Different types of Forces (Gravitational and Normal forces)

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Discussion Overview

The discussion revolves around the concepts of gravitational and normal forces, exploring their definitions, relationships, and implications in various scenarios, including objects on ramps. Participants raise questions about the nature of gravitational force, the role of normal force, and the application of Newton's laws in these contexts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents the gravitational force equation and questions how it relates to the acceleration due to gravity, specifically asking how 9.8 N translates to 9.8 m/s².
  • Another participant challenges the notion of neglecting mass in gravitational calculations, emphasizing that gravitational force is dependent on mass and should be expressed in terms of acceleration.
  • Questions are raised about whether the force exerted by the Earth on a person is equal to the force exerted by the person on the Earth, and how differing masses affect the resulting accelerations.
  • Participants discuss the role of normal force in maintaining equilibrium for objects on surfaces, questioning what opposing forces are at play when an object is on a ramp.
  • There is a discussion about the forces acting on an object on a ramp, including the components of weight and how they relate to motion down the ramp.
  • One participant notes a common misconception regarding Newton's Third Law, suggesting that the focus on "equal" and "opposite" forces may lead to misunderstandings.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of gravitational force and normal force, with no consensus reached on certain aspects, particularly regarding the implications of Newton's Third Law and the nature of forces acting on objects in various scenarios.

Contextual Notes

Some participants highlight limitations in understanding the relationship between gravitational force and acceleration, as well as the complexities involved in analyzing forces on inclined planes. The discussion reflects varying interpretations of fundamental physics concepts.

tarunsworld20
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So to give a basic idea of where I am coming from:


F = G*m1*m2/r2

In the above equation, G is the gravitational constant of 6.67 x 10-11 Nm2/kg2

m1 = Mass of Earth
m2 = Mass of Human (which we neglect since it's very tiny compared to the mass of earth)

r = distance between human's center and Earth's center.

Plugging in numbers will result in a value of 9.8 N

Q # 1) Note, the units are N. How do you get 9.8 m/s2

Q # 2) So, if you wanted to be exact, the gravitational force exerted on each person is of a completely different value, because the mass of every individual varies, right?

9.8 N is the force between me and earth.
Now, according to Newton's third law, Force between two objects are equal on opposite.

Q # 3) So, if Earth's surface is pulling me down at approximately 9.8 N, then does this mean that, I am also pulling the Earth up at 9.8 N ? If so, since the masses of Earth and me are completely different, the acceleration at which Earth is pulling me down should be completely different from the acceleration at which I am pulling up the Earth right?

Q # 4) If I was exerting the same amount of gravitational force on the Earth as Earth was on me, then how is Normal Force playing a role in helping me to stay on the ground?

Whenever I look up stuff about Normal Force, the example I get is, think of an object on a ramp. Normal Force is the upward force exerted perpendicular to the ramp. Okay cool, but here is how my train of thought goes. Gravity is pulling the object down to the surface, and the object is exerting equal and opposite amount of force of gravity to stay in balance. This is what makes the object stay on the ramp right? What role is Normal Force is playing here though? If the surface is exerting a normal force, what is it's opposing force? Free body diagram tells me its the y component of the weight of the object. Is this true?

Also, while we are still talking about the object on a ramp. Let's assume the angle of the ramp to be 30 degrees. If you look at the free body diagram, you can see that, Normal force and the Y component of the weight are balancing each other out, so the object is not moving up or down. It sits on the ramp quietly. However, it starts to slide down soon. What force is making it slide down? If you look at the equation to solve for acceleration, it would be:

Wx = m*a

(Where W = weight of the object. Wx is the x component of the weight. In this case, Wx = Sin(30)*m*g)

Note: In the free body diagram, W is the hypotenuse (resultant).

So, isn't the above equation saying that the, object is accelerating because of the x component of weight?

Detailed explanation would be very much appreciated. Thank you :)
 
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tarunsworld20 said:
So to give a basic idea of where I am coming from:


F = G*m1*m2/r2

In the above equation, G is the gravitational constant of 6.67 x 10-11 Nm2/kg2

m1 = Mass of Earth
m2 = Mass of Human (which we neglect since it's very tiny compared to the mass of earth)
No, we don't "neglect" it because it is tiny. We leave it out to get
g= -\frac{GM}{r^2}
so that
F= mg= -\frac{GMm}{r^2}

r = distance between human's center and Earth's center.

Plugging in numbers will result in a value of 9.8 N

Q # 1) Note, the units are N. How do you get 9.8 m/s2
Again, the problems is you thinking we "neglect" the value of m (but keep its units).
F= -\frac{GMm}{r^2}
has units of Newtons, kg m/s^2. That means that having removed the mass m, we have also removed the kg units leaving only m/s^2. g is not "9.8 N", it is -9.8 m/s^2, an acceleration (NOT m/s).

Q # 2) So, if you wanted to be exact, the gravitational force exerted on each person is of a completely different value, because the mass of every individual varies, right?
Yes, it is the weight of the person!

9.8 N is the force between me and earth.
No. The force between you and the Earth is -9.8m where m is your mass. You just said it was different for different masses.

Now, according to Newton's third law, Force between two objects are equal on opposite.

Q # 3) So, if Earth's surface is pulling me down at approximately 9.8 N, then does this mean that, I am also pulling the Earth up at 9.8 N ? If so, since the masses of Earth and me are completely different, the acceleration at which Earth is pulling me down should be completely different from the acceleration at which I am pulling up the Earth right?
Yes, that's right. The Earth pulls on you with force -mg which means if you stepped off a cliff you would fall with acceleration -g. And you pull on the Earth with "equal and opposite" force +mg; which means the Earth would be accelerating toward you at (the force, mg, divided by the mass of the earth) -(gm/M), a negligible amount.

Q # 4) If I was exerting the same amount of gravitational force on the Earth as Earth was on me, then how is Normal Force playing a role in helping me to stay on the ground?
? because the forces are opposite. If you and another person pull on a rope, the pulls are toward each other, they don't cancel.

Whenever I look up stuff about Normal Force, the example I get is, think of an object on a ramp. Normal Force is the upward force exerted perpendicular to the ramp. Okay cool, but here is how my train of thought goes. Gravity is pulling the object down to the surface, and the object is exerting equal and opposite amount of force of gravity to stay in balance. This is what makes the object stay on the ramp right? What role is Normal Force is playing here though? If the surface is exerting a normal force, what is it's opposing force? Free body diagram tells me its the y component of the weight of the object. Is this true?
In your previous example, where you are standing on the ground, gravity was itself "normal" (perpendicular) to the ground. On the ramp, gravitational force is still straight downward- but you can't do straight down because the ramp is in the way. The force the ramp applies to you to keep you there is the "normal force" because it is perpendicular to the ramp. And, of course, just as that normal force causes you to press against the ramp, you feel the ramp pressing against the soles of your feet- you are feeling the "equal and opposite" force. Both of those forces will be "the y component" provided you have set up your coordinate system with the x-axis along the ramp and the y-axis perpendicular to it.

Also, while we are still talking about the object on a ramp. Let's assume the angle of the ramp to be 30 degrees. If you look at the free body diagram, you can see that, Normal force and the Y component of the weight are balancing each other out, so the object is not moving up or down. It sits on the ramp quietly. However, it starts to slide down soon. What force is making it slide down? If you look at the equation to solve for acceleration, it would be:

Wx = m*a

(Where W = weight of the object. Wx is the x component of the weight. In this case, Wx = Sin(30)*m*g)

Note: In the free body diagram, W is the hypotenuse (resultant).

So, isn't the above equation saying that the, object is accelerating because of the x component of weight?

Detailed explanation would be very much appreciated. Thank you :)
Yes, as I said before, if you have set up your coordinate system so that the x-axis is along the ramp and the y-axis is perpendicular to it, then the "normal" force that is preventing you from going through the ramp is the y- component. The x-component is parallel to the ramp and, if you don't have enough friction, you will "slide" down the ramp.
 
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tarunsworld20 said:
Gravity is pulling the object down to the surface, and the object is exerting equal and opposite amount of force of gravity to stay in balance. This is what makes the object stay on the ramp right?

This is a common misconception with regards to Newton's Third Law. People tend to only focus on the "equal" and "opposite" terms, and thus come to the erroneous conclusion that the forces cancel out. However, while the pair of forces are equal in magnitude and opposite in direction, they act on different bodies. In the case of the gravitational forces acting between the Earth and a person standing on it, the Earth is pulling the person towards it, while the person is also pulling the Earth towards himself. Hence, there is no "cancelling out".
 
Yes, f = Gm1*m2/r^2 but also the force on you is given by f = m2*a so,,,

m2*a = Gm1*m2/r^2

as you can see now, m2 cancels and you are left with the acceleration your body experiences toward the Earth, which is independent of your mass

in a similar fashion, if you want the acceleration of the Earth toward you...

m1*a = Gm1*m2/r^2

m1 cancels. Now you are left with the acceleration of the Earth toward your body and it is independent of the Earths mass

Note:The acceleration of the Earth is way smaller than your acceleration, that's why you don't notice it.
:smile:
 

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