Precision spring dynamometer
Applies and measures the horizontal pulling force required to maintain steady slider motion with 0.02 N resolution.
Investigate Amontons–Coulomb laws of friction and determine the coefficient of kinetic friction μ by linear regression of friction force against normal load. Explore a virtual apparatus, collect readings and analyse a graph.
Ready for a virtual observation.
Adjust the apparatus, then take a reading.
Readings are generated by an ideal model. The diagram is schematic and is not to scale.
The simulation assumes dry Coulomb friction between homogeneous rigid surfaces without thermal softening, surface wear degradation, or stick-slip resonance. Observations reflect polished wood-on-wood contact (reference μ = 0.350) with standard dynamometer reading resolution of 0.02 N.
Applies and measures the horizontal pulling force required to maintain steady slider motion with 0.02 N resolution.
Provides uniform planar contact surfaces with captive tray for holding calibrated slotted weights.
Provides a rigid, level, polished guiding surface for slider travel.
Allows normal compressive force N to be varied systematically from 1.0 N to 14.0 N.
Investigate Amontons–Coulomb laws of friction and determine the coefficient of kinetic friction μ by linear regression of friction force against normal load. Suggested independent settings: 2.0, 4.0, 6.0, 8.0, 10.0 N.
Hold the spring balance horizontally on the bench, tap gently to relieve internal spring friction, and record any zero-point offset.
In a horizontal position, the spring does not support the hook self-weight, shifting the zero calibration compared to vertical suspension.
Verify with a spirit level that the track is strictly horizontal, and wipe both the slider base and track bed with clean lint-free cloth.
Any slope introduces a gravitational component along the track, while dust or grease drastically alters the interfacial shear strength.
Load the slider tray with slotted weights to establish the desired total normal force N (slider tare weight plus added load).
Distributing weights symmetrically over the slider ensures uniform contact pressure across the entire interface without tilting.
Connect the spring balance hook to the slider eyelet parallel to the bench and pull steadily until the slider transitions from static grip to uniform constant sliding.
Pulling at an upward or downward angle alters the effective normal force by F sin(θ), corrupting the N-axis value.
Note the force reading on the dynamometer while the slider is in steady, non-accelerating motion across the central test span.
Static friction exhibits a peak threshold before motion; only steady motion measures the true kinetic coefficient μ_k.
Repeat the observation across all five independent normal loads from 2.0 N to 10.0 N to assemble the linear regression dataset.
Testing across a wide range of normal loads verifies Amontons’ proportionality and minimizes slope estimation error.
Points are your observations. The fit uses SI x and y values before display scaling.
| # | Normal load N (N) | Frictional force Ff (N) | Normal load N (N) | Frictional force Ff (N) | Remove |
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No readings yet. Take a virtual measurement and record it.