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SCIENCE · INVESTIGATE AND EXPLAIN

Solve both velocity components before integrating the path

With isotropic linear drag per unit mass gamma, horizontal and vertical equations are dvx/dt=−gamma vx and dvy/dt=−g−gamma vy. The virtual point starts at(0,5) m with velocity(4,6) m/s. Gravity is vertical but resistance acts on both components relative to the stationary medium.

Learning outcome: Compare two gamma values at the same time. Recover initial conditions and derivative identities, then distinguish vertical velocity sign from height.

Starting recap

Differentiate/integrate with explicit initial conditions; identify each force recipient and the inertial frame. Preserve force dimensions, geometric constraints and the distinction between model and solver error.

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Try

At t=0 the formulas recover x0=0,y0=5,vx0=4,vy0=6 for every permitted gamma. Differentiate the position expressions to verify both velocity formulas.

Open the experiment

Predict

With linear drag in a stationary medium, horizontal velocity here:

Experiment

Compare two gamma values at the same time. Recover initial conditions and derivative identities, then distinguish vertical velocity sign from height.

Solve both component differential equations with drag

Worked teaching model · synthetic values · Virtual point starts at(0,5) m with velocity(4,6) m/s. Acceleration=(−gamma vx,−10−gamma vy) in stationary medium. All registered evaluation times precede ground crossing; constant isotropic linear drag and g are stipulated, not a launch protocol.

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Linear-drag trajectory before ground crossing

height (m)east position (m)03.1477556.5054290

Spatial axes use the same pixels per physical unit, preserving geometry. 1: analytic component solution (solid). Joined curves show the supplied model, not additional observations.

Equivalent numerical coordinates for Linear-drag trajectory before ground crossing

analytic component solution

east position (m)height (m)
05
0.049844085.073986
0.09937765.145954
0.14860255.215916
0.19752075.283885
0.24613415.349872
0.29444475.41389
0.34245425.475952
0.39016465.53607
0.43757785.594255
0.48469555.650521
0.53151975.704878
0.57805215.757339
0.62429465.807915
0.6702495.856619
0.71591715.903461
0.76130075.948454
0.80640145.991609
0.85122126.032938
0.89576186.072451
0.94002486.110161
0.9840126.146078
1.0277256.180214
1.0711666.212579
1.1143366.243185
1.1572376.272043
1.1998716.299163
1.242246.324557
1.2843446.348235
1.3261866.370208
1.3677676.390486
1.4090896.40908
1.4501546.426001
1.4909636.441259
1.5315176.454864
1.5718196.466826
1.611876.477157
1.6516726.485865
1.6912256.492962
1.7305326.498456
1.7695946.502359
1.8084126.50468
1.8469896.505429
1.8853256.504616
1.9234236.50225
1.9612836.498341
1.9989076.492899
2.0362976.485933
2.0734546.477453
2.110386.467468
2.1470756.455987
2.1835426.443021
2.2197816.428578
2.2557956.412667
2.2915846.395297
2.3271516.376479
2.3624956.356219
2.397626.334529
2.4325256.311416
2.4672146.286889
2.5016866.260958
2.5359436.23363
2.5699876.204915
2.6038196.174821
2.637446.143358
2.6708516.110532
2.7040546.076354
2.7370516.040831
2.7698426.003971
2.8024285.965784
2.8348125.926277
2.8669945.885458
2.8989755.843336
2.9307575.799919
2.9623415.755215
2.9937285.709232
3.024925.661977
3.0559175.613459
3.0867215.563686
3.1173335.512666
3.1477555.460406

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.

Calculated quantities under the declared measurement model
QuantityValueUnit
East position3.147755m
Height5.460406m
East velocity2.426123m/s
North velocity-4.230203m/s
East acceleration-1.213061m/s²
North acceleration-7.884899m/s²

Linear resistance couples each acceleration to its own velocity component while gravity adds a vertical drive.

vx=4exp(−gamma t) and vy=(6+g/gamma)exp(−gamma t)−g/gamma. Integrating each component retains the initial5 m height. The gamma→0 limit recovers vacuum kinematics, but substituting gamma0 directly into divided expressions is not a valid numerical operation. All supported times remain above ground; no event or impact physics is added.

Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.

Linear resistance couples each acceleration to its own velocity component while gravity adds a vertical drive.

vx=4exp(−gamma t) and vy=(6+g/gamma)exp(−gamma t)−g/gamma. Integrating each component retains the initial5 m height. The gamma→0 limit recovers vacuum kinematics, but substituting gamma0 directly into divided expressions is not a valid numerical operation. All supported times remain above ground; no event or impact physics is added.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Solve both velocity components before integrating the path

With isotropic linear drag per unit mass gamma, horizontal and vertical equations are dvx/dt=−gamma vx and dvy/dt=−g−gamma vy. The virtual point starts at(0,5) m with velocity(4,6) m/s. Gravity is vertical but resistance acts on both components relative to the stationary medium.

The solutions are vx=4exp(−gamma t) and vy=(6+g/gamma)exp(−gamma t)−g/gamma. Integrating from the given initial position gives x=4[1−exp(−gamma t)]/gamma and y=5+(6+g/gamma)[1−exp(−gamma t)]/gamma−gt/gamma. Initial height must not disappear during integration.

At gamma=.5 and t=1, position is approximately(3.14775,5.46041) m and velocity(2.42612,−4.23020) m/s. The point is already descending but remains above its starting-height-relative ground. A downward velocity is not evidence that y is negative.

The gamma→0 limit gives vacuum motion through expansion of the exponential, but directly substituting gamma0 into terms divided by gamma is undefined. The controls stay positive and all supported times precede ground crossing. No physical launch, later impact, wind variation or nonlinear resistance is modeled.

Changed case: predict before checking

At t=0 the formulas recover x0=0,y0=5,vx0=4,vy0=6 for every permitted gamma. Differentiate the position expressions to verify both velocity formulas.

Retained investigation

Compare two gamma values at the same time. Recover initial conditions and derivative identities, then distinguish vertical velocity sign from height. What additional conditions would be needed for a ground-impact calculation?

Sources and boundaries

Primary conceptual reference checked30 October2026: OpenStax University Physics Volume1. Original mathematical cases and synthetic records; no performed experiments, practical certification or actual equipment safety claims. Numerical method/error relations are derived explicitly for the supplied equations. Preserve independent checks, conditional regimes and first-response evidence. No physical release, launch, loading or pulley procedure is requested.

Apply

With linear drag in a stationary medium, horizontal velocity here:

Public practice checks a specific claim. It does not establish independent mastery.

What additional conditions would be needed for a ground-impact calculation?

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