jumping, flying and swimming

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Jumping, flying and swimming Movement in “fluids”

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Jumping, flying and swimming. Movement in “fluids”. Aim. jumping gliding powered flight insects birds drag and thrust in swimming. References. Schmidt - Nielsen K (1997) Animal physiology McNeill Alexander R (1995) CD Rom How Animals move Journals & Web links: see: - PowerPoint PPT Presentation

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Page 1: Jumping, flying and swimming

Jumping, flying and swimming

Movement in “fluids”

Page 2: Jumping, flying and swimming

Aim jumping gliding powered flight

insects birds

drag and thrust in swimming

Page 3: Jumping, flying and swimming

References Schmidt - Nielsen K (1997) Animal

physiology McNeill Alexander R (1995) CD Rom

How Animals move Journals & Web links: see:

http://biolpc22.york.ac.uk/404/

First: What limits jumping ?

Page 4: Jumping, flying and swimming

Jumping What limits how far we can jump? At take off have all energy stored as KE conversion of kinetic energy to

potential (gravitational) energy KE = ½ m v2

PE = mgh

Page 5: Jumping, flying and swimming

How high depends on KE at take off PE = KE therefore

mgh = ½ mv²

gh = ½ v² therefore h = ½ v2/g

no effect of mass on how high you jump neglects air resistance

Page 6: Jumping, flying and swimming

constant acceleration due to constant gravity not affected by mass

jumping in a parabola depends on take off angle d = (v² sin 2) /g

jumpingangle.xls maximum at 45o

Sin 90 = 1 d = v2/g

twice as far as the max height

How far do we go?

Jumping

0

0.02

0.04

0.06

0.08

0.1

0.12

0 0.05 0.1 0.15 0.2 0.25 0.3

distance (m)

hei

gh

t (m

)

Page 7: Jumping, flying and swimming

How far as before distance not affected

by body mass

Alice Daddy

age 8 ??

mass 35kg 87kg

distance 1.16m ??

Page 8: Jumping, flying and swimming

Great locust jumping test

http://biolpc22.york.ac.uk/404/practicals/locust_jump.xls

Page 9: Jumping, flying and swimming

Jumping in locusts If we could jump

as well, we could go over the Empire state building max up is ½

horizontal distance

elastic energy storage

co-contraction

Page 10: Jumping, flying and swimming

How long to take off? depends on leg length

time to generate force is 2s/v for long jump, time = 2s/(g*d)

s is leg length, d is distance jumped

bushbaby 0.05 to 0.1s frog 0.06s flea 1 ms locust ??

Page 11: Jumping, flying and swimming

Running jump much higher/further KE can be stored in

tendons and returned during leap

Page 12: Jumping, flying and swimming

Summary so far Jumping is energetically demanding muscle mass : body mass is most

important store energy in tendons if possible

Now onto: how do we fly?

Page 13: Jumping, flying and swimming

Flying gliding power flight hovering

How stay up? Can nature do better than mankind?

Page 14: Jumping, flying and swimming

Who flies? birds insects bats pterosaurs

Page 15: Jumping, flying and swimming

Lift why don’t birds fall due to gravity? where does lift come from?

speed up air Bernoulli’s Principle Total energy =

pressure potential energy + gravitational potential energy + kinetic energy of fluid

Page 16: Jumping, flying and swimming

How does air speed up? air slows down underneath

because wing is an obstacle air speeds up above wing

fixed amount of energy

Page 17: Jumping, flying and swimming

Lift and vortices faster /slower

airflow =circulation extends above /

below for length of wing

creates wake

Page 18: Jumping, flying and swimming

Circulation circulation vortex

shed at wingtips

Page 19: Jumping, flying and swimming

So to fly… we need to move through the air use PE to glide down

as go down, PE changed to KE use wings to force a forwards

movement

Page 20: Jumping, flying and swimming

Can nature beat man?

Page 21: Jumping, flying and swimming

Gliding soaring in thermals

Africa: thermals rise at 2-5m/s

soaring at sea/by cliffs

Page 22: Jumping, flying and swimming

Summary so far Jumping is energetically demanding

muscle mass : body mass is most important

store energy in tendons if possible Flying involves generating lift gliding

use PE to get KE to get speed to get lift

Page 23: Jumping, flying and swimming

Flapping flight large birds fly continuously

down stroke air driven down and back up stroke

angle of attack altered

air driven down and forwards

continuous vortex wake

Page 24: Jumping, flying and swimming

Discontinuous lift small birds with rounded wings lift only on downstroke vortex ring wake

Page 25: Jumping, flying and swimming

Summary Jumping is energetically demanding

muscle mass : body mass is most important

store energy in tendons if possible

Birds heavier than air Flying involves generating lift

gliding use PE to get KE to get speed to get lift

flapping propels air

Page 26: Jumping, flying and swimming

Insect flight flexibility of wings allows extra

opportunities to generate lift

rotation of wing increases circulation

Page 27: Jumping, flying and swimming

Insect flight flexibility of wings

allows extra opportunities to generate lift

fast flight of bee downstroke

upward lift upstroke

lift

move wingbee

Page 28: Jumping, flying and swimming

Clap and fling at top of upstroke two wings “fuse”

unconventional aerodynamics extra circulation extra force

Page 29: Jumping, flying and swimming

Wake capture wings can interact with the last vortex

in the wake to catch extra lift

first beat second beat

Page 30: Jumping, flying and swimming

Summary so far Jumping is energetically demanding

muscle mass : body mass is most important store energy in tendons if possible

Flying involves generating lift gliding

use PE to get KE to get speed to get lift flapping propels air insects often have unconventional

aerodynamics – can beat the “laws” of physics

Next… Swimming

Page 31: Jumping, flying and swimming

Jet propulsion conservation of momentum = m*v mass of fish * velocity of fish

= mass of water * velocity of water squid

contract mantle dragonfly larvae

Page 32: Jumping, flying and swimming

Paddling / rowing depends on

conservation of momentum ducks frogs

swimming beetles

Page 33: Jumping, flying and swimming

Drag

Reynolds number gives an estimate of drag Re = length * speed * density / viscosity

for air, density / viscosity = 7*104 s / m2

for water; density/ viscosity = 106 s/m2

friction

turbulence

Page 34: Jumping, flying and swimming

Reynolds number Re < 1 no wake

e.g. protozoan Re < 106 flow is

laminar e.g. beetle

Re > 106 flow is turbulent e.g. dolphin

Drag depends on shape Drag reduced by up to

65% by mucus

Page 35: Jumping, flying and swimming

Design for minimal drag tuna or swordfish:

highly efficient for high-speed cruising in calm water

torpedo-shaped body narrow caudal

peduncle lunate, rigid

fins

Page 36: Jumping, flying and swimming

Why don't all fish look like that?

The design is highly inefficient: In naturally turbulent water (streams,

tidal rips, etc.) for acceleration from stationary for turning for moving slowly & especially for lying still

Page 37: Jumping, flying and swimming

Ambush predators keep head still

long body/dorsal fins rapid start

flexible body, plenty of muscle large tail fin

barracuda pike

Page 38: Jumping, flying and swimming

Design for manoeuvrability

Small items don't move fast, but require delicate, focused movements for capture.

A short, rounded body with sculling or undulating fins.

Compressing the body laterally provides a wide surface to exert force on the water

Page 39: Jumping, flying and swimming

Optimal design?

Minimise drag often in biomechanics

No one optimal design efficient energetics isn’t all maximum speed isn’t all use drag on oars to achieve efficient

propulsion

Page 40: Jumping, flying and swimming

How does a fish move? undulations from front to back

Page 41: Jumping, flying and swimming

How is thrust generated? thrust = momentum / time anguilliform

Page 42: Jumping, flying and swimming

How else is thrust generated?

tail movement Carangiform

tail generates symmetric vortex street

noterotation

Page 43: Jumping, flying and swimming

How else is thrust generated?

tail movement acts like a hydrofoil thunniform cetaceans penguins

Page 44: Jumping, flying and swimming

Flying not swimming tail movement acts like a hydrofoil generates lift and drag

drag acts in line of motion lift acts perpendicular (normal) to drag

draglifttotal

Page 45: Jumping, flying and swimming

Summary Jumping is energetically demanding

store energy in tendons if possible Flying involves generating lift

accelerate air to get lift Insects are small enough to have

unconventional aerodynamics Minimisation of drag Adaptation to environment leads to

alternate solutions of best way to swim