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Exam code:9FM0

Problem solving with energy

How do I include air resistance in the work-energy principle?

  • The work done by a constant air resistance / drag force, DNewtons, when moving x metres is D x Joules

  • Air resistance hinders (slows down) the particle, so is negative in the work-energy principle

    • total final energy = total initial energy – work done by air resistance

  • This can work for particles moving horizontally or vertically

    • sometimes the air resistance experienced upwards has a different value to that experienced downwards

  • Air resistances, in reality, are often proportional to the speed (or square of the speed) of the particle

    • but this makes it a non-constant force

      • and the work done formula only works for constant forces

How do I use the work-energy principle on curved surfaces?

  • The work-energy principle can be used in new situations that aren’t always inclined planes!

  • e.g. skateboarding down a curving slope

    • the skater may put in their own work done (e.g. using their legs) which “helps” to go faster (+ work done)

    • but there may be a constant resistive force acting against them throughout (- work done)

      • assume that the resistances are always parallel to the curved slope at any given time (and reactions are always perpendicular)

How do I apply the work-energy principle to connected particles?

  • You can still use the work-energy principle with connected particles by considering it all as one object

    • total final energy = total initial energy ± work done

  • The total energies will be the sum of the GPEs and KEs of all particles

  • There will be a combination of “work done” terms with + or – depending on whether it’s helping or hindering its respective particle

    • e.g. for a driving car pulling a trailer, the terms look like:

    • + WD(by driving force on car) – WD(by tension in towbar on car) – WD(by resistances on car) + WD(by tension from towbar on trailer) – WD(resistances on trailer)

      • Notice that the work done by the tensions will cancel each other out

How do I apply the work-energy principle to collisions?

  • Some questions use the work-energy principle and the theory of collisions

  • There may be a particle projected into a perpendicular wall

    • Use the Work-Energy Principle to find the speed with which it impacts the wall

      • You can find the speed by making the kinetic energy the subject

    • This gives the speed of impact

    • To find the speed of rebound, calculate “e” × the speed of impact

      • “e” is the coefficient of restitution

  • Other questions may have two spheres colliding on a horizontal table, then one falling off

    • Use conservation of momentum and Newton’s law of restitution to find velocities after the collision

    • When the sphere rolls off the table, it becomes a projectile (projected horizontally with it’s new velocity)

      • If you know the height of the table, you can use the Work-Energy Principle to find the speed of impact with the ground 

Examiner Tips and Tricks

  • It is common for harder energy questions to be fully algebraic

    • look out for masses, m, cancelling in the working

Worked Example

A particle of mass m kg is projected vertically upwards from ground level at a speed of 5 square root of g H end root ms-1, where H is the vertical height in metres between the ground and the ceiling. The particle is subjected to a constant air resistance force of 1 fourth m g N, opposing its motion. The coefficient of restitution between the particle and the ceiling is fraction numerator square root of 2 over denominator 3 end fraction.
Find, in terms of g and H, the exact speed of the ball immediately after rebounding with the ceiling.

worked example focusing on problem solving aspects of energy questions, utilising algebraic terms
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