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Domains and validity of mechanics models

Find when a motion formula applies, choose physically relevant roots and distinguish a negative coordinate from an impossible prediction.

Before you startQuadratic equations, completing the square and the mechanics modelling cycle.

01 / An equation does not define its own physical scope

State the event that ends the model.

Algebraic values and physical predictions are different.

A polynomial can be evaluated at any real input. A motion model may apply only after release and before contact. Use the assumptions and the reference level to decide the valid domain.

A flight model ends at contactExplore

Use h=10+15t−5t² metres above level ground. Time t is in seconds after release. This simplified model describes free flight until the first ground contact.

02 / Understand the reference level and initial value

Height is measured from a stated zero.

01 · Release height

For h=10+15t−5t², find the height at release.

Hint

Release means t=0.

Worked solution

h(0)=10 m above the chosen ground level.

02 · Later height

Find h at t=2 s.

Hint

Substitute into every term.

Worked solution

h(2)=10+30−20=20 m. The value is above ground and before the first contact.

03 / Solve for the terminating event

Ground contact means h=0 in this coordinate system.

Find when the model reaches level ground.Worked example

10+15t−5t²=0 ⇒ t²−3t−2=0

Divide by −5 and rearrange.

t=(3±√17)/2

The roots are about −0.56155 and 3.56155.

First contact after release: T=(3+√17)/2 s

The negative root is outside this experiment. Use 0≤t≤T for the flight model.

Watch: the valid curve ends at ground contact

Pause, replay or seek freely. The notes explain the same idea and stay in view.

03 · Root choice

Why is the negative root rejected for the flight after release?

Hint

Read the definition of elapsed time.

Worked solution

It corresponds to a time before t=0. It is a root of the extended polynomial, not a ground contact during the stated experiment.

04 · End behaviour

Does this quadratic specify what happens after the object hits the ground?

Hint

The assumptions describe free flight only.

Worked solution

No. Bouncing, deformation or remaining at rest require additional assumptions. Do not extend the flight equation through the contact event.

04 / Check a turning point against the valid interval

A mathematical maximum must also occur during the modelled motion.

Complete the square.Worked example

h=85/4−5(t−3/2)²

The squared term is nonnegative.

Maximum h=85/4=21.25 m at t=1.5 s

This time lies between 0 and T, so the maximum occurs within the flight domain.

05 · Explain the maximum

Why does the completed-square form prove this upper bound?

Hint

A square cannot be negative.

Worked solution

Subtracting 5 times a nonnegative square cannot exceed 85/4. Equality occurs when t−3/2=0.

06 · Restricted interval

If observations only cover 0≤t≤1, does the observed maximum reach 21.25 m?

Hint

The turning point is outside this shorter interval.

Worked solution

No. Height increases on this interval and reaches h(1)=20 m at its endpoint. The full-flight maximum lies later.

05 / Two valid roots can describe ascent and descent

Do not discard a root merely because another one exists.

07 · Height 20 m

Solve h=20 and interpret the two times.

Hint

Rearrange to t²−3t+2=0.

Worked solution

t=1 s or t=2 s. Both lie in the flight domain: the object passes 20 m once while rising and once while falling.

08 · Unreachable height

Can the object reach 22 m in this model?

Hint

Compare with the maximum.

Worked solution

No. The maximum is 21.25 m, so there is no real time with h=22.

06 / A negative coordinate can be meaningful

Its meaning depends on the origin and the physical boundary.

09 · Invalid extension

Calculate h(4) and explain why it is not a free-flight prediction here.

Hint

Contact has already happened before 4 s.

Worked solution

h(4)=10+60−80=−10 m. It is below the level ground, but more importantly t=4 exceeds the first-contact time. The flight model no longer applies.

10 · Different reference

If vertical coordinate y is measured upwards from a balcony, what could y=−3 m mean before landing?

Hint

Zero is the balcony, not necessarily the ground.

Worked solution

The object is 3 m below the balcony. This can be a valid position if it remains above the actual ground or another contact boundary.

11 · Reference change

If the ground coordinate is h and the balcony is 10 m above ground, express y in terms of h.

Hint

Subtract the balcony height.

Worked solution

y=h−10. Ground contact is y=−10, not y=0. A change of origin does not change the physical flight.

07 / Validate the formula as well as the root

A plausible value is not evidence of accuracy by itself.

12 · Simplified gravity

What constant vertical acceleration is represented by the coefficient −5 in this quadratic?

Hint

Compare with h=h₀+ut+(1/2)at², if familiar.

Worked solution

a=−10 m/s² in the upwards-positive convention. This is a simplified constant-acceleration model, not a claim that local gravitational acceleration is exactly 10 everywhere.

13 · Assumption limit

Name one physical effect omitted by this free-flight formula.

Hint

The equation has no varying resistive force.

Worked solution

For example air resistance. A substantial drag force would make constant downward acceleration a poor approximation.

14 · Reporting a domain

State the domain and its interpretation in a complete sentence.

Hint

Include the endpoint and units.

Worked solution

The model applies from release at t=0 until first ground contact at t=(3+√17)/2≈3.562 s, with t measured in seconds.

08 / Keep the physical event beside the algebra

Choose roots using the model, not a memorised rule.

Define the reference level, solve the relevant event equation and keep all roots that fit the physical interval. Check maxima within that interval. Negative coordinates are not automatically impossible; extending a model past the event that ends its assumptions is the real problem.

Section 1 of 8 · An equation does not define its own physical scope