Exam code:9FM0
Problem solving with energy
How do I include air resistance in the work-energy principle?
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The work done by a constant air resistance / drag force,
Newtons, when moving
metres is
Joules
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Air resistance hinders (slows down) the particle, so is negative in the work-energy principle
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total final energy = total initial energy – work done by air resistance
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This can work for particles moving horizontally or vertically
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sometimes the air resistance experienced upwards has a different value to that experienced downwards
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Air resistances, in reality, are often proportional to the speed (or square of the speed) of the particle
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but this makes it a non-constant force
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and the work done formula only works for constant forces
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How do I use the work-energy principle on curved surfaces?
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The work-energy principle can be used in new situations that aren’t always inclined planes!
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e.g. skateboarding down a curving slope
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the skater may put in their own work done (e.g. using their legs) which “helps” to go faster (+ work done)
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but there may be a constant resistive force acting against them throughout (- work done)
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assume that the resistances are always parallel to the curved slope at any given time (and reactions are always perpendicular)
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How do I apply the work-energy principle to connected particles?
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You can still use the work-energy principle with connected particles by considering it all as one object
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total final energy = total initial energy ± work done
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The total energies will be the sum of the GPEs and KEs of all particles
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There will be a combination of “work done” terms with + or – depending on whether it’s helping or hindering its respective particle
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e.g. for a driving car pulling a trailer, the terms look like:
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+ 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)
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Notice that the work done by the tensions will cancel each other out
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How do I apply the work-energy principle to collisions?
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Some questions use the work-energy principle and the theory of collisions
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There may be a particle projected into a perpendicular wall
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Use the Work-Energy Principle to find the speed with which it impacts the wall
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You can find the speed by making the kinetic energy the subject
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This gives the speed of impact
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To find the speed of rebound, calculate “e” × the speed of impact
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“e” is the coefficient of restitution
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Other questions may have two spheres colliding on a horizontal table, then one falling off
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Use conservation of momentum and Newton’s law of restitution to find velocities after the collision
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When the sphere rolls off the table, it becomes a projectile (projected horizontally with it’s new velocity)
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If you know the height of the table, you can use the Work-Energy Principle to find the speed of impact with the ground
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Examiner Tips and Tricks
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It is common for harder energy questions to be fully algebraic
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look out for masses,
, cancelling in the working
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Worked Example
A particle of mass kg is projected vertically upwards from ground level at a speed of
ms-1, where
is the vertical height in metres between the ground and the ceiling. The particle is subjected to a constant air resistance force of
N, opposing its motion. The coefficient of restitution between the particle and the ceiling is
.
Find, in terms of and
, the exact speed of the ball immediately after rebounding with the ceiling.

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