$ moving downward and the system accelerating. Take $g=9.8,\text{m/s}^2$ and assume the rope is massless. Tension is the same on both sides. Determine the tension in the rope.
$21.8,\text{N}$
$19.6,\text{N}$
$22.1,\text{N}$
$4.9,\text{N}$
$24.5,\text{N}$
Explanation
This question tests AP Physics C: Mechanics skills, specifically understanding forces and free-body diagrams. Free-body diagrams for Atwood machines show that tension is the same throughout a massless rope, and both masses experience the same magnitude of acceleration in opposite directions. In this scenario, masses of 2.0 kg and 2.5 kg are connected over a frictionless pulley, with the heavier mass accelerating downward. Choice D is correct because the system acceleration is a = (m₂ - m₁)g/(m₁ + m₂) = (0.5)(9.8)/4.5 = 1.09 m/s², and the tension T = m₁(g + a) = 2.0(9.8 + 1.09) = 21.8 N, which also equals m₂(g - a) as a check. Choice E is incorrect because it represents the weight of the lighter mass (19.6 N), showing the common error of assuming tension equals weight when the system accelerates. To help students: Set up separate free-body diagrams and equations for each mass, use the constraint that both accelerations have the same magnitude, and solve the system of equations. Verify the answer by checking that the same tension satisfies both force equations. Watch for: students assuming tension equals one of the weights, using different accelerations for each mass, or making sign errors in the force equations.
Two masses $m_1=4.0,\text{kg}$ and $m_2=6.0,\text{kg}$ hang on either side of a light rope over a frictionless pulley. Consider the scenario described above, with $m_2$ accelerating downward and the rope remaining taut. Take $g=9.8,\text{m/s}^2$ and neglect pulley mass. Tension is uniform throughout the rope. Determine the tension in the rope.
$78.4,\text{N}$
$47.0,\text{N}$
$58.8,\text{N}$
$23.5,\text{N}$
$39.2,\text{N}$
Explanation
This question tests AP Physics C: Mechanics skills, specifically understanding forces and free-body diagrams. Free-body diagrams for connected objects must show tension forces that obey Newton's third law, with the rope providing equal tension on both masses in an Atwood machine setup. In this scenario, masses of 4.0 kg and 6.0 kg hang on either side of a frictionless pulley, with the heavier mass accelerating downward. Choice A is correct because applying Newton's second law to the system: the net force is (m₂ - m₁)g = 19.6 N, giving acceleration a = 19.6/10 = 1.96 m/s², and the tension T = m₁(g + a) = 4.0(9.8 + 1.96) = 47.0 N. Choice B is incorrect because it represents the weight of the lighter mass (39.2 N), which students often confuse with tension when they don't account for the acceleration of the system. To help students: Draw separate free-body diagrams for each mass, write Newton's second law equations for each object, and solve the system of equations simultaneously. Emphasize that tension is not simply equal to the weight of either mass when the system accelerates. Watch for: students assuming tension equals weight, forgetting to use the same acceleration for both masses, or incorrectly setting up the force equations.
A $2.0,\text{kg}$ block rests on a $40^\circ$ incline with $\mu_s=0.50$ and no applied force. Consider the scenario described above, with the block initially at rest and $g=9.8,\text{m/s}^2$. Static friction acts along the plane as needed, up to $\mu_s N$. The normal force is perpendicular to the plane and weight is vertical. Is the object in equilibrium? Justify your answer.
Yes; $mg\sin\theta < \mu_s mg\cos\theta$
Yes; friction points down the plane here
No; static friction is always $\mu_s N$
Yes; $N=mg\sin\theta$ guarantees rest
No; $mg\sin\theta > \mu_s mg\cos\theta$
Explanation
This question tests AP Physics C: Mechanics skills, specifically understanding forces and free-body diagrams. Free-body diagrams on inclined planes require careful analysis of static friction, which can vary from zero up to μₛN depending on what's needed to prevent motion. In this scenario, a 2.0 kg block rests on a 40° incline with static friction coefficient 0.50, and we must determine if it remains in equilibrium. Choice B is correct because the component of weight down the plane is mg sin(40°) = 12.6 N, while the maximum static friction is μₛmg cos(40°) = 0.50(2.0)(9.8)cos(40°) = 7.5 N; since 12.6 N > 7.5 N, static friction cannot balance the weight component, so the block will slide. Choice A is incorrect because it reverses the inequality - students often confuse when to use sine versus cosine or compare the forces incorrectly. To help students: Teach the critical angle concept where tan(θ) = μₛ determines the steepest angle for equilibrium, and practice comparing the weight component down the plane with maximum static friction. Emphasize that static friction adjusts to match the applied force up to its maximum value. Watch for: students always using μₛN for static friction instead of recognizing it as a maximum, confusing the conditions for static equilibrium, or mixing up force components.