End an electric trajectory at its first boundary event
A uniform electric field gives a passive charge constant force qE. In this fictional model the bead has q=1 nC and mass 10⁻⁸ kg, enters halfway between plates with horizontal velocity and zero vertical velocity, and experiences no gravity. The vertical acceleration is a_y=qE/m=0.1E in SI units. Horizontal velocity stays constant because the ideal field is vertical.
Learning outcome: Compare E=−100,0,+100 N/C at fixed horizontal speed. Then increase speed to 3 m/s and classify the first event again. Retain event times, endpoint and work/energy residual rather than extrapolating all paths to the far edge.
Starting recap
Use signed charge, common coordinate axes, SI units, vector components and algebraic ratios. Separate a source field from probe force and a fitted parameter from independently tested evidence.
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For E=100 N/C and vx=2 m/s, a_y=10 m/s². Contact occurs at √.02≈.141421 s before exit at .2 s. At contact x≈.282843 m, y=.1 m and vy≈1.414214 m/s. Work qEΔy=10⁻⁸ J matches the gained vertical kinetic energy.
Open the experimentPredict
If plate contact occurs before horizontal exit, the valid endpoint is:
Experiment
Compare E=−100,0,+100 N/C at fixed horizontal speed. Then increase speed to 3 m/s and classify the first event again. Retain event times, endpoint and work/energy residual rather than extrapolating all paths to the far edge.
Stop the trajectory at the first plate or exit event
Worked teaching model · synthetic values · Fictional bead q=1 nC, mass=1e−8 kg enters at y=0 with vy=0. Plates at y=±.1 m, length .4 m, uniform field inside and no gravity. A first contact or horizontal exit ends the model; no post-contact or fringe prediction. Virtual only.
Reset keeps your prediction, captures and practice history.
Trajectory only up to first event
Spatial axes use the same pixels per physical unit, preserving geometry. 1: bounded bead trajectory (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Trajectory only up to first event
bounded bead trajectory
| x (m) | y (m) |
|---|---|
| 0 | 0 |
| 0.00707107 | 0.0000625 |
| 0.0141421 | 0.00025 |
| 0.0212132 | 0.0005625 |
| 0.0282843 | 0.001 |
| 0.0353553 | 0.0015625 |
| 0.0424264 | 0.00225 |
| 0.0494975 | 0.0030625 |
| 0.0565685 | 0.004 |
| 0.0636396 | 0.0050625 |
| 0.0707107 | 0.00625 |
| 0.0777817 | 0.0075625 |
| 0.0848528 | 0.009 |
| 0.0919239 | 0.0105625 |
| 0.0989949 | 0.01225 |
| 0.106066 | 0.0140625 |
| 0.113137 | 0.016 |
| 0.120208 | 0.0180625 |
| 0.127279 | 0.02025 |
| 0.13435 | 0.0225625 |
| 0.141421 | 0.025 |
| 0.148492 | 0.0275625 |
| 0.155563 | 0.03025 |
| 0.162635 | 0.0330625 |
| 0.169706 | 0.036 |
| 0.176777 | 0.0390625 |
| 0.183848 | 0.04225 |
| 0.190919 | 0.0455625 |
| 0.19799 | 0.049 |
| 0.205061 | 0.0525625 |
| 0.212132 | 0.05625 |
| 0.219203 | 0.0600625 |
| 0.226274 | 0.064 |
| 0.233345 | 0.0680625 |
| 0.240416 | 0.07225 |
| 0.247487 | 0.0765625 |
| 0.254558 | 0.081 |
| 0.26163 | 0.0855625 |
| 0.268701 | 0.09025 |
| 0.275772 | 0.0950625 |
| 0.282843 | 0.1 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Vertical acceleration | 10 | m/s² |
| First event time | 0.141421 | s |
| First event x | 0.282843 | m |
| First event y | 0.1 | m |
| First event is contact (includes tie) | 1 | flag |
| Horizontal velocity at event | 2 | m/s |
| Vertical velocity at event | 1.41421 | m/s |
| Kinetic energy gain | 1e-8 | J |
| Electric work to event | 1e-8 | J |
| Potential difference to event | -10 | V |
The first plate contact ends the model before any later exit prediction.
Use a_y=qE/m, y=a_y t²/2 and x=v_x t. Compare event times before evaluating endpoints; the zero-field case has no plate-contact event. Work qE Delta y equals the kinetic-energy increase, with Delta V=−E Delta y. Contact is not a continuation through a plate; a simultaneous exit/contact is labeled explicitly by the contact flag.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
The first plate contact ends the model before any later exit prediction.
Use a_y=qE/m, y=a_y t²/2 and x=v_x t. Compare event times before evaluating endpoints; the zero-field case has no plate-contact event. Work qE Delta y equals the kinetic-energy increase, with Delta V=−E Delta y. Contact is not a continuation through a plate; a simultaneous exit/contact is labeled explicitly by the contact flag.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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