Springs, Torque & Static Equilibrium · Grade 12 Science

Chapter: Forces, Rotation & Equilibrium

Springs, Torque & Static Equilibrium

Learning goals

Readings for this unit

Before this unit

Vectors, force, energy, graph area, and ratios.

Use the detailed parent plan: two core 50–60-minute sessions per focused unit, with a third assigned for selected calculation/modeling topics. First study the core explanation and Parts 1–2 with their figures/checks; next study Parts 3–4, the whole-unit application, worked cases, varied practice and exit check. Attempt reasoning before opening guidance. Extend time when actual understanding requires it; investigations and chapter assessments have separate sessions.

Start with something to explain

Why can a small force turn a door more easily near its edge?

Illustrative evidence case. The same perpendicular push is applied at two distances from a hinge.

A spring constant describes a tested force–extension rangeA spring constant describes a tested force–extension rangeApplied force at equilibrium (N)0481200.020.040.06Extension from natural length (m)Slope k=200 N/m only in the stated elastic range.
Calculated linear elastic model, not a claim of unlimited extension.

Notice and wonder

Record two observations using the stated quantities or relationships. Keep observations separate from possible causes. Write one question that a new measurement could help answer.

Why can a small force turn a door more easily near its edge?

Your first model

Draw the force line and shortest pivot distance.

Build the language from the idea

spring constant
Stiffness parameter in a linear elastic model.
torque
Turning effect of a force about a specified pivot.
lever arm
Perpendicular distance from pivot to force line.

Hooke’s law models a spring within its linear elastic range: restoring force Fs=−kx, with x measured from the natural equilibrium length and k in N/m. The force magnitude is k times the absolute extension. The minus sign expresses opposition to displacement, not a negative stiffness. Outside this tested range the relation can fail or permanent deformation can occur.

A spring constant describes a tested force–extension rangeA spring constant describes a tested force–extension rangeApplied force at equilibrium (N)0481200.020.040.06Extension from natural length (m)Slope k=200 N/m only in the stated elastic range.
Calculated linear elastic model, not a claim of unlimited extension.

Elastic potential energy is Us=½kx². Work needed to stretch a spring gradually from zero to x is the area under the force-displacement graph. Because force grows from zero to kx, the triangular area is ½kx², not simply final force times total stretch.

A force can also cause rotation. Torque magnitude about a chosen pivot is τ=rF sinθ, with θ between the radius-to-application-point and the force. The perpendicular lever arm version τ=F dperp is equivalent. A force through the pivot produces no torque about it.

Torque uses the perpendicular distance to the force lineTorque uses the perpendicular distance to the force liner⊥ = 0.60 mF = 20 Nτ = F r⊥ = 12 N·m counterclockwise
Original lever geometry; the labeled 0.60 m is the perpendicular arm for this upward force.

A rigid object in static equilibrium needs both zero net force and zero net torque. Balancing upward and downward forces alone does not guarantee it will not rotate. Choose a pivot that removes an unknown support force from the torque equation, then solve remaining force balances.

Static equilibrium requires force and torque balanceStatic equilibrium requires force and torque balance30 N at 0.30 m30 N at 0.30 msupport 60 NΣF=0 and Στ=0 are both required.
Original symmetric weightless-bar model; distributed bar weight is intentionally excluded here.

Ideal levers trade force for motion without creating energy. A longer input lever arm can allow a smaller force to balance a larger load; the input moves farther. Actual mechanisms have friction, flexing, and mass, so evaluate efficiency and stresses before applying an ideal ratio.

A household ruler balance or a gentle small spring is suitable with adult setup and soft light loads. Do not use heavy suspended objects or overstretch an elastic band toward a face. This unit’s equations describe a bounded model, not a structural safety rating.

Build your understanding

Use the detailed parent plan: two core 50–60-minute sessions per focused unit, with a third assigned for selected calculation/modeling topics. First study the core explanation and Parts 1–2 with their figures/checks; next study Parts 3–4, the whole-unit application, worked cases, varied practice and exit check. Attempt reasoning before opening guidance. Extend time when actual understanding requires it; investigations and chapter assessments have separate sessions.

Part 1 · Use the elastic range for Hooke’s law

Extension x is the change from a spring’s natural length. In its linear elastic range, the restoring force is −kx: its sign opposes displacement from equilibrium. A quasistatic applied force balancing it has magnitude kx, producing the plotted positive slope. Past the elastic range a spring may not return to its original length or obey the same linear law. Distinguish the force exerted by the spring from the external force required to hold it stretched.

A spring constant describes a tested force–extension rangeA spring constant describes a tested force–extension rangeApplied force at equilibrium (N)0481200.020.040.06Extension from natural length (m)Slope k=200 N/m only in the stated elastic range.
Calculated linear elastic model, not a claim of unlimited extension.

Read the visual model

Identify the labeled structures and units, then trace the arrows or compare values under the caption’s stated conditions. Separate the displayed evidence from a further inference. Write your reasoning before opening the guidance.

What balancing force is needed at x=0.03 m for this model?

Visual reasoning — after your attempt

F=kx=200×0.03=6 N; the spring exerts 6 N in the opposite direction.

An ideal linear spring exerts restoring force F=−kx along a chosen displacement axis. The minus sign indicates opposition to displacement from equilibrium. Real springs follow this approximation only over a suitable range; k is a stiffness, not a force by itself.

OpenSciEd drawing of six cushioning rings arranged in a triangle with a broad base on the table and one top ring touching the loaded plate.
OpenSciEd 8.1’s actual ring/loaded-plate arrangement is a geometry and deformation prompt. It shows no measured force–time trace and does not by itself establish stiffness, impact performance or safety. The complete local plate-force model below explains the static support account; use measured force/extension evidence before assigning a spring constant. Triangular stack of cushioning rings · OpenSciEd · 8.1 Contact Forces, Lesson 13, source, CC BY 4.0. Figure excerpt rendered from the PDF and resized for the web.
Completed static model for the selected loaded plateCompleted static model for the selected loaded plateplate+loadrings support plateEarth attracts plate+loadBoundary excludes rings; support and weight balance at rest.
Original complete plate-only force model accompanying the OpenSciEd ring arrangement. The rings’ upward support acts on the plate/load system; its weight acts down. These are not a third-law pair. The plate’s downward force on the rings belongs on a separate ring diagram. A static picture alone does not provide a stiffness or stopping-force curve.

A 200 N/m spring stretched 0.050 m has a restoring-force magnitude 10 N in the linear model.

Pause and explain

Why is k not measured in newtons alone?

Check your reasoning after answering

Since force is proportional to extension, k has units N/m so multiplying by displacement gives force.

Part 2 · Use the perpendicular moment arm

Torque measures a force’s turning effect about a chosen pivot. Its magnitude is rFsinθ=F r⊥, where r⊥ is the shortest distance from pivot to the force’s line of action. A large force aimed directly through the pivot can have zero torque even with a long position vector. Assign a turning sign convention, such as counterclockwise positive, and retain N·m units; torque and energy share dimensions but describe different quantities.

Torque uses the perpendicular distance to the force lineTorque uses the perpendicular distance to the force liner⊥ = 0.60 mF = 20 Nτ = F r⊥ = 12 N·m counterclockwise
Original lever geometry; the labeled 0.60 m is the perpendicular arm for this upward force.

Read the visual model

Identify the labeled structures and units, then trace the arrows or compare values under the caption’s stated conditions. Separate the displayed evidence from a further inference. Write your reasoning before opening the guidance.

What torque results if this 20 N force acts along the bar through the pivot?

Visual reasoning — after your attempt

Zero, because its perpendicular moment arm is zero.

Torque about a specified pivot has magnitude rF sinθ, or force times the perpendicular distance from pivot to the force’s line of action. A force through the pivot gives zero torque even if large. Specify clockwise and counterclockwise signs before summing.

For a perpendicular 10 N force at 0.40 m, torque magnitude is 4.0 N·m. An angled force at that radius has a smaller perpendicular contribution.

Pause and explain

Why can a long lever arm still yield zero torque?

Check your reasoning after answering

If the force’s line of action passes through the pivot, perpendicular distance is zero; the physical handle length alone does not determine torque.

Part 3 · Require both force and torque balance

Static equilibrium means the body remains at rest without translational or rotational acceleration. It needs ΣF=0 and Στ=0 about a selected pivot in the rigid-body model. Equal opposing torques alone can coexist with nonzero net force, while balanced forces can still form a turning couple. For this weightless-bar example equal downward loads at equal opposite arms balance torque, and the upward support must balance their combined 60 N force.

Static equilibrium requires force and torque balanceStatic equilibrium requires force and torque balance30 N at 0.30 m30 N at 0.30 msupport 60 NΣF=0 and Στ=0 are both required.
Original symmetric weightless-bar model; distributed bar weight is intentionally excluded here.

Read the visual model

Identify the labeled structures and units, then trace the arrows or compare values under the caption’s stated conditions. Separate the displayed evidence from a further inference. Write your reasoning before opening the guidance.

Could a zero-torque calculation alone establish static equilibrium?

Visual reasoning — after your attempt

No. The vector force sum must also vanish, and the starting state must be at rest.

Static equilibrium needs zero net external force and zero net torque. Torque balance alone does not guarantee no translation. Choose a convenient pivot to eliminate an unknown support torque, then use the force balance to determine that support.

A beam may have balanced moments but still an unbalanced total downward force unless the support force is included.

Pause and explain

Can force balance alone establish static equilibrium?

Check your reasoning after answering

No. Equal opposite forces at different lines of action can produce a nonzero turning effect; torque must also balance.

Part 4 · Account for distributed weight and assumptions

A center of mass summarizes a body’s mass distribution. In a uniform gravitational field, its total weight can be represented at that point for external force and torque calculations. A uniform bar’s center lies at its midpoint, but an attached load or nonuniform density changes it. The small arrows show distributed weight and the larger arrow is an equivalent alternative representation, not an additional force to add on top of them.

A distributed weight needs a justified equivalent locationA distributed weight needs a justified equivalent locationUniform bar weight can be represented at its center.effective mgNonuniform load → find its actual center of mass.
Original distributed/equivalent weight comparison for a uniform bar; choose one representation in a calculation.

Read the visual model

Identify the labeled structures and units, then trace the arrows or compare values under the caption’s stated conditions. Separate the displayed evidence from a further inference. Write your reasoning before opening the guidance.

Should the distributed arrows and equivalent mg both enter the same torque sum?

Visual reasoning — after your attempt

No. They are two representations of the same weight; counting both would double it.

For a uniform beam in a uniform gravitational field, weight acts effectively at its midpoint. A nonuniform beam requires its center of mass. Draw each load and support; indicate whether beam weight, friction, or connector mass is neglected.

A light beam assumption can simplify torque, but a real heavy beam can substantially change the support and spring requirement.

Pause and explain

What is needed if beam mass is not negligible?

Check your reasoning after answering

Its weight and center of mass must enter the force and torque account, along with the existing loads and supports.

Apply the whole unit · Balance a load with an ideal spring

Illustrative massless horizontal beam pivots at its left end. A 10.0 N downward load acts 0.40 m from the pivot; an upward linear spring acts 0.20 m from it, k=200 N/m.

Your task

Find spring force and extension, then determine the signed vertical pivot force. Explain why torque balance does not answer the pivot-force question alone.

What your response should show

  • Define the system, quantities, units, and relevant conditions before selecting a model.
  • Show intermediate calculations or a labeled evidence account, including signs or denominators.
  • Explain how the supplied evidence supports the conclusion rather than reporting only an answer.
  • Identify a meaningful uncertainty, model limit, or measurement needed to test the conclusion.
Response guidance — after your attempt
  1. Torque balance: Fspring×0.20=10.0×0.40; Fspring=20.0 N upward.

  2. Extension magnitude=20.0/200=0.100 m in the linear range.

  3. Vertical balance: Rpivot+20.0−10.0=0; pivot force is 10.0 N downward.

The downward pivot force is consistent with the assumed fixed pivot, which can exert force in either vertical direction. A simple unfastened support that can only push upward would not fit this arrangement. Beam weight and an out-of-range spring would require a revised model.

Scientific references and source-model foundations

Parent / teacher teaching notes

Use separate force and torque sums. Ask whether the support can physically provide the calculated direction rather than treating every algebraic support as feasible. Ask the learner to explain each symbol, axis, unit and arrow before calculating. Calculated examples, supplied illustrative records and actual historical observations are labeled separately. Selected public OpenSciEd middle-school source figures are foundation examples, not complete high-school editions or an endorsement; all advanced explanations are supplied locally.

The key idea

Equilibrium requires balanced forces and torques; spring energy grows with displacement squared.

Worked examples

Example 1

k=200N/m and x=.050 m. Find spring force magnitude and stored energy.
  1. F=kx=10N.
  2. U=½(200)(.050)².
Answer: 10N and .250 J

Example 2 · Worked application

A 20 N force acts perpendicular to a lever 0.30 m from its pivot. Find torque, and balance it with a force at 0.60 m.
  1. τ=rF=0.30×20=6.0 N·m.
  2. For opposite balancing torque, F×0.60=6.0.
  3. F=10 N, assuming other torques balance.
Answer: 6.0 N·m; 10 N opposite-sense force at the stated perpendicular arm.
Check the reasoning

Use perpendicular lever arm and rotational sign.

Example 3

A 6N load at .20 m balances an input at .60 m on the other side. Find input.
  1. Equal opposite torques:6(.20)=F(.60).
  2. F=1.20/.60.
Answer: 2N, neglecting lever mass.

Example 4 · Find and fix the mistake

Context: A 20 N force acts perpendicular to a lever 0.30 m from its pivot. Find torque, and balance it with a force at 0.60 m. A student claims: “Any force applied at a pivot creates a large torque.” Evaluate the claim and write a corrected explanation.
  1. Test the claim against the stated conditions: Use perpendicular lever arm and rotational sign.
  2. Its lever arm about that pivot is zero, so its torque is zero.
Answer: Its lever arm about that pivot is zero, so its torque is zero.
Check the reasoning

Use perpendicular lever arm and rotational sign.

Example 5 · Reason from the visual model

Static equilibrium requires force and torque balanceStatic equilibrium requires force and torque balance30 N at 0.30 m30 N at 0.30 msupport 60 NΣF=0 and Στ=0 are both required.
Original symmetric weightless-bar model; distributed bar weight is intentionally excluded here.
Could a zero-torque calculation alone establish static equilibrium?
  1. Static equilibrium means the body remains at rest without translational or rotational acceleration. It needs ΣF=0 and Στ=0 about a selected pivot in the rigid-body model. Equal opposing torques alone can coexist with nonzero net force, while balanced forces can still form a turning couple. For this weightless-bar example equal downward loads at equal opposite arms balance torque, and the upward support must balance their combined 60 N force.
  2. No. The vector force sum must also vanish, and the starting state must be at rest.
Answer: No. The vector force sum must also vanish, and the starting state must be at rest.
Check the reasoning

Original symmetric weightless-bar model; distributed bar weight is intentionally excluded here.

Avoid these mistakes

Check your understanding

Why does a force through a pivot have zero torque?

Discuss the answer

The perpendicular distance from pivot to force line is zero.

Return to the phenomenon

Return to the initial case. Why can a small force turn a door more easily near its edge? Revise your drawing or explanation using two named ideas and one stated limitation.

Compare explanations after your attempt

Torque grows with the perpendicular arm, while static equilibrium also requires net-force balance.

What should we investigate next?

Which comparison would test a remaining uncertainty? State what you would change, keep comparable and measure.

Investigate, calculate and revise

Keep a first model and an evidence-supported revision. Attempt each task before opening guidance; all required explanations and supplied-data routes are available locally.

Activity 1 · Return to the opening case

Assigned reading and preparation

Use the opening phenomenon, unit definitions and explained Parts 1–4.

Your task

Return to the initial case. Why can a small force turn a door more easily near its edge? Revise your drawing or explanation using two named ideas and one stated limitation.

Success criteria

  • Use the stated observations and appropriate units.
  • Connect a labeled model with the physical/environmental mechanism.
  • State assumptions and an evidence limitation.
  • Explain a substantive revision or next test.
Hint

Keep object/material identity, material transfer and energy account distinct.

Response guidance — discuss after your attempt

Torque grows with the perpendicular arm, while static equilibrium also requires net-force balance.

Activity 2 · Transfer to a changed case

Assigned reading and preparation

Cover the worked answer and use the explained models, relationships and notebook.

Your task

A weightless 2 m beam is pivoted at its left end. A 60 N load acts 0.50 m from the pivot. An upward force acts at the right end. Find that force and vertical pivot reaction for equilibrium.

Success criteria

  • Use the stated measurements or conditions, with correct units.
  • Connect the result to the physical or environmental mechanism or evidence relationship.
  • Identify the assumption, model limit or further evidence requested.
Hint

Name known quantities and conditions, show intermediate steps and check conservation.

Response guidance — discuss after your attempt

Torque balance: F×2=60×0.50, so F=15 N upward. Vertical balance gives pivot reaction=60−15=45 N upward. Both balances are necessary.

Words to know

spring constant
Stiffness parameter in a linear elastic model.
torque
Turning effect of a force about a specified pivot.
lever arm
Perpendicular distance from pivot to force line.

In the real world

Use the chapter investigation to connect this unit to measured evidence and a practical decision.

Exit check

Why does a force through a pivot have zero torque?

Check your explanation after answering

The perpendicular distance from pivot to force line is zero.

Explain your reasoning without notes. If a key idea is missing, revisit the lesson and try again.

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