A. Space, time and motion
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A.1 Kinematics
• Describe motion using position, velocity and acceleration.
• Velocity is the rate of change of position, and acceleration is the rate of change of velocity.
• Change in position is the displacement.
• Distinguish distance and displacement.
• Distinguish instantaneous vs average speed, velocity and acceleration.
• Use SUVAT equations for uniform acceleration: s=(u+v)t/2; v=u+at; s=ut+1/2at^2; v^2=u^2+2as. • Apply only to uniformly accelerated motion.
• Motion with uniform and non-uniform acceleration.
• Resolve projectile motion into horizontal and vertical components when fluid resistance is absent.
• Describe effects on trajectory, flight time, velocity, acceleration, range and terminal speed.
A.2 Forces and momentum
• Newton’s three laws of motion.
• Forces as interactions between bodies.
• Forces acting on a body can be represented in a free-body diagram.
• Free-body diagrams can be analysed to find the resultant force on a system.
• Contact forces include normal, friction, tension, elastic restoring force, viscous drag and buoyancy.
• Normal force FN acts perpendicular to the contact surface.
• Friction acts parallel to contact. • Static: Ff <= μsFN; dynamic: Ff = μdFN.
• Tension.
• Elastic restoring force follows Hooke’s law: FH = -kx.
• Viscous drag on a small sphere: Fd = 6πηrv, opposite motion. • η is fluid viscosity, r sphere radius, v speed through fluid.
• Buoyancy from displaced fluid: Fb = ρVg.
• Know field forces: gravitational, electric and magnetic.
• Weight is gravitational force: Fg = mg.
• Electric force Fe.
• Magnetic force Fm.
• Linear momentum p=mv is conserved unless a resultant external force acts.
• Impulse from resultant external force: J = FΔt = Δp.
• The applied external impulse equals the change in momentum of the system.
• Use F=ma for constant mass; use F=Δp/Δt when mass changes.
• Elastic and inelastic collisions of two bodies.
• Explosions.
• Compare energy in elastic collisions, inelastic collisions and explosions.
• Centripetal acceleration is radial: a=v^2/r=ω^2r=4π^2r/T^2. • Direction is radially toward the centre of the circle.
• Circular motion is caused by a centripetal force acting perpendicular to the velocity.
• A centripetal force causes the body to change direction even if its magnitude of velocity may remain constant.
• Circular motion relation: v=2πr/T=ωr. • Use angular velocity ω and period T to link angular and linear descriptions.
A.3 Work, energy and power
A.3.1—Conservation of energy
• Principle of the conservation of energy.
A.3.2—Work as energy transfer
• Work done by a force is equivalent to a transfer of energy.
A.3.3—Sankey diagrams
• Energy transfers can be represented on a Sankey diagram.
A.3.4—Work by constant force
• Work by constant force along displacement: W = Fs cos θ.
A.3.5—Work-energy change
• Work done by the resultant force on a system is equal to the change in the energy of the system.
A.3.6—Mechanical energy
• Mechanical energy includes kinetic, gravitational potential and elastic potential energy.
A.3.7—Mechanical energy conservation
• Mechanical energy is conserved when friction/resistive forces are absent.
A.3.8—Mechanical energy transformations
• If mechanical energy is conserved, work transforms energy between mechanical forms. • Relevant forms: translational kinetic, near-Earth gravitational potential and elastic potential.
A.3.9—Kinetic energy
• Translational kinetic energy: Ek = 1/2mv^2 = p^2/2m.
A.3.10—Gravitational potential energy
• Near Earth, gravitational potential energy change: ΔEp = mgΔh.
A.3.11—Elastic potential energy
• Elastic potential energy: EH = 1/2k(Δx)^2.
A.3.12—Power
• Power is rate of work or energy transfer: P=ΔW/Δt=Fv.
A.3.13—Efficiency
• Efficiency: η=Eoutput/Einput=Poutput/Pinput.
A.3.14—Fuel energy density
• Energy density of the fuel sources.