Torque. Correlation between Linear Momentum and Angular Momentum Resistance to change in motion:...
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Torque. Correlation between Linear Momentum and Angular Momentum Resistance to change in motion: Linear behavior: Inertia Units M (mass), in kg Angular
Correlation between Linear Momentum and Angular Momentum
Resistance to change in motion: Linear behavior: Inertia Units M
(mass), in kg Angular Rotational Inerita, Symbol I aka Moment of
Inertia Has to do with more than just mass, it includes the shape
of the object. If x cm is far away, I is bigger. Based on mass and
mass distribution.
Slide 3
Three Important equations for I : Thin Walled Cylinder I = MR 2
(also valid for an orbiting body) Solid Cylinder I = (1/2)MR 2
(easier because the mass is not so far away) Sphere I = (2/5)MR 2
(marble)
Slide 4
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Cause of acceleration Linear Force (Newtons) Angular Torque (
Nm)
Slide 6
Momentum Linear p = mv ( units kgm/s) Angular L = I (units kgm
2 /s) Bigger mass = harder to stop Faster moving = harder to
stop
Slide 7
Kinetic Energy Linear K = (1/2) mv 2 (Units Joules) Angular K R
= (1/2) I 2 A rolling ball has translational and rotational Kinetic
energy. Remember: ms become Is, vs become s
Slide 8
Pivoting Object Take a shape and a piece of paper. Label an x-y
axis on the paper. Label pivot point on the shape. Place at origin.
Label x cm on shape. Draw weight vector. Draw position vector r
from pivot to x cm. Move position vector from origin to x cm.
Slide 9
Definition: torque Torque is the cause of angular acceleration
in the same way that force is the cause of linear acceleration.
Symbol (pronounced tao) is the cross product between r and F We say
= r cross F = r x F
Slide 10
Relationship between torque and Newtons second law F = ma rF =
rma a is tangential, so a =r rF = torque, = rmr = mr 2 = I ( I=m 1
r 1 2 = m 2 r 2 2 ) So = I ( must be in rad/s 2 )
Slide 11
Back to picture Draw the angle between the FIRST r vector that
starts at the pivot point and the F vector. Then draw the angle
between the moved r vector and F. The moved vector is 180-. The old
r vector was at . = rF g sin(180-) Mathematically, sin(180-) = sin
So = rF g sin() in magnitude. Use RHR for direction.
Slide 12
On picture, Split weight vector out into components mgcos
points toward pivot, mgsin points perpendicular to make it rotate.
mgcos gets cancelled out, thats why we use the sin component, =
rFsin() That component in this case is spinning it cw, or in the
negative direction.
Slide 13
Lever arm Draw a line from pivot point across to weight vector
so that is crosses weight vector at 90 degrees. That line has a
magnitude of rsin This is very important. It has a special
definition. Its called a lever arm (symbol l ) We can say: = l
F
Slide 14
Cross Product Guided Practice #1 P = 4i + 2j k Q = -3i + 6j -2k
P x Q = Answer: 2i + 11j + 30k
Slide 15
Guided Practice #2 Cross Products P = 2.12i + 8.15j 4.28k N and
Q = 2.29i -8.93j 10.5k m Find P x Q Answer: -124i +12.5j 37.6k
Slide 16
Slide 17
Solution 1) O = 0.17 rad/s (v/r) 2) I = (2/5)MR 2 = 0.0144 kgm
2 3) = 1735 rad/s 4) = use quadratic to find time 5) t = 4.25
s
Slide 18
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Solution Find I I = MR 2 =.625 kgm 2 Find = 16 rad/s Find = =
800 rad = 127 rev
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