Measuring “g” on Earth’s Surface: Photogates & Ticker Tape Lab
Determine the acceleration due to gravity on Earth by comparing two classic experimental methods: 4 dual-beam digital photogates and a 60 Hz ticker tape timer with quadratic curve fitting.
Standard: g = 9.80 m/s²
1. Laboratory Setup & Pedagogical Guide
Learn the principles of dual-sensor photogates and 60 Hz ticker timers, identify equipment components, and understand how data is collected.
🔬 Laboratory Equipment & Apparatus Orientation
Dual-Sensor Photogate Principles
Each modern digital photogate unit contains two internal optical sensors (Gate 1 at the top and Gate 2 at the bottom, spaced exactly 2.0 cm apart). Across 4 photogates, students collect 8 distinct position and time data points!
Experimental Protocol
Measure Gate Heights: Always align your eye level with the small optical hole of each sensor. Measure both Gate 1 and Gate 2.
Record Block Times: When the falling cylinder cuts through the light beam, the digital sensor state transitions from 0 to 1. Record this exact timestamp.
Watch for Sensor Shuffling: In digital setups, wireless sensors can occasionally report channels out of physical vertical order. Always match the channel ID to its measured height!
Measurement Best Practices
Height Measurement: Align the ruler's horizontal sightline directly with the sensor beam aperture before recording each height.
Release Technique: Support the cylinder gently right above the first gate and release smoothly from rest.
Data Verification: Compare the recorded timestamps with the physical gate order on the stand.
The 60 Hz Spark / Ticker Mechanism
An AC electromagnetic clapper vibrates up and down at 60 cycles per second (60 Hz). Every strike on the rotating carbon disc transfers a dot to the moving paper tape. The time interval between every dot is:
Δt = 1 / 60 s ≈ 0.01667 s
Measuring Protocol
Tape Alignment: Thread the paper strip under the carbon disc so the striker pin makes clear carbon impressions.
Choose Dot 0 (Origin): The first marks made while holding the tape at rest are crowded. Select the first clearly distinct dot and label it Dot 0 (where t = 0 s, y = 0 m).
Measure 12 Consecutive Dots: Using the calibrated metric ruler, measure positions for 12 consecutive points (Dot 0 to Dot 11) relative to Dot 0. Do not skip dots!
Measurement Best Practices
Ensure the ruler's 0 cm line is aligned exactly with Dot 0. Use the vertical sightline hairline to read every dot's position to the nearest millimeter before recording.
⏱️ Photogate Drop Stand
4 Units · 8 Sensors
Height: 0.800 m (80.0 cm)
Cursor:
📍 Release Height (y_drop):m
Δy = 0.0 cm (flush at Gate 1)
🔧 Move Photogates (Gate 1 Height):(Drag on stand or enter heights below)
📡 Digital Sensor Event Log
Time (s)
Sensor Unit
Channel
State
Ready. Click "Drop Object" to capture photogate block timestamps.
📋 Student Data Table (Method I)
Sensor Gate
Height y (m)
Time t (s) [State = 1]
📜 60 Hz Ticker Tape Drop Apparatus
Frequency: 60 Hz (Δt = 1/60 s ≈ 0.01667 s)
The clapper strikes 60 times per second. Spacing expands quadratically with constant acceleration.
📐 Tape Inspection & Ruler Workbench
💡 Click any dot to set as Dot 0. Drag the yellow ruler to measure 12 points.
⚪ Fresh Blank Strip LoadedActive Dot 0: #—
Zoom:1.0x
12 Points at Δt = 0.0167 s each
📋 Student Data Table (Method II)
Dot #
Time t (s) [n/60]
Position y (m)
📈 Position vs. Time & Quadratic Fit
Quadratic Fit Parameters
Model Assumptions & Theory
Empirical fit: y = At² + Bt + C. Standard parabolic freefall model with initial velocity and position parameters.
Teacher Reference: Curve Fit Overview
Empirical fit: y = At² + Bt + C. Students correlate the coefficients with standard 1D kinematics in their lab report.
📝 Official Student Lab Handout Document
Lab: Measuring the Acceleration Due to Gravity on Earth’s Surface “g”
Purpose
In this lab we are going to find out the value of the acceleration of gravity on Earth, “g”, by two methods.
Method I: Photogates
Using the photogates, create a Position vs. Time graph.
Apply a quadratic fit for the parabola.
Copy and paste the graph below
[Method I: Photogates Position vs. Time Graph]
Plot your photogates data in the Analysis tab, or click below to attach the graph:
Method II: Ticker Tape
Using the values of the points in the ticker tape, create a Position vs. Time graph.
Apply a quadratic fit for the parabola.
Copy and paste the graph below
[Method II: Ticker Tape Position vs. Time Graph]
Plot your ticker tape data in the Analysis tab, or click below to attach the graph:
Analysis of the Data
1. In the table below, write the initial position, initial velocity, and acceleration for each case according to the quadratic fit equation.
Photogates
Ticker Tape
y₀ =
v₀ᵧ =
a =
g =
y₀ =
v₀ᵧ =
a =
g =
2. Calculate the % difference in each case by comparing with the reference value of g = 9.8 m/s².
3. Explain why your measured values might differ from the reference value. Mention only reasons that would actually affect the value in a significant way. Write at least 3 valid reasons.
4. Alternative Analysis: Linearization (y versus t²)
Inquiry Extension
Assume the simplified freefall relationship where v0y = 0: y = ½at² + y₀. Graphing y versus t² yields a linear model: y = M·(t²) + K, where the slope represents M = ½a (hence a = 2·M and g = 2·|M|).
Photogates Linearized (y vs. t²)
Ticker Tape Linearized (y vs. t²)
Slope (M) =
Intercept (K) =
g = 2·|M| =
Slope (M) =
Intercept (K) =
g = 2·|M| =
Teacher Grading Rubric & Accepted Explanations
Valid Reason 1 - Mechanical Friction (Ticker Tape): Physical drag between the striker pin, carbon disc, and tape guide slots reduces net acceleration below 9.80 m/s².
Valid Reason 2 - Human Hand Release Jitter (Photogates): If the object is released with an upward/downward nudge (v0y ≠ 0) or tilts while cutting the beam, the effective path timing is altered.
Valid Reason 3 - Parallax & Measuring Scale: Sighting the small photogate beam holes against a meter stick introduces ±1–2 mm parallax uncertainty.
Question 4 Rubric - Linearization Assumptions: The linear model y = M·(t²) + K assumes v₀ = 0 because it contains only a constant and a t² term with no linear t term. When the timer begins at Gate 1 after falling, v₀ ≠ 0; the missing v₀·t term bends the y vs. t² points, lowering R² and skewing the slope.
Invalid Student Explanations: "Human reaction time" (invalid because sensors and timers record automatically), or "gravity changes day to day".