Understanding Force Pairs in Accelerated Systems: Explained for Beginners

AI Thread Summary
The discussion focuses on understanding force pairs in accelerated systems, particularly when a hand supports a mass that is too heavy to hold. It clarifies that when the hand and mass accelerate downwards, the force exerted by the mass on the hand is less than its weight due to the downward acceleration. In static equilibrium, the forces are equal, but in acceleration, the dynamics change, resulting in a net downward force. The conversation highlights that if both the hand and mass are in free fall, the forces between them would be zero, emphasizing the difference in force interactions during acceleration versus static conditions. This understanding is crucial for grasping Newton's third law in non-static scenarios.
kbm
Messages
7
Reaction score
0
This is going to be a very elementary question, but I am having a hard time wrapping my head around it for whatever reason.

In static equilibrium, like a book on a table, I have no problem seeing that the force exerted on the table by the book is equal and opposite to the force exerted on the book by the table.

But when things are being accelerated I am having a hard time grasping how the force pairs are equal.

For example, if a hand is holding up a mass that is too heavy for the person to hold, then the mass and the hand will both be accelerated downwards. The forces acting on the mass would be the force of gravity, acting down, and the pushing force of the hand, acting up. The force of gravity is greater than the pushing force so there is a net force downwards.

How is it that the hand exerts an equal and opposite force on the mass?

The forces on the hand would be the weight of the mass, acting downwards, the force of gravity on the hand, acting downwards, and the pushing force of the arm on the hand, acting upwards.

The force of the mass on the hand is equal to the weight of the mass (mg), and the force of the hand on the mass is equal to the pushing force of the arm. But if these were equal, then the pushing force of the arm would equal the weight, or force of gravity, on the mass, an then there would be no net force downwards on the mass.

What am I getting confused?
 
Physics news on Phys.org
Welcome to PF!

Hi kbm! Welcome to PF! :smile:
kbm said:
The force of the mass on the hand is equal to the weight of the mass (mg) …

No, the force of the mass on the hand is less than mg (if you like, because the hand is accelerating away, so it isn't getting the full oomph from the mass), and the force of the hand on the mass is the same (less than mg), causing the mass to accelerate downwards.
 
Thanks for the reply.

Alright so just for clarification: If the hand was holding the mass up at equilibrium, then the force of the mass on the hand would be equal to mg, correct?

But because the hand is moving downwards, the force of the mass on the hand is <mg. So in an FBD the forces acting on the mass would be (mg) acting downwards and (<mg) acting upwards, so a net force down. Similarly, the forces on the hand would be (<mg) acting downwards, the weight of the hand acting down, and a push force acting upwards, which must be still LESS than (<mg).

Why though, if the hand and the mass are still in direct contact and accelerating down at the same rate, is the force of the mass on the hand LESS than it would be if they were both stationary?
 
kbm said:
Alright so just for clarification: If the hand was holding the mass up at equilibrium, then the force of the mass on the hand would be equal to mg, correct?

But because the hand is moving downwards, the force of the mass on the hand is <mg. So in an FBD the forces acting on the mass would be (mg) acting downwards and (<mg) acting upwards, so a net force down. Similarly, the forces on the hand would be (<mg) acting downwards, the weight of the hand acting down, and a push force acting upwards, which must be still LESS than (<mg).

Yes. :smile:
Why though, if the hand and the mass are still in direct contact and accelerating down at the same rate, is the force of the mass on the hand LESS than it would be if they were both stationary?

If they were free-falling, they would still be in direct contact and accelerating down at the same rate, but the forces between them would be zero, wouldn't they?

This is an intermediate stage.
 
Alright that makes sense. Thanks for the help.
 
Consider an extremely long and perfectly calibrated scale. A car with a mass of 1000 kg is placed on it, and the scale registers this weight accurately. Now, suppose the car begins to move, reaching very high speeds. Neglecting air resistance and rolling friction, if the car attains, for example, a velocity of 500 km/h, will the scale still indicate a weight corresponding to 1000 kg, or will the measured value decrease as a result of the motion? In a second scenario, imagine a person with a...
Thread 'Gauss' law seems to imply instantaneous electric field propagation'
Imagine a charged sphere at the origin connected through an open switch to a vertical grounded wire. We wish to find an expression for the horizontal component of the electric field at a distance ##\mathbf{r}## from the sphere as it discharges. By using the Lorenz gauge condition: $$\nabla \cdot \mathbf{A} + \frac{1}{c^2}\frac{\partial \phi}{\partial t}=0\tag{1}$$ we find the following retarded solutions to the Maxwell equations If we assume that...
Dear all, in an encounter of an infamous claim by Gerlich and Tscheuschner that the Greenhouse effect is inconsistent with the 2nd law of thermodynamics I came to a simple thought experiment which I wanted to share with you to check my understanding and brush up my knowledge. The thought experiment I tried to calculate through is as follows. I have a sphere (1) with radius ##r##, acting like a black body at a temperature of exactly ##T_1 = 500 K##. With Stefan-Boltzmann you can calculate...
Back
Top