sect. 6-3: gravity near earth’s surface. g & the gravitational constant g
TRANSCRIPT
![Page 1: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/1.jpg)
Sect. 6-3: Gravity Near Earth’s Surface
![Page 2: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/2.jpg)
g & The Gravitational Constant G
![Page 3: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/3.jpg)
• Obviously, it’s very important to distinguish between G and g– They are obviously very different physical quantities!
G The Universal Gravitational ConstantIt is the same everywhere in the Universe!
G = 6.673 10-11 N∙m2/kg2
It ALWAYS has this value at every location anywhere
g The Acceleration Due to Gravityg = 9.80 m/s2 (approximately!) on Earth’s surface
g varies with location
G vs. g
![Page 4: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/4.jpg)
• Consider an object sitting on Earth’s surface:
mE = mass of Earth (say, known)
RE = radius of Earth (known).
Assume Earth is a uniform, perfect sphere.
m = mass of m (known)
• We defined the Weight of an object of mass m on or near the Earth’s surface as the Gravitational Force on m: FG = mg
• Newton’s Gravitation Law says that the Gravitational force on m is
Fg = G[(mmE)/(rE)2] • Setting these equal gives:
g = 9.8 m/s2
g in terms of Gm
ME
![Page 5: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/5.jpg)
m
ME
Knowing g = 9.8 m/s2 & the radius of the Earth rE, the mass of the Earth can be calculated:
Using the same process, we can
“Weigh” Earth! (Determine it’s mass).
On the surface of the Earth, equate the usual weight of mass m to the Newtonian
Gravitation Force Law form.
![Page 6: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/6.jpg)
Effective Acceleration Due to Gravity• Acceleration due to gravity at a
distance r from Earth’s center.• Write the gravitational force as:
FG = G[(mME)/r2] mg
(effective weight)
g effective acceleration
due to gravity.
SO : g = G (ME)/r2
![Page 7: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/7.jpg)
• If an object is some distance h above the Earth’s surface,
r becomes RE + hAgain, set the gravitational force equal to mg:
G[(mME)/r2] mg This gives:
• This shows that g decreases with increasing altitude• As r , the weight of the object approaches zero• Example 6-4, g on Mt. Everest
2E
E
GMg
R h
Altitude Dependence of g
![Page 8: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/8.jpg)
Altitude Dependence of g
Lubbock, TX: Altitude: h 3300 ft 1100
m g 9.798 m/s2
Mt. Everest: g on Altitude: h 8.8 km
g 9.77 m/s2
2E
E
GMg
R h
![Page 9: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/9.jpg)
Example 6-5: Effect of Earth’s rotation on g
Assuming Earth is perfect sphere, determine how Earth’s rotation affects the value of g at equator compared to its value at pole.
![Page 10: Sect. 6-3: Gravity Near Earth’s Surface. g & The Gravitational Constant G](https://reader036.vdocument.in/reader036/viewer/2022062301/5697c0271a28abf838cd6191/html5/thumbnails/10.jpg)
Example 6-5: Effect of Earth’s rotation on g
Assuming Earth is perfect sphere, determine how Earth’s rotation affects the value of g at equator compared to its value at pole is: (Taking towards the Earth’s center as the positive direction)
Newton’s 2nd Law: ∑F = ma = mg – W
W = mg – ma = “effective weight”
At the poles, zero centripetal acceleration: a = 0 W = mg
At the equator, non-zero centripetal acceleration:
aR = [(v2)/(rE)] = W = mg - m[(v2)/(rE)] = mg
g = g - [(v2)/(rE)] = 0.037 m/s2
(v = (2πrE)/T = 4.64 102 m/s, T = 1 day = 8.64 104 s)