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Full Hooke's Law Investigation Lab

A full-workflow physics investigation. Choose an investigation, state your hypothesis, identify the independent and dependent variables, collect replicated trials, fit a regression line, and analyze residuals and percent error.

Choose an Investigation

Investigation A. F vs x (derive k)

How does the force applied to a spring depend on its extension, and what does the slope of F vs x tell us about the spring constant?

Independent Variable

Mass m hung on the spring (or applied force F)

Dependent Variable

Extension x (averaged from 3 ruler readings)

Controlled Variables
  • Spring constant k (one fixed spring)
  • Gravity g (local, constant)
  • Temperature, mounting position
Hypothesis Prompt

Predict the shape of the F vs x curve below the elastic limit. What relationship should appear, and what does the slope represent?

Expected Result

F vs x is linear with slope = k. R² should exceed 0.99 with careful measurement. Derived k should match the nominal spring constant within a few percent.

Procedure
  1. Record 6 to 8 trials at different masses (or applied forces) within the elastic range
  2. Verify F vs x is linear (R² near 1)
  3. Read the slope directly. The slope IS the spring constant k
  4. Compute percent error vs the accepted nominal k
  5. Identify any trials whose residuals stand out as outliers

Setup

N/m
kg
m/s²
N
m
N/m

Each "Record Trial" simulates 3 ruler readings of the extension with realistic measurement scatter (±2 mm). The recorded x is the average of those three readings. In Investigation A the applied force is m·g; in Investigations B and C the applied force F is set directly.

Current Setup

rest0.30 kgx = 0.059 mk = 50 N/mF = 2.94 N

Force F (N) vs Extension x (m)

-0.0500.2250.5000.7751.050-0.100.200.500.801.10Extension x (m)Force F (N)

Record at least 2 trials (or load sample data) to see the regression line.

Regression & Error Analysis

Record at least 2 trials to compute the regression. For a defensible fit you should collect 6 or more trials across the full range of the IV.

Data Table

(0 rows)
#TrialMass (m)(kg)Force F(N)Extension x (avg of 3)(m)x std dev(m)Elastic PE(J)Derived k = F/x(N/m)
0 / 500
0 / 500
0 / 500

Reference Guide

Investigation Workflow

A scientific investigation needs more than a single measurement. It needs a hypothesis, a clear independent and dependent variable, repeated trials, a fit line, and an honest error analysis.

  1. State a testable hypothesis
  2. Identify IV, DV, and controlled variables
  3. Record at least 6 replicated trials across the range of the IV
  4. Fit a regression line and inspect residuals
  5. Quote a final value with uncertainty and percent error

Hooke's Law

For an ideal spring inside its elastic range, the restoring force is proportional to the extension.

F=kxF = k\,x

Doubling the extension doubles the force. The constant of proportionality k is the spring constant in newtons per metre. Stiffer springs have larger k.

U=12kx2U = \tfrac{1}{2}\,k\,x^{2}

The elastic potential energy stored in a stretched spring grows quadratically with the extension.

Deriving k from F vs x

Hooke's Law is already linear in x, so the slope of a best-fit line through your F vs x data IS the spring constant.

kexp=slope of F vs xk_{\text{exp}} = \text{slope of } F \text{ vs } x

A higher R² and a smaller slope uncertainty give a more reliable derived k. With careful ruler readings R² should exceed 0.99 across six trials in the elastic regime.

In Investigation A the applied force is m·g for each mass; in Investigation B the same fixed force is applied to springs of different stiffness; in Investigation C the force is pushed beyond the yield point so the slope changes.

Error Analysis

Quote the derived value with both uncertainty and percent error.

%error=kexpkacceptedkaccepted×100%\%\text{error} = \frac{|k_{\text{exp}} - k_{\text{accepted}}|}{k_{\text{accepted}}} \times 100\%

Slope uncertainty propagates directly to k since k equals the slope. Inspect residuals for systematic patterns. A growing residual at high x is a signature of the spring approaching its elastic limit, where Hooke's Law no longer holds and the apparent k drops below the small-extension value.

The main sources of uncertainty are ruler resolution (about 1 mm), parallax in reading the ruler, slight nonlinearity of the spring, and the mass of the spring itself adding a small extra extension.

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