Lesson 3 of 195 minutes

Vectors and Two-Dimensional Motion

Start with the lesson question, connect the representations, and test the model with evidence.

vectorscomponentsprojectile motionindependencetrajectorymodel assumptions

Learning objectives

  • Create and connect motion diagrams, graphs, and algebraic models.
  • Analyze one- and two-dimensional motion using evidence.
  • Justify predictions with units, signs, and limiting cases.
Lesson flowHook, model, explanationShow guidance

Inspect the opening phenomenon

Predict what changes, then name the evidence.

Apply in the lab

Name the evidence before reading the answer.

Read only what helps

Then use the lab and recall check.

More when needed

Transcript and resources stay available below.

Course progress

AP Physics 1 — Algebra-Based · Kinematics · Lesson 3

Vectors and Two-Dimensional Motion

In progress

Decision challenge

Observe the phenomenon. Then connect the representations.

Use the opening example to make a prediction, identify evidence, and explain which model supports it.

Sideways Speed Does Not Delay the Fall | AP Physics 1

Predict whether a dropped ball or horizontally launched ball reaches the floor first from the same height.

Predict which ball lands first, calculate the shared flight time, and test what changes when horizontal speed doubles.

Before

Predict whether a dropped ball or horizontally launched ball reaches the floor first from the same height.

During

Pause after the 1.80-meter height appears and calculate the shared flight time before the result is revealed.

After

Explain what doubles and what stays unchanged when horizontal launch speed doubles.

Reference drawerTranscript, source notes, scripts, and package status stay tucked away until you need them.7 files

Lesson reading

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5 min

Video script

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Transcript fallback

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courses/ap-physics-1/modules/01-kinematics/lessons/03-vectors-and-two-dimensional-motion/video-transcript.md

Test the Shared-Time Projectile Model

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1 hr 15 min

Mastery check

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7 questions / 18 min

Book section:courses/ap-physics-1/modules/01-kinematics/lessons/03-vectors-and-two-dimensional-motion/book-section.md
Transcript for accessibility and fallback

# Transcript Two balls leave the same table together. One drops. One launches sideways. Which lands first? Sideways speed feels like extra airtime, but gravity only cares about the vertical motion. For the horizontal launch, horizontal velocity stays constant. Vertically, both balls start with zero vertical velocity and accelerate downward at g. Same height, same vertical model, same clock. From one point eight meters, time equals the square root of two h over g, or zero point six one seconds. At three point zero meters per second sideways, the projectile travels one point eight two meters, but still lands with the dropped ball. At the top of an angled path, only vertical velocity is zero. Horizontal velocity remains. Double the horizontal speed: what doubles, and what stays the same? Learn the full vector method free at EduQuest AI.

Reading lab

Core explanation

Connect the lesson's words, diagrams, graphs, evidence, and equations.

Driving question

How can one curved path be predicted by two simpler motions?

Before learning: make a prediction

At the same instant, one ball is dropped and an identical ball is launched horizontally from the same height. Ignore air resistance. Which reaches the floor first? Sketch both paths and explain what evidence would change your mind.

Hook: sideways motion does not buy extra fall time

Gravity changes vertical velocity whether the object also moves sideways or not. A projectile's curved path is the combination of constant horizontal velocity and accelerated vertical motion.

Resolve a vector before using it

For a vector of magnitude AA at angle θ\theta above the positive horizontal axis,

Ax=Acosθ,Ay=Asinθ.A_x=A\cos\theta,\qquad A_y=A\sin\theta.

The signs come from the chosen axes, not from the trigonometric function alone. Reconstruct the vector with

A=Ax2+Ay2,θ=tan1 ⁣(AyAx),A=\sqrt{A_x^2+A_y^2},\qquad \theta=\tan^{-1}\!\left(\frac{A_y}{A_x}\right),

then use the component signs to select the correct quadrant.

Velocity vector resolved into signed horizontal and vertical components

Worked component check

A ball leaves a launcher at 20.0 m/s20.0\text{ m/s} and 30.030.0^\circ above horizontal:

v0x=(20.0)cos30.0=17.3 m/s,v_{0x}=(20.0)\cos30.0^\circ=17.3\text{ m/s}, v0y=(20.0)sin30.0=10.0 m/s.v_{0y}=(20.0)\sin30.0^\circ=10.0\text{ m/s}.

The magnitude check gives 17.32+10.0220.0 m/s\sqrt{17.3^2+10.0^2}\approx20.0\text{ m/s}.

One clock, two component models

Choose positive xx horizontally and positive yy upward. With negligible drag,

ax=0,ay=g.a_x=0,\qquad a_y=-g.

Therefore,

x=x0+v0xt,x=x_0+v_{0x}t, y=y0+v0yt12gt2,y=y_0+v_{0y}t-\frac12gt^2, vx=v0x,vy=v0ygt.v_x=v_{0x},\qquad v_y=v_{0y}-gt.

The components evolve independently, but they share the same time tt. That shared clock reconnects them into one trajectory.

A dropped ball and a horizontally launched ball have equal vertical positions at equal times

Worked example: horizontal launch

A ball rolls horizontally from a 1.80 m1.80\text{ m} table at 3.00 m/s3.00\text{ m/s}. Take the launch point as y=0y=0 and upward as positive.

Vertical motion determines flight time:

1.80=12(9.80)t2,-1.80=-\frac12(9.80)t^2,

so

t=2(1.80)9.80=0.606 s.t=\sqrt{\frac{2(1.80)}{9.80}}=0.606\text{ s}.

Horizontal displacement is then

Δx=(3.00)(0.606)=1.82 m.\Delta x=(3.00)(0.606)=1.82\text{ m}.

At impact,

vx=3.00 m/s,vy=(9.80)(0.606)=5.94 m/s.v_x=3.00\text{ m/s},\qquad v_y=-(9.80)(0.606)=-5.94\text{ m/s}.

The impact-speed magnitude is

v=3.002+(5.94)2=6.66 m/s.v=\sqrt{3.00^2+(-5.94)^2}=6.66\text{ m/s}.

Read the velocity along the path

At the highest point of an angled projectile, vy=0v_y=0 for an instant, but vxv_x is still nonzero when drag is negligible. The acceleration is still downward: ay=ga_y=-g.

Projectile velocity vectors showing constant horizontal component and changing vertical component

During learning: component audit

  1. Define axes, origin, positive directions, and the system.
  2. Draw the vector before resolving it.
  3. Keep xx and yy equations separate.
  4. Use one shared value of time.
  5. Recombine components only when the question asks for magnitude or direction.
  6. Check units, signs, and limiting cases.

Model limits

The simple projectile model assumes negligible air resistance, nearly constant gg, and a flat-Earth scale small enough that Earth's curvature is irrelevant. Drag can change both components and break the constant-vxv_x claim.

Misconception clinic

“A horizontal launch delays the fall.” Horizontal velocity does not change the vertical acceleration in the ideal model.

“Velocity is zero at the top.” Only vyv_y is zero; vxv_x remains.

“The components are two different objects.” They are perpendicular descriptions of one vector.

“Acceleration points along the path.” In ideal projectile motion it points vertically downward.

“A negative component means slowing down.” It indicates direction relative to the chosen axis.

After learning: retrieval and transfer

  1. Why do a dropped ball and a horizontally launched ball reach the floor together?
  2. What is shared between the xx and yy component models?
  3. What are vxv_x, vyv_y, and aya_y at the top of an ideal trajectory?
  4. If horizontal launch speed doubles from the same height, what changes and what does not?
  5. Which observation would show that air resistance is not negligible?

AP-style evidence routine

  1. State axes and assumptions.
  2. Resolve initial vectors with signs and units.
  3. Select the component that determines time.
  4. Solve each component model independently.
  5. Recombine only if needed.
  6. Defend the answer with a graph, limiting case, or measured comparison.

Key takeaway

A curved projectile path becomes predictable when you resolve vectors, model horizontal and vertical motion separately, and reconnect them with their shared time.

Further learning and alignment

Practice labTest the Shared-Time Projectile ModelOpen this when you are ready to apply the model, collect evidence, and check your explanation.1 hr 15 min

Objective

Test whether horizontal launch speed changes flight time and evaluate a two-component projectile model with uncertainty.

Safety and supervision

Adult or teacher supervision is required. Use a soft foam ball or low-energy marble ramp. Keep the landing zone clear and away from faces, glass, electronics, stairs, and walkways. Do not launch projectiles toward people. Use floor padding and retrieve objects only after trials stop.

Materials

  • Soft ball or marble and a short tabletop ramp
  • Meterstick or tape measure
  • Phone slow-motion camera on a stable support, or a projectile-motion simulation
  • Masking tape and landing paper
  • Optional plumb line

Setup

Measure launch height hh from the ball's center at release to the floor. Arrange a horizontal exit and mark the point directly below it. Define +x+x outward and +y+y upward.

Steps

  1. Predict whether a slow and fast horizontal launch from the same height have different flight times.
  2. Record launch height and its uncertainty.
  3. Make at least five slow and five fast launches without changing height.
  4. Use video frames to measure flight time, or measure range and independently estimate launch speed over a known horizontal interval.
  5. Record raw values before averaging.
  6. Calculate the model time t=2h/gt=\sqrt{2h/g}.
  7. Compare mean slow/fast times and uncertainty intervals with the model.
  8. Graph horizontal position versus time for one trial and vertical position versus time for the same frames.
  9. Identify systematic effects such as nonhorizontal release, frame timing, bounce location, parallax, or air drag.

Data table

Triallaunch conditionhh (m)v0xv_{0x} (m/s)measured tt (s)range (m)notes
1slow
2slow
3fast
4fast

Expected Result

Within uncertainty, slow and fast horizontal launches from the same height should have the same flight time when drag is negligible. The faster launch should have greater horizontal range.

Uncertainty and CER

Report measurement resolution, variation across trials, and at least one systematic limitation. Write a claim about flight-time independence, cite quantitative evidence, and connect the evidence to the separate-component model.

Reflection Questions

  1. Which measurements test the vertical model directly?
  2. Why is range alone insufficient to show equal flight time?
  3. What pattern should appear on x(t)x(t) and y(t)y(t) graphs?
  4. Which error could create an apparent speed-dependent flight time?
  5. Does agreement prove drag is exactly zero? Explain.

Accessibility and alternatives

Use a simulation with keyboard controls and exported data if physical launching, reaching the floor, hearing impact, or frame-by-frame video work is inaccessible. Provide high-contrast markers, a partner role, and a text description of every visual observation.

Extension Challenge

Launch at a small upward angle, fit x(t)x(t) and y(t)y(t) separately, and test whether one shared time series explains both components.