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Outline Kinetics (external) – Forces in human motion – Impulse-momentum – Mechanical work, power, & energy – Locomotion Energetics
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Outline Kinetics – Forces in human motion Gravity Ground reaction Inertial (F = ma) Centripetal Friction Fluid Resistance – Multi force Free body diagrams Dynamic and Static Analysis with Newton’s Laws
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Reading Newton’s Laws – Ch 2: pages 41-44; 46-61 Friction – Ch 2: pages 61-62 Static/Dynamic Analyses & FBDs – Ch 3: pages 107-124 Fluid Resistance – Ch 2: pages 63-68 Linear Impulse/Momentum – Ch 2: pages 68-72 Mechanical Energy/Work/Power – Ch 2: pages 81-90 Applications (Locomotion, Jumping) – Ch 4: pages 145-159
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Human movements where fluid resistance is important?
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Factors affecting fluid resistance Density – mass per unit volume – resistance to motion through a fluid increases with density Viscosity – a measure of the fluid’s resistance to flow
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Figure 2.20 Components of Fluid Resistance Drag Force: Opposes motion Lift Force: perpendicular to motion
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Components of drag force Surface drag: friction of fluid rubbing on surface Pressure drag: front-back pressure differential Wave drag: waves at interface of two fluids.
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Streamlines Drag force is effected by: 1) different velocities of the streamlines 2) the extent to which the relative motion of the streamlines is disturbed
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Laminar flow Uniform layers of different speed Slowest layer closest to the surface of the object
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Air direction relative to ball Velocity of air Laminar flow: Surface drag dominates
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Surface drag also called skin friction Depends on – velocity of fluid relative to surface – roughness of surface – surface area of object – properties of fluid
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Reducing surface drag Speed skater: wearing a smooth spandex suit – 10% less surface drag than wool clothes Cyclist: wearing Lycra long sleeved shirt, tights, and shoe covers Swimmer: Shaving body hair
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Surface drag Surface drag: Friction within boundary layer – human movement in air: surface drag (3-5%) – small compared to pressure drag (95-97%)
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Pressure drag: dominant form of drag in human movement Turbulent flow: Non-uniform flow of fluid around an object Pressure differential causes a “pressure drag force”. Higher Pressure Lower Pressure
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Streamlining reduces turbulence and pressure drag Flow remains laminar for longer -- less turbulence – less pressure drag Enoka, Figure 2.3A
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Pressure drag vs. surface drag Pressure drag: dominates for large objects moving in low density & viscosity fluids – e.g., human running, cycling in air Surface drag: dominates when small objects moving in high viscosity fluids, e.g. sperm swimming
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Pressure drag force F d = (0.5 C D )Av 2 = fluid density – air: 1.2 kg/m 3 – water: 1000 kg/m 3 C D = coefficient of drag A = projected area (m 2, frontal area as object moves through the fluid) v = velocity of the fluid relative to the object (m/s)
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Coefficient of drag (C D ): combines shape & aspect ratio index Unitless Magnitude depends on – shape of object – orientation of object relative to fluid flow Independent of size Streamlining reduces C D
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Coefficient of drag examples Mackerel: 0.0053 Rainbow trout: 0.15 Pigeon or vulture: 0.4 Sphere: 0.47 Human swimmer: 0.66 Cyclist and bike: 0.9 Runner: 0.9 Flat plate: 1.0
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How can we measure frontal area?
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Velocity (v) of fluid relative to the object Example: v cyclist = 7 m/s Still air: v air = 0 Headwind: v air = 7 m/s Tailwind: v air = 7 m/s v object v = v object - v air
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Velocity (v) of fluid relative to the object Example: v cyclist = 7 m/s Still air: v air = 0 v = 7 m/s Headwind: v air = -7 m/s v = 14 m/s Tailwind: v air = 7 m/s v = 0 m/s v object v air v = v object - v air
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Components of drag force Surface drag: friction of fluid rubbing on surface Pressure drag: front-back pressure differential Wave drag: waves at interface of two fluids.
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Figure 2.20 Components of Fluid Resistance Drag Force: Opposes motion Lift Force: perpendicular to motion
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Lift Force Asymmetric objects Spinning object Bernoulli’s Principle: Pressure is inversely proportional to the velocity of the fluid
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Low Velocity High Pressure High Velocity Low Pressure
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Figure 2.22
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Drag acts in horizontal (x) direction, opposite to the direction of locomotion Drag
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Drag in locomotion ( F d = 0.5 C D Av 2 ) Walking or running in air (C D = 0.9, = 1.2 kg/m 3 ) – 0.5 C D = 0.55 kg/m 3 – F d = 0.55Av 2 Frontal area (A) = 0.4 m 2 – F d (Newtons) = 0.22 * v 2
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Role of F d in locomotion Person in still air – Walk (1.25 m/s): F d ~ 0.001 F g,x – Run (4 m/s): F d ~ 0.01 F g,x – Run (8 m/s): F d ~ 0.025 F g,x Person in headwind of 17 m/s (~ 35 mph) – Run (8 m/s): F d ~ 0.25 F g,x
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Role of F d in locomotion
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Drag in cycling ( F d = 0.5 C D Av 2 ) For cyclist in air (C D = 0.9, = 1.2 kg/m 3 ) – 0.5 C D = 0.55 kg/m 3 – F d = 0.55Av 2 Frontal area (A) of cyclist & bike – Touring position (upright): 0.5 m 2 – Racing position: 0.3 m 2 – Recumbent position: 0.2 m 2
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Touring Racer Recumbent Cycling
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Swimming Water density >> air density – greater pressure drag F d = 0.5 C D Av 2 – = 1000 kg/m 3 – C D = 0.66 – A = 0.073 m 2 F d (swimming) = 24* v 2 – Comparison: F d (walk, run) = 0.22 * v 2
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Drag: walking vs. swimming Drag force comparison at a given speed – F d (swimming) ~ 100 x > F d (walk, run in air) Reasons – Water density >> air density – frontal area less – Cd less for swimming position
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Total force: walking vs. swimming Swimming – Drag: largest force – 2 m/s ---> F d ~ 0.14 * body weight Walking – Ground reaction force: largest force – 2 m/s ---> F g ~ 1.5 * body weight
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Figure 2.23
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Figure 2.24
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Problem: Friction force on slope FnFn mg Find maximum friction force in terms of mg, , & µ s.
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Friction force on slope F s,max = F n µ s F n = mg cos F s,max = µ s mg cos F parallel (force pulling downhill parallel to slope) = mg sin FnFn mg
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Friction vs. Gravity force parallel m=70kg µ s = 0.5 theta = 30 degrees Solve for static friction force and the component of gravitational force pulling parallel to the slope.
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Recitation a skier starts at the top of a 30 degree incline,init. vel. = 0 considering gravity, air resist. & friction, draw a FBD.
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a skier starts at the top of a 30 degree incline,init. vel. = 0 considering gravity, air resist. & friction, draw a FBD If = 0.050 and mass is 70.0kg, what is max. frictional force? add that number to FBD Recitation
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If frontal area is 0.600 m^2, air density is 1.200 kg/m^3, Cd is 0.9, what is air resist force when velocity = 10 m/sec add this # value to your FBD Recitation
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if we include air resistance, kinematic problems get more difficult. In the bike lab we will take aero force into account and use an iterative computer approach. Neglect or Do Not Neglect?
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What is the fastest velocity that can be reached by the skier. i.e. what is terminal velocity? Recitation
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