Predict attraction and repulsion between charges
Use charge signs and inverse-square distance scaling to interpret a force pair.
Learning outcome: Apply Coulomb’s law with units and distinguish third-law partners from net force on one object.
Starting recap
Positive and negative are charge signs, not labels for greater or smaller mass. Equal-and-opposite interaction forces act on different objects.
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Try
If two charges exert opposite forces, why does each still need a support to remain fixed?
Open the experimentPredict
At Q = +2 nC and r = 0.20 m, predict force direction for q = +2 nC and q = −2 nC. Predict the magnitude change if separation doubles.
Experiment
Capture q = +2 and −2 nC at 0.20 m. Keep q fixed and compare 0.40 m. Inspect both force rows and explain the shared signed scale.
Separate electric force, field and potential
Worked teaching model · synthetic values · Two prescribed stationary point charges in vacuum, Q = +2 nC at x = 0 and q = −4 to +4 nC to its right. Rounded Coulomb constant k = 8.99 × 10⁹ N m²/C². The field and potential shown at q are due to Q alone and exclude self-fields. Q and q remain fixed as sources for each selected scenario; controls select comparisons, not time evolution or a charge-transfer process. Mutual electric forces are equal and opposite but act on different charges. External supports that hold positions are not drawn; their forces would balance the electric forces. Potential and pair interaction energy are zero at infinite separation. Work compares the same q moved from r = 0.20 m to the selected r with Q fixed; external work assumes quasistatic transfer with no kinetic-energy change. No acceleration, radiation, polarization, finite-size charges, breakdown or dielectric response. Charge zero is a neutral ideal point with no polarization, not a general model of neutral matter.
Reset keeps your prediction, captures and practice history.
| Quantity | Value | Interpretation |
|---|---|---|
| Electric field from Q at q | 449.500000 N/C | Rightward; defined even when q = 0 |
| Force on q | 0.899000 µN | qE; sign gives direction |
| Force on Q | -0.899000 µN | Equal-and-opposite partner on a different charge |
| Potential from Q at q | 89.900000 V | Energy per charge; 1 V = 1 J/C |
| Pair interaction energy | 0.179800 µJ | qV, with zero at infinite separation |
| Quantity | Value | Meaning |
|---|---|---|
| Reference potential | 89.900000 V | From Q at 0.20 m |
| Initial pair energy | 0.179800 µJ | Same q as selected now |
| Change in pair energy | 0.000000 µJ | Final minus initial |
| Work by electric field | 0.000000 µJ | Negative of interaction-energy change |
| Quasistatic external work | 0.000000 µJ | Equal to energy change when kinetic energy does not change |
The work comparison holds the selected q fixed between the reference and final positions. Changing the charge slider selects another scenario; it is not a simulated charging process. Supporting forces are omitted from the force-pair diagram, so its electric force values are not the total forces on the held charges.
repulsion: force on q 0.899000 µN; field from Q 449.500000 N/C to the right.
Potential from Q 89.900000 V; pair interaction energy 0.179800 µJ. From 0.20 m, field work 0.000000 µJ and quasistatic external work 0.000000 µJ. Changing q does not change the displayed field or potential from the prescribed Q.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
Understand
Apply
Public practice checks a specific claim. It does not establish independent mastery.
State which object each force acts on, how charge and distance affect magnitude, and why changing the charge slider is not a conservation-of-charge simulation.
Continue
Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.
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