Keep carrier averaging separate from pulse integration
A plane wave carries energy through its Poynting vector. For a sinusoidal carrier, cycle averaging gives intensity epsilon0c Eamplitude²/2. Now let that carrier amplitude have a slowly varying envelope Epeak sin(πt/T) over a pulse of duration T. The carrier frequency is stipulated 1 GHz while T is in microseconds, so the envelope is slow relative to the carrier.
Learning outcome: Compare doubled amplitude with doubled duration and derive each scaling before revealing values. Retain both averaging steps, area and momentum idealization. Explain what additional material and geometry evidence would be needed to infer deposited heat or detector response.
Starting recap
Review flux integrals, linear differential equations, initial conditions, complex numbers and vector derivatives. Keep source constraints, RMS conventions and calibration roles explicit.
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For Epeak=2 V/m and T=2 microseconds, Ipeak=2epsilon0c and fluence is 2epsilon0c×10⁻⁶ J/m². With the internally consistent teaching constants this is about 5.305165×10⁻⁹ J/m². The selected area intercepts about 5.305165×10⁻¹¹ J; perfect reflection transfers twice the absorbing momentum for that same intercepted energy.
Open the experimentPredict
At fixed duration, doubling peak electric carrier amplitude changes pulse energy by:
Experiment
Compare doubled amplitude with doubled duration and derive each scaling before revealing values. Retain both averaging steps, area and momentum idealization. Explain what additional material and geometry evidence would be needed to infer deposited heat or detector response.
Integrate pulse energy and transferred momentum
Worked teaching model · synthetic values · Locally plane vacuum wave, carrier frequency1 GHz and slowly varying sine envelope over duration T. Cycle-averaged intensity I(t)=epsilon0 c Epeak² sin²(pi t/T)/2 for0≤t≤T. Uniform intercepted area.01 m²; compare ideal complete absorption and perfect normal reflection. No exposure, detector response or material-safety claim.
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Cycle-averaged envelope, not resolved carrier oscillations
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: sin-squared envelope (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Cycle-averaged envelope, not resolved carrier oscillations
sin-squared envelope
| time (microseconds) | intensity (W/m²) |
|---|---|
| 0 | 0 |
| 0.025 | 8.17703e-6 |
| 0.05 | 3.26577e-5 |
| 0.075 | 7.32911e-5 |
| 0.1 | 0.0001298266 |
| 0.125 | 0.0002019158 |
| 0.15 | 0.0002891142 |
| 0.175 | 0.0003908841 |
| 0.2 | 0.0005065982 |
| 0.225 | 0.0006355429 |
| 0.25 | 0.0007769234 |
| 0.275 | 0.0009298679 |
| 0.3 | 0.001093434 |
| 0.325 | 0.001266612 |
| 0.35 | 0.001448335 |
| 0.375 | 0.001637483 |
| 0.4 | 0.001832889 |
| 0.425 | 0.002033349 |
| 0.45 | 0.002237627 |
| 0.475 | 0.002444463 |
| 0.5 | 0.002652582 |
| 0.525 | 0.002860702 |
| 0.55 | 0.003067538 |
| 0.575 | 0.003271815 |
| 0.6 | 0.003472275 |
| 0.625 | 0.003667682 |
| 0.65 | 0.00385683 |
| 0.675 | 0.004038553 |
| 0.7 | 0.004211731 |
| 0.725 | 0.004375297 |
| 0.75 | 0.004528241 |
| 0.775 | 0.004669622 |
| 0.8 | 0.004798567 |
| 0.825 | 0.004914281 |
| 0.85 | 0.005016051 |
| 0.875 | 0.005103249 |
| 0.9 | 0.005175338 |
| 0.925 | 0.005231874 |
| 0.95 | 0.005272507 |
| 0.975 | 0.005296988 |
| 1 | 0.005305165 |
| 1.025 | 0.005296988 |
| 1.05 | 0.005272507 |
| 1.075 | 0.005231874 |
| 1.1 | 0.005175338 |
| 1.125 | 0.005103249 |
| 1.15 | 0.005016051 |
| 1.175 | 0.004914281 |
| 1.2 | 0.004798567 |
| 1.225 | 0.004669622 |
| 1.25 | 0.004528241 |
| 1.275 | 0.004375297 |
| 1.3 | 0.004211731 |
| 1.325 | 0.004038553 |
| 1.35 | 0.00385683 |
| 1.375 | 0.003667682 |
| 1.4 | 0.003472275 |
| 1.425 | 0.003271815 |
| 1.45 | 0.003067538 |
| 1.475 | 0.002860702 |
| 1.5 | 0.002652582 |
| 1.525 | 0.002444463 |
| 1.55 | 0.002237627 |
| 1.575 | 0.002033349 |
| 1.6 | 0.001832889 |
| 1.625 | 0.001637483 |
| 1.65 | 0.001448335 |
| 1.675 | 0.001266612 |
| 1.7 | 0.001093434 |
| 1.725 | 0.0009298679 |
| 1.75 | 0.0007769234 |
| 1.775 | 0.0006355429 |
| 1.8 | 0.0005065982 |
| 1.825 | 0.0003908841 |
| 1.85 | 0.0002891142 |
| 1.875 | 0.0002019158 |
| 1.9 | 0.0001298266 |
| 1.925 | 7.32911e-5 |
| 1.95 | 3.26577e-5 |
| 1.975 | 8.17703e-6 |
| 2 | 0 |
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 |
|---|---|---|
| Peak cycle-averaged intensity | 0.005305165 | W/m² |
| Pulse duration | 2.00000e-6 | s |
| Integrated energy per area | 5.30516e-9 | J/m² |
| Energy intercepted by selected area | 5.30516e-11 | J |
| Absorbing-surface momentum transfer | 1.76839e-19 | kg m/s |
| Perfect normal-reflector momentum transfer | 3.53678e-19 | kg m/s |
| Average intensity over pulse duration | 0.002652582 | W/m² |
Integrating the envelope gives a second factor of one half beyond the carrier average.
A plane wave has instantaneous Poynting magnitude epsilon0 c E². Averaging the rapid sinusoidal carrier gives epsilon0 c Eamplitude²/2. The envelope amplitude is Epeak sin(pi t/T); its squared integral over the pulse is T/2. Thus fluence=epsilon0 c Epeak²T/4. Complete absorption transfers U/c momentum and perfect normal reflection 2U/c under the stated idealization. Neither relation determines a material response or exposure limit.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Integrating the envelope gives a second factor of one half beyond the carrier average.
A plane wave has instantaneous Poynting magnitude epsilon0 c E². Averaging the rapid sinusoidal carrier gives epsilon0 c Eamplitude²/2. The envelope amplitude is Epeak sin(pi t/T); its squared integral over the pulse is T/2. Thus fluence=epsilon0 c Epeak²T/4. Complete absorption transfers U/c momentum and perfect normal reflection 2U/c under the stated idealization. Neither relation determines a material response or exposure limit.
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