W 7.8 FE/EIT: Circular motion graphs. (Section 8.3.2 and Hw 7.6). The following figure shows a NASA centrifuge that rotates a rigid arm A with a constant angular speed a relative to Earth (frame N). An astronaut (modeled as a particle Q) is rigidly strapped into the arm and moves at constant speed in a circle whose center N, is fixed in N. Radius of circle R = 10 m A's angular speed in N w = 2rad = rad 2 sec Form expressions and graph the quantities below. Form a. w. (measures of A's angu- lar acceleration, angular velocity, and angle, respectively). · 41 1.3 1.6 14 0 1 OF 04 82 0 = 2 1 a = = rad sec 05 1 05 1.5 1=8= 1 15 2 25 9 05 1 15 2 3 rad sec 7.9 Particle acopl 3 3.5 4 (radians). Use 0(t=0) = 0. 4 2.5 3 3.5 4 Forma, V, F (magnitudes of Q's acceleration and velocity in N and Q's position from N). Hint: Hw 7.6. 15 10 3 0 25 D 15 10 5 0 0 30 25 15 10 5 0 9 03 a = 0.5 1 0.5 V T 13 1 2 time (seconds) = F = R = 1.5 2 time (seconds) 2.5 15 2 2.5 m m S 3 3.5 meters 4 2.5 3 3.5 4 25 20 Form , , r (where r is the horizontally-right measure of magni- tudes of Q's position from No.). 15 10 Ï I= 3 0 -5 10 -15 -20 -25 0 16 12 4 -8 -12 -16 10 i 0 6 -6 -10 0.5 0.5 T= 0 0 0.5 1 1 1.5 1 Top view V 1.3 2 time (seconds) 25 1.3 R 2.5 2 time (seconds) 3 2 time (seconds) 25 3 3.5 (meters) 33 3 35 4 4
Angular Momentum
The momentum of an object is given by multiplying its mass and velocity. Momentum is a property of any object that moves with mass. The only difference between angular momentum and linear momentum is that angular momentum deals with moving or spinning objects. A moving particle's linear momentum can be thought of as a measure of its linear motion. The force is proportional to the rate of change of linear momentum. Angular momentum is always directly proportional to mass. In rotational motion, the concept of angular momentum is often used. Since it is a conserved quantity—the total angular momentum of a closed system remains constant—it is a significant quantity in physics. To understand the concept of angular momentum first we need to understand a rigid body and its movement, a position vector that is used to specify the position of particles in space. A rigid body possesses motion it may be linear or rotational. Rotational motion plays important role in angular momentum.
Moment of a Force
The idea of moments is an important concept in physics. It arises from the fact that distance often plays an important part in the interaction of, or in determining the impact of forces on bodies. Moments are often described by their order [first, second, or higher order] based on the power to which the distance has to be raised to understand the phenomenon. Of particular note are the second-order moment of mass (Moment of Inertia) and moments of force.
![W²=0
7.8 FE/EIT: Circular motion graphs. (Section 8.3.2 and Hw 7.6).
The following figure shows a NASA centrifuge that rotates a rigid arm A with a constant angular
Top view
An astronaut (modeled as a particle Q) is rigidly
strapped into the arm and moves at constant
speed in a circle whose center N, is fixed in N.
Radius of circle
R = 10 m
A's angular speed in N
W = 2 rad
4 sec
Form expressions and graph the quantities below.
1
Form a, w, e (measures of A's angu-
Forma, V, F (magnitudes of Q's
lar acceleration, angular velocity, and acceleration and velocity in N and Q's
position from No). Hint: Hw 7.6.
angle, respectively).
a = =
플
(.
0.6
0.4
0
18
1.6
12
1
0.8
0.6
0.4
0.2
0 6 =
6
5
2
0
0.5
1
W=
05
15
2
time (seconds)
0 =
rad
sec2
15 2 25
0.5 1 15 2
3
rad
sec
3
3.5
3.5
4
4
(radians). Use 0(t=0) = 0.
=
2 25 3 3.5 4
30
25
20
15
3
0
D
30
25
rad
2 sec
20
15
10
5
0
30
0
25
20
15
10
5
0
0
0.3
a
0.5
ŕ
0.5
1
V
1
1.5
1
2
time (seconds)
=
1.5
2.5
= R =
2.5
time (seconds)
3
m
S
1.5 2
time (seconds)
3.5
3
Can
4
3.5 4
meters
2.5 3 3.5
4
Form , , x (where is the
x
tudes of Q's position from N.).
horizontally-right measure of magni-
25
20
15
10
I
5
0
-5
-10
-15
-20
-25
0
16
12
8
-4
-12
0
10
8
6
7.9 Particle accelerator (with classical mechanics) (Section 8.3.1).
A particle moves along a curve (fixed to Earth) with velocity v = UT
and acceleration a = a + app, where 7 is tangent to the curve and
p is perpendicular. Determine the distances and elapsed time ty for
a particle to go from rest to 3y 106 m 11
Result
X =
-6
-10
0.5
x =
0
1
0.5
1.5
0.5 1 1.5
1
2
time (seconds)
2.5
2
time (seconds)
R
100
1.5 2
time (seconds)
3
3
3.5
1422
3.3
3
2.5
4
(meters)
3.5
A particle with a = 300 gs
takes 37 trips around
Earth's equator to reach
speed of light.
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