Vanier College · 203-SN1-RE

Vanier 203-SN1-RE: mechanics tutoring

Work through motion and force questions in Vanier 203-SN1-RE. Your tutor can help you distinguish velocity from acceleration, choose the forces on one object and check the signs in your equation. Start with the elevator example, then choose the braking or beam problem to review.

About 203-SN1-RE

Vanier lists 203-SN1-RE as Mechanics in Pure and Applied Science. Its Physics Wiki brings together material on motion, forces and conservation laws. The example below connects a change in velocity to the force a scale measures.

Topics to review

  • Units, measurement and vectors
  • Motion in one and two dimensions; rotational kinematics
  • Newton’s laws and force diagrams
  • Static equilibrium and torque
  • Work, energy and power
  • Linear and angular momentum

For work–energy practice, read a force–position graph and check which positions can be reached. The worked example and four optional questions connect signed area, initial kinetic energy and speed.

Start here

Before you start

You will use signed numbers, the slope of a straight velocity–time graph and a one-step force equation. Acceleration describes how velocity changes; its direction can differ from the direction of travel.

What to watch for

  • Inferring acceleration from a change in velocity
  • Distinguishing weight from the scale’s normal force

Mechanics: stopping distance and torque balance

Find a stopping time and distance, then balance a beam. Choose positive directions before writing the force and torque equations.

Before you start: Allow 20–25 minutes to try both questions, then 15 minutes to check and retry any missed steps.

1. A force gives a stopping distance

A 2.0 kg2.0\,\mathrm{kg} cart moves right at 4.0 m/s4.0\,\mathrm{m/s}. A constant net horizontal force of 4.0 N4.0\,\mathrm N acts left until it stops. Find the stopping time and distance.

Show the explained solution
  1. With right positive, a=Fnet/m=−2.0 m/s2a=F_{\mathrm{net}}/m=-2.0\,\mathrm{m/s^2}.
  2. From 0=4.0−2.0t0=4.0-2.0t, the stopping time is t=2.0 st=2.0\,\mathrm s.
  3. Using 02=4.02+2(−2.0)Δx0^2=4.0^2+2(-2.0)\Delta x gives Δx=4.0 m\Delta x=4.0\,\mathrm m. Check with work: the initial 16 J16\,\mathrm J is removed by (−4.0)(4.0)=−16 J(-4.0)(4.0)=-16\,\mathrm J.

Check the stopping time, distance and braking interval

2. Balance rotation and translation

A massless horizontal beam is hinged at its left end. A 60 N60\,\mathrm N downward load acts 0.80 m0.80\,\mathrm m from the hinge. An upward vertical cable force acts 1.20 m1.20\,\mathrm m from the hinge. Find the cable tension and the vertical hinge force in static equilibrium.

Show the explained solution
  1. Let TT be the upward cable tension and HyH_y the hinge-force component, positive upward. Take torques about the hinge, so its force contributes no torque. With counterclockwise positive, 1.20T−0.80(60)=0.1.20T-0.80(60)=0.
  2. Thus T=40 NT=40\,\mathrm N. Next impose vertical force balance: Hy+40−60=0H_y+40-60=0.
  3. The hinge force is Hy=20 NH_y=20\,\mathrm N upward. Zero net torque alone does not establish zero net force; both conditions are needed.

Review a hinged beam and cable

Use your answers to plan your revision
  1. Stopping problems

    Use one sign convention from the force equation through the motion calculation. Check the distance against the loss of kinetic energy.

  2. Equilibrium problems

    Choose the torque pivot deliberately, then write both rotational and translational equilibrium equations.

When requesting mechanics support, include your free-body diagram, axis choice and your section’s permitted review questions. That makes it easier to target the setup you need.

Request 203-SN1-RE exam preparation help

Original Nablio practice, not an official examination.

Course topic sources

A rising elevator: what does the scale read?

A passenger of mass m=60 kgm=60\,\mathrm{kg} stands on a force scale in an elevator. The elevator is rising, but its upward velocity decreases uniformly from 3.0 m/s3.0\,\mathrm{m/s} to 1.0 m/s1.0\,\mathrm{m/s} over 2.0 s2.0\,\mathrm s. The passenger stays at rest relative to the elevator. Use g=9.8 m/s2g=9.8\,\mathrm{m/s^2}. Model the passenger as a single point, ignoring body size. Neglect air resistance. Find the scale reading in newtons during this interval. First predict: is it greater than, equal to or less than the passenger’s weight?

Show a hint

Take upward as positive. Find acceleration from the change in velocity before writing the force equation. The scale reads the normal force it exerts on the passenger.

Show the reasoning
  1. 1. Separate motion from change in motion

    Both velocities are positive because the elevator is moving upward. However, velocity is decreasing, so acceleration points downward. A positive velocity does not require a positive acceleration.

  2. 2. Find the acceleration

    Let viv_i and vfv_f be the initial and final vertical velocities, Δt\Delta t the elapsed time, and aa the vertical acceleration. Because the velocity changes uniformly, aa is constant.

    a=vf−viΔta=\frac{v_f-v_i}{\Delta t}

    a=(1.0−3.0) m/s2.0 sa=\frac{(1.0-3.0)\,\mathrm{m/s}}{2.0\,\mathrm s}

    a=−1.0 m/s2a=-1.0\,\mathrm{m/s^2}

  3. 3. Draw forces on the passenger

    There are two vertical forces: the normal force NN from the scale upward, and the gravitational force mgmg downward. Here mm is mass in kilograms and gg is gravitational acceleration in m/s2\mathrm{m/s^2}.

    The magnitude of the weight is:

    mg=(60)(9.8) Nmg=(60)(9.8)\,\mathrm N

    mg=588 Nmg=588\,\mathrm N

    Draw one dot for the passenger, an upward arrow labelled NN and a downward arrow labelled mgmg. The elevator’s upward velocity is not an extra force.

  4. 4. Use the net force

    With upward positive, Newton’s second law is:

    N−mg=maN-mg=ma

    Rearranging gives:

    N=m(g+a)N=m(g+a)

    Substitute the values in SI units:

    N=60(9.8−1.0) NN=60(9.8-1.0)\,\mathrm N

    N=528 NN=528\,\mathrm N

    The scale reads 528 N528\,\mathrm N, less than the 588 N588\,\mathrm N weight.

  5. 5. Check the result

    N−mg=(528−588) NN-mg=(528-588)\,\mathrm N

    N−mg=−60 NN-mg=-60\,\mathrm N

    This agrees with:

    ma=(60)(−1.0) Nma=(60)(-1.0)\,\mathrm N

    ma=−60 Nma=-60\,\mathrm N

    Also, kg⋅m/s2\mathrm{kg\cdot m/s^2} is a newton. The passenger is still moving upward while the net force slows that upward motion. The mass and the gravitational force have not changed.

Upward velocity and downward acceleration are separate from the passenger’s two forces: N = 528 N upward and mg = 588 N downward.
Upward is positive. The motion arrows indicate only the directions of velocity v and acceleration a. The two force arrows start at the point representing the passenger; their lengths are proportional to 528 N and 588 N.

Try the opposite direction

The same passenger now travels downward. With upward still positive, the elevator’s velocity changes uniformly from −3.0 m/s-3.0\,\mathrm{m/s} to −1.0 m/s-1.0\,\mathrm{m/s} in 2.0 s2.0\,\mathrm s. Predict whether the scale reading is above or below 588 N588\,\mathrm N, then calculate it.

Check your answer
  1. Find the sign from the velocity change

    a=[−1.0−(−3.0)] m/s2.0 s\begin{gathered}a=\\\frac{[-1.0-(-3.0)]\,\mathrm{m/s}}{2.0\,\mathrm s}\end{gathered}

    a=+1.0 m/s2a=+1.0\,\mathrm{m/s^2}

    The elevator is moving downward and slowing down, so acceleration points upward.

  2. Reuse the force equation

    N=m(g+a)N=m(g+a)

    N=60(9.8+1.0) NN=60(9.8+1.0)\,\mathrm N

    N=648 NN=648\,\mathrm N

    The reading is above 588 N588\,\mathrm N. The sign of acceleration controls this comparison. At constant vertical velocity, a=0a=0 and the scale would read 588 N588\,\mathrm N in either direction.

If the acceleration sign was the difficult part, review motion graphs. If the force equation was the difficult part, review free-body diagrams.

How a tutor can help

A tutor can ask you to predict the scale reading before calculating, check your chosen positive direction and help you separate a velocity arrow from a force arrow. You can then fix the first incorrect equation and try the downward-motion check without copying the worked answer.

Prepare for an assessment

Bring the topics announced for your assessment and a practice problem. Include any work you have started, or ask your tutor to help you begin. Practise explaining a sign or force choice before doing the calculation, then redo a missed question with the direction of motion changed.

Angular momentum: choose the system and axis

For a rotation problem, extend your force diagram by naming the system and axis. The six questions ask when angular momentum is conserved, how a changed inertia affects rotation and what happens when an object sticks to a disk. Use them when this topic is in your current chapter.

Try six angular-momentum questions

Bring a question to a tutor. You can build the diagram and first angular-momentum equation together, or review what you have started. You can check the external-torque assumption, the signs and the energy comparison before retrying a missed question.

Official course information

Before a lesson

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Use your current course outline and your instructor’s announced topics to decide which parts of this guide to practise. Follow your section’s assessment instructions.

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Connect equilibrium and static friction

When rigid-body equilibrium is in your assigned material, practise force diagrams, torques and the friction limit in one model. This supplement is not a complete course review or an exam prediction.

Ladder equilibrium: maximum distance and minimum angle