Download Forces and COM - K

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Machine (mechanical) wikipedia , lookup

Fictitious force wikipedia , lookup

Momentum wikipedia , lookup

Specific impulse wikipedia , lookup

Centrifugal force wikipedia , lookup

Force wikipedia , lookup

Rigid body dynamics wikipedia , lookup

Newton's laws of motion wikipedia , lookup

Centripetal force wikipedia , lookup

Classical central-force problem wikipedia , lookup

Work (physics) wikipedia , lookup

Transcript
Classification of Forces
•
•
•
•
Action vs reaction
Internal vs external
Motive vs resistive
Force resolution – horizontal and vertical
components
• Simultaneous application of forces - vector
summation
Types of external forces encountered by
humans
• Gravitational force (weight = mg)
• Ground Reaction Force (GRF)
– Vertical
– Horizontal (frictional)
•
•
•
•
•
Frictional force (coefficient of friction)
Elastic force (coefficient of restitution)
2
Centripetal force (mv /r)
Buoyant force
Free body diagram - force graph
Force Plates –
Measurement of ground
reaction forces
While walking
Cfr = Frf /Nof
Coefficient of restitution – Relative
velocity before and after impact:
Coefficient of restitution – drop
test
Centripetal &
Centrifugal forces
2
Cf = mv /r
Buoyant Force = weight of water displaced by a
body. If weight of water displaced by your body
is more than your body, then you will float. Your
body will only sink down to the point where Wt = Bf
Buoyant force = wt
of water displaced
Will this person float?
Rotate?
How can you tell?
Free body diagrams:
Free body diagrams
Force and Motion Relationships
• Instantaneous Effect of force on motion is
to accelerate the object: F=ma
• Force applied through a distance: workenergy relationship
• Force applied through a time: impulsemomentum relationship
Instantaneous Effect of Force on
an Object
• Remember the concept of net force?
• Need to combine, or add forces, to
determine net force
• Newton’s third law of motion (F = ma)
• Inverse dynamics – estimating net forces
from the acceleration of an object
• Illustrations from Kreighbaum: Figures F.4,
F.5, and F.6 (pp 283-284)
Vector Resolution Problems
• Projectile motion situations
– Find horizontal velocity
– Find vertical velocity
• Friction problems
– Find horizontal force component (Friction)
– Find vertical component (Normal)
• First step in adding, or combining vectors
– When more than one force is acting on an object
– When adding velocity vectors
Vector resolution:
Vert comp = F•sin•Θ
Horiz comp = F•cos•Θ
Θ
Θ
Vert comp = F•sinΘ
Horiz comp = F•cosΘ
Θ
Θ
d
Θ
Turning comp = F•d•sinΘ
Radial comp = F•d•cosΘ
(d = d•sinθ)
Vector Addition Problems
• Combining forces
– Net effect of two forces applied to any object
– What is maximum safe speed for a curve?
• Centrifugal force, frictional force, & gravity
– What makes a spitball work?
• Wind force and weight
• Combining velocities
– In crossing a river, what direction is best?
• Velocity of water and swimmer
– In aviation, correcting for wind
• air speed and ground speed
Sum of two forces:
Sum of two velocities:
(May be deleted if your calculator provides
resultant angle in a 0-360 deg system)
Force Applied Through a Time:
Impulse-Momentum Relationship
•
•
•
•
Force applied through a time
Impulse - the area under the force-time curve
Momentum - total amount of movement (mass x velocity)
An impulse applied to an object will cause a change in its
momentum (Ft = mv)
• Conservation of momentum (collisions, or impacts)
– in a closed system, momentum will not change
– what is a closed system?
Impulse: area
under forcetime curve
Impulse produces
a change in
momentum (mV)
Vertical
impulse
While
Running:
Area under
Force-time
curve
Anterioposterior
(frictional)
component
of GRF: impulse
Is area under
Force-time curve
Positive and
Negative impulse
Are equal if
Horizontal comp
Of velocity is
constant
Conservation of momentum: when net impulse is zero
(i.e. the system is closed), momentum does not change
Conservation of momentum: is this a closed system?
Force Applied Through a Distance: Work,
Power, Energy
• Work - force X distance (Newton-meters, or Joules)
– On a bicycle: Work = F (2r X N)
– On a treadmill: Work = Weightd X per cent grade
• Power - work rate, or combination of strength and
speed (Newton-meters/second, or watts)
– On a treadmill: P = Weightd X per cent grade/ time
– On a bicycle: P = F (2r X N) / time
• What about kilogram-meters/min?
• Energy - capacity to do work
– kinetic, the energy by virtue of movement (KE = 1/2 mv2 )
– gravitational potential, energy of position (PE = Weight x
height)
– elastic potential, or strain, energy of condition (PE = Fd)
Work while pedaling on bicycle:
From McArdle and Katch.
Exercise Physiology
Work while running on treadmill:
From McArdle and Katch. Exercise Physiology
Note that %grade = tan θ X 100,
and tan θ and sin θ are very
similar below 20% grade
Calculating Power on a Treadmill
• Problem: What is workload (power) of a 100 kg
man running on a treadmill at 10% grade at 4 m/s?
• Solution:
– Power = force x velocity
– Force is simply body weight, or 100 x 9.8 = 980 N
– Velocity is vertical velocity, or rate of climbing
• Rate of climbing = treadmill speed x percent grade = 4 m/s x .1 = .4 m/s
– Workload, workrate, or power = 980N X .4 m/s = 392 Watts
• Note: 4 m/s = 9 mph, or a 6 min, 40 sec mile
• Problem:
Calculate your workload if you are running on
a treadmill set at 5% grade and 5 m/s.
– Answer for 200 lb wt is: 223 Watts
Power running up stairs:
Work rate = (weight X vertical dist) ÷ time
Conservation of Energy
• In some situations, total amount of mechanical energy
(potential + kinetic) does not change
– Stored elastic energy converted to kinetic energy
•
•
•
•
diving board
bow (archery)
bending of pole in pole vault
landing on an elastic object (trampoline)
– Gravitational potential energy converted to kinetic energy
• Falling objects
Energy conservation – Case I : elastic potential (strain) and kinetic
Potential energy (FD) +
Kinetic energy (1/2mv2)
remains constant
Energy conservation – Case II : gravitational potential and kinetic
Potential energy
(Wh) + kinetic
energy (1/2mv2)
remains constant
Linear Kinetics Formulae