Gravitational field strength at latitude

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SUMMARY

The discussion clarifies the distinction between gravitational force and apparent weight at latitude, specifically addressing the terms mg0 and mgθ. It establishes that mg0 represents the true weight of an object, while mgθ denotes the apparent weight influenced by centripetal force at latitude θ. The term gθ is accurately described as the gravitational field strength at latitude θ, which combines the gravitational component g0 with rotational effects. This terminology is consistent with the textbook "New Way PHYSICS for Advanced Level" used in the discussion.

PREREQUISITES
  • Understanding of gravitational force and weight concepts
  • Familiarity with centripetal force and its effects
  • Knowledge of gravitational field strength terminology
  • Basic physics principles related to latitude and Earth's rotation
NEXT STEPS
  • Research the mathematical derivation of gravitational field strength at different latitudes
  • Study the effects of Earth's rotation on apparent weight
  • Explore the differences between true weight and apparent weight in various contexts
  • Examine the implications of gravitational variations on satellite orbits
USEFUL FOR

Students of physics, educators teaching gravitational concepts, and anyone interested in the effects of latitude on weight measurements.

zohapmkoftid
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This figure is captured from my physics textbook and it is about the gravity at latitude

http://pix.gogobox.com.tw/out.php?i=567045_.JPG

I want to know the difference between mg0 and mg(theta). Which one is the weight of the object? Thank you!
 
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Looks to me like mg0 is the gravitational force on the object and mgθ is the apparent weight of the object at latitude θ. The apparent weight is the gravitational force minus the centripetal force. (If you hung an object from a string, the string would end up parallel to the apparent weight.)
 
Is gθ called 'apparent gravity'?
 
zohapmkoftid said:
Is gθ called 'apparent gravity'?
That's what I would call it, but it is also called the local value of g as a function of θ. It's somewhat a matter of semantics. What does your textbook call it? (What text are you using?)
 
It is a Hong Kong textbook called New Way PHYSICS for Advanced Level
In the book, gθ is called gravitational field strength at latitude θ
I think the author uses the wrong name
The gravitational field strength at latitude θ should be g0, right?

Here is the related page from my textbook
http://uploadpie.com/bHHsD
 
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zohapmkoftid said:
I think the author uses the wrong name
The gravitational field strength at latitude θ should be g0, right?
No, the author's terminology is reasonable. When they talk about 'gravitational field strength at latitude θ' they are lumping together the strictly gravitational component (g0) with the effect due to rotation. Think of it as the 'net' or 'apparent' gravitational field strength. (It is a bit confusing, but commonly done.)
 
gravity = g0
apparent gravity / gravity at latitude = gθ
weight = mg0
apparent weight = mgθ

I hope I don't understand wrongly

So when we measure our body weight, the reading of the balance = mgθ rather than mg0
 
zohapmkoftid said:
gravity = g0
apparent gravity / gravity at latitude = gθ
weight = mg0
apparent weight = mgθ

I hope I don't understand wrongly

So when we measure our body weight, the reading of the balance = mgθ rather than mg0
Looks good to me. (Of course, this is just a simple model of the Earth as a sphere, ignoring various complications.)
 

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