AP Physics 1 Review Packet
AP Physics 1 • Quarter 1 Review
Mechanics & Dynamics Study Packet
Kinematics • Newton's Laws
Circular Motion • Gravitation
Student Name: ___________________
Date: ____________
Period: _______
Required AP Physics 1 Standards & Learning Objectives
Unit 1: Kinematics (AP 1.1 - 1.4)
• 1.1-1.2 Motion Graphs: Slopes (\(v = dx/dt\), \(a = dv/dt\)) and areas (\(\Delta x = \int v\,dt\), \(\Delta v = \int a\,dt\)).
• 1.3 Projectile Motion: Independence of horizontal (\(a_x=0\)) and vertical (\(a_y = -g\)) motion.
• 1.4 Relative Velocity: Vector summation of velocities across reference frames.
Unit 2: Force & Newton's Laws (AP 2.1 - 2.5)
• 2.1 Center of Mass: Acceleration of system center of mass \(a_{cm} = \Sigma F_{ext} / M_{total}\).
• 2.2-2.3 Newton's 1st & 2nd Laws: Inertial frames, \(\Sigma \vec{F} = m\vec{a}\), multi-body systems, inclines.
• 2.4-2.5 3rd Law & Friction: Action-reaction pairs; static \(f_s \le \mu_s F_N\) vs kinetic \(f_k = \mu_k F_N\).
Unit 3: Circular Motion & Gravity (AP 3.1 - 3.3)
• 3.1 Centripetal Force: Radial acceleration \(a_c = v^2/r\); physical forces providing centripetal net force.
• 3.2 Vertical Circles: Critical speed at apex (\(v_{min} = \sqrt{gr}\)) and peak tension at nadir.
• 3.3 Universal Gravitation: \(F_g = G\frac{m_1 m_2}{r^2}\); gravitational field superposition and null points.
Science Practices & FRQ Reasoning
• SP 1-2 Representations: Free-body diagrams with proportional vector lengths and correct points of origin.
• SP 3-4 Experimental Design: Independent/dependent variables, timing gates, linearization of data.
• SP 6-7 QQT & Argumentation: Qualitative-Quantitative Translation and Claim-Evidence-Reasoning.
Essential Formula Toolkit & Conventions (Use \(g = 10\text{ m/s}^2\))
1D Kinematics
\(v_x = v_{x0} + a_x t\)
\(x = x_0 + v_{x0}t + \frac{1}{2}a_x t^2\)
\(v_x^2 = v_{x0}^2 + 2a_x(x - x_0)\)
Dynamics & Inclines
\(\vec{a} = \frac{\Sigma \vec{F}_{ext}}{m_{sys}}\)
\(F_{g\parallel} = mg\sin\theta,\; F_{g\perp} = mg\cos\theta\)
\(f_{s,max} = \mu_s F_N,\; f_k = \mu_k F_N\)
Circles & Gravitation
\(a_c = \frac{v^2}{r},\; \Sigma F_r = m\frac{v^2}{r}\)
\(F_g = G\frac{m_1 m_2}{r^2}\)
\(g = G\frac{M}{r^2}\)
AP Physics 1 Problem-Solving Strategy:
- Identify the System: Internal forces (between system parts) cancel in pairs and never accelerate the center of mass.
- Free-Body Diagrams: Never draw components on formal FBDs. Draw only real contact and field forces with tail on object.
- Thinking Hints: Use the hint callouts on every practice problem below to guide your initial physics modeling!
AP Physics 1 Quarter 1 Comprehensive Packet Section 1: 20 Multiple Choice • Section 2: 10 Constructed Response
Section I: Multiple Choice • Questions 1–4 Kinematics & Graph Interpretation
1. A box carrying an active internal battery-powered robotic toy is accidentally knocked off a table of height \(h\). While in midair, the toy inside rolls, thumps against the container walls, and spins rapidly. Neglecting air resistance, what is the acceleration of the center of mass of the box-toy system while in flight?
(A) Directed downward with magnitude less than \(g\) because of internal upward impacts.
(B) Directed downward with constant magnitude equal to \(g\).
(C) Fluctuating continuously in magnitude and direction due to internal mechanical collisions.
(D) Zero, because internal forces maintain dynamic equilibrium.
Thinking Hint: Distinguish between internal forces and external forces. What is the only external force acting on the two-object system once it leaves the table? How does Newton's second law apply to \(a_{cm}\)?
2. Object 1 moves along the \(x\)-axis according to \(x_1(t) = 4t - t^2\), while Object 2 moves according to \(x_2(t) = 2t\), with \(x\) in meters and \(t\) in seconds. From \(t = 0\) to \(t = 4\text{ s}\), which statement correctly compares the total distance traveled by the two objects?
(A) Object 1 traveled a greater distance than Object 2.
(B) Object 2 traveled a greater distance than Object 1.
(C) Both objects traveled the exact same total distance.
(D) The distances cannot be compared without knowing the mass of each object.
Thinking Hint: Remember that distance is path length, not net displacement. Check if Object 1 stops and turns around (\(v_1(t) = dx_1/dt = 0\)) between \(t = 0\) and \(t = 4\text{ s}\). Sum the positive and negative segments!
3. Two runners, \(A\) and \(B\), travel along a straight track. The position-versus-time graph for Runner \(A\) is a straight line with a constant positive slope. The graph for Runner \(B\) is a parabola opening upward that intersects Runner \(A\)'s line at times \(t_1\) and \(t_2\) (\(t_2 > t_1\)). At what time do the runners have identical velocities?
(A) Exactly at time \(t_1\)
(B) At a time strictly between \(t_1\) and \(t_2\)
(C) Exactly at time \(t_2\)
(D) They never have the same velocity because Runner B is accelerating.
Thinking Hint: What graphical feature of a position-versus-time graph represents instantaneous velocity? When is the tangent slope of the curve equal to the secant slope between \(t_1\) and \(t_2\)?
4. A 5.0 kg crate is sliding to the right along a horizontal floor. The normal force on the crate is 50 N, and the coefficient of kinetic friction between crate and floor is \(\mu_k = 0.25\). No other horizontal force acts on the crate. The magnitude and direction of the crate's acceleration are:
(A) \(2.5\text{ m/s}^2\) to the left
(B) \(2.5\text{ m/s}^2\) to the right
(C) \(1.25\text{ m/s}^2\) to the left
(D) \(5.0\text{ m/s}^2\) to the left
Thinking Hint: Compute kinetic friction: \(f_k = \mu_k F_N\). Which direction does kinetic friction always oppose? Use \(a = \Sigma F / m\).
AP Physics 1 Study Packet • Section 1 Page 2 of 11
Section I: Multiple Choice • Questions 5–8 Relative Motion, System Dynamics & Gravitation
5. A drone flies due East with a velocity of \(18\text{ m/s}\) relative to the ground. A bicyclist directly below rides due East at \(7\text{ m/s}\) relative to the ground. What is the velocity of the drone from the reference frame of the bicyclist?
(A) \(25\text{ m/s}\) East
(B) \(11\text{ m/s}\) East
(C) \(11\text{ m/s}\) West
(D) \(7\text{ m/s}\) West
Thinking Hint: Relative velocity formula: \(\vec{v}_{D/B} = \vec{v}_{D/G} - \vec{v}_{B/G}\). If both move in the same direction, subtract magnitudes.
6. Block \(A\) of mass \(m\) rests on the floor of an elevator, and Block \(B\) of mass \(2m\) rests on top of Block \(A\). The elevator is moving upward while slowing down at rate \(a\). Let \(F_{A\text{ on }B}\) be the normal contact force exerted on \(B\) by \(A\), \(F_{B\text{ on }A}\) be the contact force exerted on \(A\) by \(B\), and \(F_{gB}\) be the weight of Block \(B\). Which ranking is correct?
(A) \(F_{B\text{ on }A} = F_{A\text{ on }B} = F_{gB}\)
(B) \((F_{B\text{ on }A} = F_{A\text{ on }B}) < F_{gB}\)
(C) \(F_{gB} < (F_{B\text{ on }A} = F_{A\text{ on }B})\)
(D) \(F_{A\text{ on }B} < F_{B\text{ on }A} < F_{gB}\)
Thinking Hint: First, Newton's 3rd law mandates \(F_{A\text{ on }B} = F_{B\text{ on }A}\) unconditionally. Next, moving upward and slowing down means acceleration points downward. For Block \(B\), \(\Sigma F_y = F_{A\text{ on }B} - F_{gB} = -m_B a\).
7. Two gliders move along a frictionless 1D air track. From \(t = 0\) to \(t = t_1\), the position of their center of mass \(x_{cm}\) increases linearly with time. Between \(t = t_1\) and \(t = t_2\), the graph of \(x_{cm}\) curves upward (concave up). Which physical event could cause this change?
(A) A compressed internal spring between the gliders expanded, pushing them apart.
(B) A net external force in the \(+x\)-direction was exerted on one or both gliders.
(C) An inelastic collision occurred where the gliders stuck together.
(D) Equal and opposite magnetic attraction forces pulled the gliders closer together.
Thinking Hint: Concave up on \(x-t\) means positive acceleration (\(a_{cm} > 0\)). What is required to accelerate the center of mass: internal forces or net external force?
8. Three scientific satellites orbit Earth in concentric circular paths. Satellite 1 has mass \(m_0\) at orbital radius \(R_0\); Satellite 2 has mass \(4m_0\) at radius \(2R_0\); Satellite 3 has mass \(6m_0\) at radius \(3R_0\). Let \(F_1, F_2, F_3\) represent the gravitational force exerted on each satellite by Earth. Which is the correct ranking?
(A) \(F_1 = F_2 > F_3\)
(B) \(F_1 > F_2 > F_3\)
(C) \(F_2 > F_3 > F_1\)
(D) \(F_3 > F_2 > F_1\)
Thinking Hint: Newton's Law of Gravitation: \(F_g = G \frac{M_E m}{r^2}\). Evaluate the ratio \(m/r^2\) for each satellite: \(1/1^2 = 1\), \(4/2^2 = 1\), \(6/3^2 = 6/9 = 2/3\).
AP Physics 1 Study Packet • Section 1 Page 3 of 11
Section I: Multiple Choice • Questions 9–12 Friction Models, Inclines & Projectile Motion
9. An 80.0 N equipment crate rests on a horizontal concrete floor. The coefficient of static friction is \(\mu_s = 0.40\), and the coefficient of kinetic friction is \(\mu_k = 0.25\). A technician applies a horizontal pulling force of \(24.0\text{ N}\) to the crate. What is the magnitude of the resulting acceleration of the crate?
(A) \(0\text{ m/s}^2\)
(B) \(0.5\text{ m/s}^2\)
(C) \(2.5\text{ m/s}^2\)
(D) \(3.0\text{ m/s}^2\)
Thinking Hint: First calculate the maximum threshold of static friction: \(f_{s,max} = \mu_s F_N = 0.40(80\text{ N}) = 32\text{ N}\). Compare the applied force (\(24\text{ N}\)) to \(f_{s,max}\). Does the crate move?
10. A block of mass \(M\) is placed on an incline tilted at angle \(\theta\) above the horizontal. The incline is rough, with static friction coefficient \(\mu_s\). The block remains completely stationary. What is the exact magnitude of the static friction force exerted on the block by the incline surface?
(A) \(\mu_s M g \cos\theta\)
(B) \(M g \sin\theta\)
(C) \(\mu_s M g \sin\theta\)
(D) \(M g \tan\theta\)
Thinking Hint: Static friction is an adjustable force governed by equilibrium (\(\Sigma F_\parallel = 0\)) unless slipping is impending! \(\mu_s F_N\) gives the maximum potential friction, not the actual friction needed to hold it still.
11. A block of mass \(M\) is launched with initial velocity \(v_0\) so that it slides UP an incline of angle \(\theta\). The coefficient of kinetic friction is \(\mu_k\). What is the total magnitude of the net force acting on the block parallel to the incline as it slides upward?
(A) \(M g \sin\theta - \mu_k M g \cos\theta\)
(B) \(\mu_k M g \cos\theta\)
(C) \(M g \sin\theta + \mu_k M g \cos\theta\)
(D) \(M g (\sin\theta + \cos\theta)\)
Thinking Hint: When sliding UP, which direction does gravity act along the ramp? Down the ramp. Which direction does kinetic friction act? Down the ramp (opposing motion). Since both point down the ramp, their magnitudes add!
12. A tennis ball is launched from ground level at an angle of \(35^\circ\) above the horizontal with initial speed \(v_0\). Neglecting air resistance, which statement is true at the precise instant the ball reaches the peak (apex) of its parabolic trajectory?
(A) Both velocity and acceleration are zero.
(B) Velocity is non-zero, but acceleration is zero.
(C) Velocity is zero, but acceleration is non-zero.
(D) Both velocity and acceleration are non-zero.
Thinking Hint: At the apex, only the vertical component of velocity is zero (\(v_y = 0\)). What about horizontal velocity \(v_x = v_0 \cos(35^\circ)\)? And what external force is acting, dictating the acceleration vector?
AP Physics 1 Study Packet • Section 1 Page 4 of 11
Section I: Multiple Choice • Questions 13–16 Angled Pulls, Kinematic Reversals & Newton's 3rd Law
13. A block of mass \(m\) rests on a rough ramp inclined at angle \(\theta\). A rope pulls the block with tension \(F\) directed at an angle \(\phi\) ABOVE the surface of the ramp. As the block slides UP the ramp with friction force \(f\), what is the correct algebraic expression for the net force along the incline?
(A) \(F \sin\phi - mg \cos\theta - f\)
(B) \(F \cos\phi - mg \sin\theta - f\)
(C) \(F \cos(\theta + \phi) - mg \sin\theta - f\)
(D) \(F - mg \sin\theta - f\)
Thinking Hint: Resolve force \(F\) into axes parallel and perpendicular to the ramp. The component parallel to the ramp is \(F\cos\phi\). The opposing forces along the ramp are gravity component \(mg\sin\theta\) and friction \(f\).
14. A laboratory cart is launched along a straight track inclined at angle \(\theta\). At \(t = 0\), the cart has velocity \(v_0 = +3.0\text{ m/s}\) in the \(+x\)-direction (up the track) and experiences a constant acceleration \(a = -1.0\text{ m/s}^2\). Which statement correctly describes the cart's motion at \(t = 5.0\text{ s}\)?
(A) Moving in the \(+x\)-direction and slowing down.
(B) Moving in the \(-x\)-direction and slowing down.
(C) Moving in the \(-x\)-direction and speeding up.
(D) At rest at its turnaround point.
Thinking Hint: Use \(v(t) = v_0 + at = 3.0 + (-1.0)(5.0) = -2.0\text{ m/s}\). Since velocity is negative (\(-x\)) and acceleration is negative (\(-x\)), are the vectors aligned or opposing? When signs match, speed increases!
15. Two identical stars of equal mass orbit each other while their center of mass orbits a supermassive black hole at radius \(R\) in a clockwise circular path. At a given instant, which arrow correctly represents the acceleration of the two-star system's center of mass?
(A) Pointing tangentially along the direction of circular velocity.
(B) Pointing directly toward the supermassive black hole.
(C) Pointing directly toward the more massive star.
(D) Zero, because the internal gravitational pulls cancel.
Thinking Hint: For any system traveling in uniform circular orbit, what is the net external force on the center of mass? In which direction must the centripetal acceleration point?
16. A tow truck exerts a constant horizontal force \(F\) on three different vehicles: an immobile stuck trailer (\(a = 0\)), an accelerating lightweight sedan (\(a > 0\)), and a heavy truck skidding backwards against the pull (\(a < 0\)). In which case is the magnitude of the force exerted by the vehicle on the tow truck greatest?
(A) The stuck trailer, because no motion occurs.
(B) The accelerating sedan, because it gains speed.
(C) The skidding truck, because it opposes the tow direction.
(D) The force is exactly the same (\(F\)) in all three cases.
Thinking Hint: Read carefully: Newton's Third Law states that if Object A exerts force \(F\) on Object B, Object B exerts force \(-F\) on Object A regardless of mass, state of motion, or acceleration!
AP Physics 1 Study Packet • Section 1 Page 5 of 11
Section I: Multiple Choice • Questions 17–20 Acceleration Rankings, Circular Motion & Pulleys
17. A cart moves along a straight line. Segment \(AB\) runs from \(t=0\) to \(1.0\text{ s}\) with velocity changing from \(0\) to \(8\text{ m/s}\). Segment \(BC\) runs from \(t=1.0\) to \(2.0\text{ s}\) with constant velocity \(8\text{ m/s}\). Segment \(CD\) runs from \(t=2.0\) to \(2.5\text{ s}\) with velocity decreasing from \(8\) to \(0\text{ m/s}\). Segment \(DE\) runs from \(t=2.5\) to \(3.5\text{ s}\) with velocity decreasing from \(0\) to \(-4\text{ m/s}\). Which segment has the greatest magnitude of average acceleration?
(A) Segment \(AB\)
(B) Segment \(BC\)
(C) Segment \(CD\)
(D) Segment \(DE\)
Thinking Hint: Average acceleration magnitude is \(|a_{avg}| = |\Delta v / \Delta t|\). Calculate: \(AB = 8/1.0 = 8\text{ m/s}^2\); \(CD = |-8|/0.5 = 16\text{ m/s}^2\); \(DE = |-4|/1.0 = 4\text{ m/s}^2\).
18. A child of mass \(M\) sits on a playground swing of negligible mass. The swing rope runs over an ideal overhead pulley, and the free end is held by the child, who pulls downward with tension \(T\) so the system hangs at rest in equilibrium. Which equation represents the relationship between tension \(T\), child's mass \(M\), and \(g\)?
(A) \(T = Mg\)
(B) \(2T = Mg\)
(C) \(T = 2Mg\)
(D) \(T = \frac{1}{4}Mg\)
Thinking Hint: Consider the system consisting of (child + swing). How many rope segments pull upward on this system? The left rope segment pulls up with \(T\), and the child's hands pull down on the right rope, so the right rope pulls UP on the hands with \(T\)!
19. Two spheres of mass \(m\) and \(4m\) are separated by distance \(L\) on a frictionless horizontal rod. If both spheres are simultaneously shifted a distance \(\Delta x\) directly toward one another, how does the location of the system's center of mass shift?
(A) It shifts toward the \(4m\) sphere by an amount less than \(\Delta x\).
(B) It shifts toward the \(m\) sphere by an amount less than \(\Delta x\).
(C) It shifts toward the \(m\) sphere by an amount greater than \(\Delta x\).
(D) It does not shift at all.
Thinking Hint: Use \(\Delta x_{cm} = \frac{m_1 \Delta x_1 + m_2 \Delta x_2}{m_1 + m_2}\). If sphere 1 moves \(+\Delta x\) and sphere 2 moves \(-\Delta x\): \(\Delta x_{cm} = \frac{m(+\Delta x) + 4m(-\Delta x)}{5m} = -\frac{3}{5}\Delta x\). It moves in the direction of the \(4m\) sphere's shift!
20. A stunt driver executes a vertical loop-the-loop of radius \(R\). What is the minimum speed \(v_{min}\) the car can have at the exact peak (top) of the loop without losing contact with the track?
(A) \(v_{min} = \sqrt{\frac{gR}{2}}\)
(B) \(v_{min} = \sqrt{gR}\)
(C) \(v_{min} = \sqrt{2gR}\)
(D) \(v_{min} = 2\sqrt{gR}\)
Thinking Hint: At the apex, \(\Sigma F_c = F_N + mg = m\frac{v^2}{R}\). To maintain contact without falling off, normal force \(F_N \ge 0\). The minimum condition occurs when \(F_N = 0\).
AP Physics 1 Study Packet • Section 1 Page 6 of 11
Section II: Constructed Response • Questions 1 & 2 Kinematics QQT & 2D Projectiles
CR 1. Qualitative-Quantitative Translation: Chase & Catch-Up Kinematics
At \(t = 0\), a stationary sports car starts from rest at \(x = 0\) with constant acceleration \(a_c\). At that exact instant, a delivery truck passes the car at constant speed \(v_T\). The sports car catches up alongside the truck at position \(x = D\) at time \(t_D\).
Part (a): Express time \(t_D\) in terms of \(D\) and \(v_T\). Then derive an expression for the car's acceleration \(a_c\) in terms of \(v_T\) and \(D\).
Part (b): A student claims: "Because both vehicles travel distance \(D\) over the same time \(t_D\), their final speeds at \(x = D\) must be equal." Critique this claim. State what is correct and incorrect using velocity-time relationships.
Thinking Hint: Truck moves at constant speed, so \(D = v_T t_D\). Car starts from rest, so \(D = \frac{1}{2}a_c t_D^2\). Substitute \(t_D\). For part (b), remember the car's average speed is \(\frac{0 + v_{car}(t_D)}{2}\). For equal average speed, what must \(v_{car}(t_D)\) be compared to \(v_T\)?
Student Work / Derivation Area:
CR 2. Multi-Trajectory Projectile Comparison
Three identical rocks are launched from a cliff of height \(H\) with the same launch speed \(v_0\): Rock 1 launched at \(+45^\circ\) above horizontal, Rock 2 launched horizontally (\(0^\circ\)), and Rock 3 launched at \(-45^\circ\) below horizontal. Air resistance is negligible.
Part (a): Rank the rocks by total time in air from greatest to least. Justify.
Part (b): Compare the vertical velocity components \(|v_y|\) immediately before hitting the ground for Rocks 1 and 3.
Part (c): Compare the overall impact speeds \(v_{impact}\) of all three rocks. Explain physically.
Thinking Hint: Vertical motion alone dictates time in flight (\(\Delta y = v_{y0}t - \frac{1}{2}gt^2\)). Notice Rock 1 reaches its original launch height on the way down with velocity \(-v_0\sin 45^\circ\), identical to Rock 3's launch! For impact speed, think about conservation of mechanical energy (\(\frac{1}{2}m v_0^2 + mgH\)).
Student Work Area:
AP Physics 1 Study Packet • Section 2 Page 7 of 11
Section II: Constructed Response • Questions 3 & 4 Vertical Circular Motion & Atwood System
CR 3. Vertical Circular Motion & String Rupture Dynamics
A small sphere of mass \(M\) is tethered to a light string of length \(R\) rotating clockwise in a vertical plane. Point \(Z\) is at the top of the circle, Point \(Q\) is at the bottom, and Point \(P\) is at 9 o'clock where the string is horizontal and moving upward.
Part (a): Draw free-body diagrams for the ball at Point \(P\) and Point \(Q\). Include relative vector lengths.
Part (b): Derive an expression for \(v_{min}\) at the apex \(Z\) so the string remains taut.
Part (c): If the string abruptly snaps at the exact instant the ball passes Point \(P\), describe the subsequent trajectory.
Thinking Hint: At the top, \(\Sigma F_c = T + Mg = M v^2/R\). Critical speed occurs at \(T \to 0\). At Point \(P\), velocity is directed strictly vertically upward; once the string snaps, what force remains? The ball becomes a 1D vertical projectile!
Student FBD & Derivation Box:
CR 4. Modified Multi-Body Atwood Machine Analysis
Two blocks of masses \(m_1\) and \(m_2\) (\(m_2 > m_1\)) hang vertically over frictionless massless pulleys connected across a flat horizontal bench. Initially, the string runs straight across between the pulleys.
Part (a): Treating \((m_1 + m_2)\) as a combined system, derive the system acceleration \(a_{sys}\) in terms of \(m_1, m_2,\) and \(g\).
Part (b): A third block of mass \(m_3\) is now tied between the pulleys onto the horizontal string on the frictionless bench. Does the acceleration of \(m_2\) increase, decrease, or remain the same? Justify using Newton's second law.
Thinking Hint: Net external force driving the original system is \((m_2 - m_1)g\). When \(m_3\) is placed on the frictionless horizontal table, does the net external force change? What happens to the total system mass that must be accelerated? Use \(a = \Sigma F_{ext} / M_{total}\).
Student Derivation & Explanation Area:
AP Physics 1 Study Packet • Section 2 Page 8 of 11
Section II: Constructed Response • Questions 5 & 6 Wall Friction & Incline Center of Mass
CR 5. Static Friction Against a Vertical Surface
A physics textbook of mass \(m = 2.0\text{ kg}\) is held against a vertical wall by a horizontal pushing force \(F\). The coefficient of static friction between book and wall is \(\mu_s = 0.40\), and kinetic friction is \(\mu_k = 0.25\).
Part (a): Draw a fully labeled free-body diagram of the book while stationary.
Part (b): Derive an algebraic expression for the minimum force \(F_{min}\) required to keep the book from slipping.
Part (c): If the applied force is increased to \(2F_{min}\), does the friction force double? Explain clearly.
Thinking Hint: Vertical equilibrium requires \(f_s = mg\). Horizontal equilibrium requires \(F_N = F\). For no slipping, \(f_s \le \mu_s F_N \implies mg \le \mu_s F\). In part (c), if the book doesn't accelerate vertically, what must the actual friction force equal?
Student FBD & Calculations:
CR 6. Incline Multi-Body Dynamics & String Severance
Two identical blocks, \(X\) and \(Y\), each of mass \(M\), are connected by a taut string of length \(d\) on a frictionless incline of angle \(\theta\). The two-block system is released from rest, sliding down the incline together.
Part (a): Derive the original acceleration \(a_{cm,orig}\) of the center of mass of the connected two-block system down the incline.
Part (b): Suppose the string is cut. Block \(Y\) is allowed to slide freely while Block \(X\) is held clamped in place. Compare the new acceleration of the center of mass \(a_{cm,new}\) to \(a_{cm,orig}\).
Thinking Hint: On a frictionless incline, each free mass has acceleration \(g\sin\theta\). For part (b), system mass is still \(2M\). The external force down the incline is now only the gravity component on Block \(Y\) (\(Mg\sin\theta\)). Use \(a_{cm} = \frac{\Sigma F_{ext}}{M_{total}} = \frac{Mg\sin\theta}{2M}\).
Student Derivation & Analysis:
AP Physics 1 Study Packet • Section 2 Page 9 of 11
Section II: Constructed Response • Questions 7 & 8 Experimental Design & Elevator Apparent Weight
CR 7. Experimental Design: Sprinter Kinematics Investigation
A varsity sprinter runs a 100 m dash. Past athletic studies suggest sprinters accelerate with constant acceleration \(a_u\) for time \(t_u\), then maintain constant top speed \(v_{max}\) for the remainder of the race. Your physics class has 10 students with stopwatches, measuring tape, chalk, and a starter's horn.
Part (a) Procedure: Outline a step-by-step procedure to measure the runner's position versus time along the straight 100 m track to determine \(a_u\) and \(t_u\).
Part (b) Analysis: Describe how to analyze the data (graphing method) to determine the exact time \(t_u\) at which acceleration ceases and calculate \(a_u\).
Thinking Hint: Have timers stationed at known pre-measured intervals (e.g., every 10 meters). All timers start simultaneously on the sound/flash. On an \(x\) vs \(t\) graph, the accelerating phase is a parabola (\(x = \frac{1}{2}a t^2\)), transitioning into a straight line of slope \(v_{max}\). How can you find the transition point?
Student Experimental Plan:
CR 8. Apparent Weight & Elevator Mechanics
A passenger of mass \(M = 60\text{ kg}\) stands on a calibrated platform scale inside an elevator cab. Consider three distinct operational phases: (1) Ascending and speeding up at \(2\text{ m/s}^2\), (2) Ascending at constant velocity of \(4\text{ m/s}\), and (3) Ascending while slowing down to a stop at \(3\text{ m/s}^2\).
Part (a): Calculate the scale reading (normal force in Newtons) during each of the three phases. Take \(g = 10\text{ m/s}^2\).
Part (b): Explain why the scale reading changes even though the passenger's actual gravitational weight remains constant.
Thinking Hint: The scale measures the normal force \(F_N\) it exerts on the passenger's feet. Write Newton's 2nd Law: \(\Sigma F_y = F_N - Mg = M a_y \implies F_N = M(g + a_y)\). Assign correct signs to \(a_y\) for each phase!
Student FBD & Calculations:
AP Physics 1 Study Packet • Section 2 Page 10 of 11
Section II: Constructed Response • Questions 9 & 10 Gravitational Fields & Incline Variable Angles
CR 9. Gravitational Field Superposition & Lagrange Null Point
Two isolated spherical planetoids, Body 1 of mass \(M_1 = M\) and Body 2 of mass \(M_2 = 4M\), are situated in deep space with their centers separated by distance \(D\). Point \(P\) is located along the line joining their centers.
Part (a): Derive the exact distance \(x\) from Body 1 to Point \(P\) where the net gravitational field of the two bodies is zero (\(g_{net} = 0\)).
Part (b): If a third small probe of mass \(m\) is placed at this null point with a tiny perturbation toward Body 2, explain whether it will return to Point \(P\) or accelerate away.
Thinking Hint: Equate field magnitudes: \(G \frac{M}{x^2} = G \frac{4M}{(D - x)^2}\). Take the square root of both sides to avoid quadratic factoring: \(\frac{1}{x} = \frac{2}{D - x}\). Solve for \(x\). Is the equilibrium stable or unstable?
Student Derivation Area:
CR 10. Incline Scale Tension as a Function of Tilt Angle
A cart of mass \(m\) is held stationary on a frictionless ramp by a lightweight string attached to a force sensor parallel to the incline. The angle \(\theta\) of the incline can be smoothly adjusted from \(\theta = 0^\circ\) (horizontal) to \(\theta = 90^\circ\) (vertical).
Part (a): Derive the tension \(F_T(\theta)\) measured by the sensor as an explicit function of \(m, g,\) and \(\theta\).
Part (b): Sketch the curve of \(F_T\) versus \(\theta\) from \(0^\circ\) to \(90^\circ\). Describe the curvature (concave up or down) and explain why the reading reaches \(mg\) at \(90^\circ\).
Thinking Hint: Parallel equilibrium gives \(F_T - mg\sin\theta = 0 \implies F_T = mg\sin\theta\). Recall the shape of the sine function from \(0\) to \(\pi/2\) radians (\(0^\circ\) to \(90^\circ\)). What is its second derivative? It starts at 0 with positive slope and curves downward (concave down) to a maximum of \(mg\) at \(90^\circ\)!
Student Graph Sketch & Justification Area:
AP Physics 1 Study Packet • Section 2 Page 11 of 11