John Abbott College · 203-SN1-RE

John Abbott College Mechanics tutoring

Get help choosing a method for John Abbott 203-SN1-RE Mechanics. Work through a pendulum question that uses energy to find speed, then forces to find string tension.

About 203-SN1-RE

John Abbott’s Science program describes Mechanics through forces, acceleration, energy, momentum, rotational motion and the gravitational field. The example below focuses on connecting energy and forces in one problem.

Topics to review

  • Forces and acceleration
  • Energy and momentum
  • Rotational motion
  • Gravitational field
  • Vectors and projectile motion

Start here

Before you start

Review the cosine of an angle, square roots and force diagrams. You will also use the inward acceleration v2L\frac{v^2}{L} of an object moving along a circular path of radius LL at speed vv.

If you want to practise force diagrams before combining energy and circular motion, start with the six force-setup questions.

What to watch for

  • Choosing energy for an interval and forces at an instant
  • Distinguishing speed from velocity direction

Mechanics: connect projectile motion and energy

Separate horizontal and vertical motion for a launched ball, then use energy to find the speed of a spring-launched block.

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

1. A horizontal launch from a bench

A small ball leaves a horizontal bench at 3.0 m/s3.0\,\mathrm{m/s}, from a height of 1.25 m1.25\,\mathrm m. Ignore air resistance and use g=9.8 m/s2g=9.8\,\mathrm{m/s^2}. Find its flight time and horizontal range.

Show the explained solution
  1. The initial vertical velocity is zero. The vertical drop gives 1.25=12gt21.25=\tfrac12gt^2, hence t=2(1.25)/9.8≈0.505 st=\sqrt{2(1.25)/9.8}\approx0.505\,\mathrm s.
  2. Horizontal velocity stays constant, so R=vxt≈1.52 mR=v_xt\approx1.52\,\mathrm m.
  3. Horizontal speed does not appear in the flight-time equation for this fixed-height horizontal launch.

Review constant-acceleration equations and signs

2. Find speed without finding time

A 0.50 kg0.50\,\mathrm{kg} block is released from rest against an ideal spring compressed by 0.10 m0.10\,\mathrm m. The spring’s other end is fixed to a wall, and its constant is 200 N/m200\,\mathrm{N/m}. On a frictionless horizontal surface, find the block’s speed as the spring returns to its natural length.

Show the explained solution
  1. Let c=0.10 mc=0.10\,\mathrm m be the compression, k=200 N/mk=200\,\mathrm{N/m} the spring constant and m=0.50 kgm=0.50\,\mathrm{kg} the block’s mass. For the block–spring system, the initial spring energy becomes kinetic energy: 12kc2=12mv2.\tfrac12kc^2=\tfrac12mv^2.
  2. Take the nonnegative root because the question asks for speed: v=ck/m=0.10200/0.50=2.0 m/s.v=c\sqrt{k/m}=0.10\sqrt{200/0.50}=2.0\,\mathrm{m/s}.
  3. The initial spring energy is 1.0 J1.0\,\mathrm J, matching the final kinetic energy. A constant-acceleration equation would fail because the spring force changes as it expands.

Review spring energy and energy conservation

Use your answers to plan your revision
  1. Separate components

    Give each direction its own initial velocity and acceleration; use the common time to connect them.

  2. Choose the system

    For energy, list initial and final stores and any work transferring energy across the system boundary.

Bring the point where you had to choose between motion equations, forces and energy. We can practise that decision with your current 203-SN1-RE review topics.

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Original Nablio practice, not an official examination.

Course topic sources

A pendulum: find speed before tension

A small mass m=0.50 kgm=0.50\,\mathrm{kg} hangs from a string of length L=0.80 mL=0.80\,\mathrm m. It is released from rest with the taut string at θ=60∘\theta=60^\circ to the downward vertical. Treat the mass as a single point, ignoring its size. The string has no mass and does not stretch; the pivot is fixed. Neglect air resistance and friction. Use gravitational acceleration g=9.8 m/s2g=9.8\,\mathrm{m/s^2}. Find the speed and the string tension as the mass passes through the lowest point. First decide which quantity an energy equation can find.

Show a hint

Find the vertical drop, then use conservation of mechanical energy. At the lowest point, the net force toward the pivot supplies the inward acceleration.

Show the reasoning
  1. 1. Find the vertical drop

    Let hh be the release height above the lowest point, in metres. The initial vertical distance below the pivot is Lcos⁡θL\cos\theta; at the bottom it is LL.

    h=L−Lcos⁡θh=L-L\cos\theta

    h=L(1−cos⁡θ)h=L(1-\cos\theta)

    h=(0.80 m)(1−cos⁡60∘)h=(0.80\,\mathrm m)(1-\cos60^\circ)

    h=(0.80 m)(1−0.50)h=(0.80\,\mathrm m)(1-0.50)

    h=0.40 mh=0.40\,\mathrm m

    Use the vertical height, not the distance travelled along the arc.

  2. 2. Use energy to find speed

    Let vv be the speed at the lowest point, in m/s\mathrm{m/s}. Choose zero gravitational potential energy at that point. With the mass and Earth as the energy system, the initial gravitational potential energy becomes kinetic energy. The string’s tension is perpendicular to motion and does no work.

    mgh=12mv2mgh=\frac12mv^2

    v2=2ghv^2=2gh

    v2=2(9.8)(0.40) m2/s2v^2=2(9.8)(0.40)\,\mathrm{m^2/s^2}

    v2=7.84 m2/s2v^2=7.84\,\mathrm{m^2/s^2}

    Taking the positive square root gives:

    v=2.8 m/sv=2.8\,\mathrm{m/s}

  3. 3. Change to a force equation at the bottom

    Let TT be the string tension in newtons. At the lowest point, draw TT upward toward the pivot and mgmg downward. The path is circular, so the inward acceleration is ar=v2La_r=\frac{v^2}{L}; the subscript rr denotes the radial direction. Here that direction is upward.

    ar=7.84 m2/s20.80 ma_r=\frac{7.84\,\mathrm{m^2/s^2}}{0.80\,\mathrm m}

    ar=9.8 m/s2a_r=9.8\,\mathrm{m/s^2}

    Even though the velocity is horizontal at this instant, its direction is changing.

  4. 4. Solve for tension

    Newton’s second law toward the pivot is:

    T−mg=mv2LT-mg=\frac{mv^2}{L}

    Thus:

    T=mg+mv2LT=mg+\frac{mv^2}{L}

    Calculate the two terms using SI values:

    mg=(0.50)(9.8) Nmg=(0.50)(9.8)\,\mathrm N

    mg=4.9 Nmg=4.9\,\mathrm N

    mv2L=(0.50)(7.84)0.80 N\frac{mv^2}{L}=\frac{(0.50)(7.84)}{0.80}\,\mathrm N

    mv2L=4.9 N\frac{mv^2}{L}=4.9\,\mathrm N

    T=4.9 N+4.9 NT=4.9\,\mathrm N+4.9\,\mathrm N

    T=9.8 NT=9.8\,\mathrm N

  5. 5. Explain why T=mgT=mg would fail

    The weight is 4.9 N4.9\,\mathrm N, so tension is twice the weight here. If TT equalled mgmg, the net inward force would be zero, which would not keep this moving mass on its circular path. Tension can do zero work while still changing the direction of velocity.

A 0.80 m pendulum is released at 60° to the downward vertical, with a 0.40 m vertical drop. In the separate force diagram at the lowest point, T = 9.8 N upward and mg = 4.9 N downward.
The same mass is shown at release and at the lowest point. The 60° angle is measured from the downward vertical; h is the vertical drop. The separate force diagram is for the lowest point: T’s arrow is twice as long as mg’s.

Change the length, keep the release angle

Use the same mass and release angle, but replace the string with one of length 1.60 m1.60\,\mathrm m. Keep the same assumptions. Predict whether the speed and the tension at the lowest point increase, decrease or stay the same, then check your prediction.

Check your answer
  1. Find what changes in the energy calculation

    The height doubles:

    h=(1.60 m)(1−cos⁡60∘)\begin{gathered}h=\\(1.60\,\mathrm m)(1-\cos60^\circ)\end{gathered}

    h=0.80 mh=0.80\,\mathrm m

    v2=2ghv^2=2gh

    v2=15.68 m2/s2v^2=15.68\,\mathrm{m^2/s^2}

    v≈4.0 m/sv\approx4.0\,\mathrm{m/s}

    The speed increases by a factor of 2\sqrt{2}, not by a factor of 2.

  2. Keep the radius in the force equation

    Both v2v^2 and LL have doubled, so:

    v2L=15.68 m2/s21.60 m\frac{v^2}{L}=\frac{15.68\,\mathrm{m^2/s^2}}{1.60\,\mathrm m}

    v2L=9.8 m/s2\frac{v^2}{L}=9.8\,\mathrm{m/s^2}

    The inward acceleration remains unchanged.

    T=(0.50)(9.8+9.8) NT=(0.50)(9.8+9.8)\,\mathrm N

    T=9.8 NT=9.8\,\mathrm N

    This is the same tension as before. A greater speed alone does not determine tension; the radius also matters.

Use the energy lesson to choose a system and a time interval. Use the force-diagram lesson to identify interactions before writing the equation at the lowest point.

How a tutor can help

A tutor can help you label the height on a sketch, explain why tension does no work and decide where to switch from an energy equation to a force equation. You can compare an attempted T=mgT=mg solution with the curved path, then try the longer-string check to see which quantities change.

Prepare for an assessment

Bring your current topic list and a practice question. You can start it with your tutor or review a solution you could not finish. For each practice problem, state the system, the interval and the unknown before choosing a law. Include a short explanation of why the method applies, then check units and the physical meaning of the answer.

Official course information

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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