physics chapter 7.3 and 8
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Ch 7.3 and Ch 8TRANSCRIPT
Chapter 7.3 and 8
Circular and Planetary Motion
Rotational Inertia The resistance of an object to changes in its
rotational motion. Question: Which way is easier to balance? Question: Which easier to rotate? Rotational Inertia increases as you move the
mass away from the axis of rotation Example is a Baseball bat. Long Bat held near
the end has more rotational motion than one that is “choked up” Players are told to choke up in order to get the speed of the bat going.
Rotational Inertia An ice skater can spin around really fast by decreasing
their rotational axis. How do they do it? By pulling their arms in and thus increasing their
rotational speed. Here is our example: One of you will do this. This is exactly how you do flips in gymnastics and
cheerleading. Question: Why is the rotational inertia greater for a
gymnast when she’s swinging at full length or executing a somersault?
Question: Why do you hold your arms out to balance on a tight rope?
Question: Which can will roll down the incline faster? Beans or Juice?
Speed and Acceleration in a Circle
You can find the speed in a circle by the following formula.
V = 2πr / T
Centripetal Notes Centripetal means center seeking Centripetal acceleration – acceleration
towards the center of circleac = v2 / r
ac = 4π2r / T2
Centripetal Force – Force that is directed towards the center; it allows an object to follow a circular path
Fc = m ac
Scientists
Tycho Brahe – believed in an earth centered universe
Johannes Kepler – believed in a sun centered universe
Kepler’s Laws of Planetary Motion
1. The paths of the planets are ellipses with the center of the sun at one focus.
2. An imaginary line from the sun sweeps out equal areas in equal time intervals. Thus, the planets move fastest when closest to the sun.
3. Ratio of the squares of the periods of any two planets revolving about the sun is equal to the ratio of the cubes of their average distance from the sun.
Formula for Kepler’s Laws
T2
T1
=
2
r1
r2
3
Newton’s Universal Law of Gravitation
States that the attractive force between two objects is directly proportional to the product of the masses and inversely proportional to the square of the distance between the objects centers.
Law of Gravitation
F = G (m1) (m2) / d2
F = Force in NewtonsG = Gravitational ConstantM = mass in kgD = distance in meters
Henry Cavendish found the value of G
G = 6.67 x 10 -11 Nm2/kg2
Satellite Motion
How do satellites stay in orbit? By the amount of speed, satellites
are always falling. They have enough speed to outrun
the curvature of the earth. V2 = GMo/ro
Newton’s Variation of Kepler’s Third Law
T2 = 4 π2 ro3 / G Mo
Orbital radius for a satellite is:
ro = rp + h
Newton’s Variation of Kepler’s Third Law (Derivation)
m v2 / r = G m M / r2 & v = 2 π r / T
v2 / r = G M / r2 canceling m
4 π2 r2 / T2 r = G M / r2 plug in for v
G M T2 r = 4 π2 r4 cross multiply
T2 = 4 π2 r3 / G M solve for T
Satellite orbits
http://science.nasa.gov/Realtime/jtrack/3d/JTrack3D.html
Gravitational Fields
Michael Faraday came up with the concept that a “field” is required for a magnet to attract an object.
This concept was later applied to the “gravitational fields”. Anything with mass has a gravitational field
Gravitational Fields
g = F / m
g = N/kg (units)
Use these units for gravity not near the
surface of a planet (gravitational field)
Determining the gravity of a planet
mg = G m Mp / rp2
g = G Mp / rp2
What is the gravity on your planet? How much does a 980N adult
weigh on your planet?
Weightlessness
Caused when an object is in freefall
Other Gravity Scientist
Galileo Galilei - Discovered gravity makes things fall at the same rate if not affected by air resistance
Other Gravity Scientist
Albert Einstein - Developed theories of general and special relativity and showed that mass curves space. Black holes are so massive that light will not escape the space they curve.