Frequently Made Errors - Pseudo and Resultant Forces - Comments

Click For Summary

Discussion Overview

The discussion revolves around the concepts of pseudo and resultant forces, particularly in the context of circular motion and non-inertial reference frames. Participants explore the distinctions between applied and resultant forces, the implications of these definitions, and the nature of fictitious forces in various frames of reference.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants express confusion regarding the distinction between applied and resultant forces, particularly in the context of centripetal force and gravitational force acting on orbiting bodies.
  • There is a suggestion that centripetal force should be avoided as a term due to misconceptions it may create, with some arguing that it is not an applied force.
  • One participant argues that the gravitational force on an orbiting planet is an applied force that results in centripetal force, while others challenge this view.
  • Concerns are raised about the definition and implications of fictitious forces, with some asserting that using a non-inertial frame does not invalidate kinematic laws.
  • There is a debate over the existence of Coriolis force versus Coriolis acceleration, with participants discussing the definitions and implications of these terms.
  • Some participants propose that the term "centripetal" refers to a situation rather than an interaction, suggesting a need for clarity in terminology.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the definitions and implications of applied versus resultant forces, the validity of fictitious forces, or the terminology surrounding centripetal and Coriolis forces. Multiple competing views remain throughout the discussion.

Contextual Notes

There are unresolved issues regarding the definitions of forces, the assumptions underlying the use of non-inertial frames, and the implications of various terms used in the discussion. Participants acknowledge the complexity and nuance involved in these concepts.

haruspex
Science Advisor
Homework Helper
Insights Author
Gold Member
Messages
42,843
Reaction score
10,509
haruspex submitted a new PF Insights post

Frequently Made Errors - Pseudo and Resultant Forces

Coriolis-80x80.png


Continue reading the Original PF Insights Post.
 
Physics news on Phys.org
The distinction between applied and resultant force may be confusing. And even misleading, when you say that the centripetal force cannot be "applied" but only resultant. What if there is only one force acting on the body in circular motion? What if there is a tangential force as well as a radial force? Will their resultant be the centripetal force?
 
A little confused about the applied vs resultant bit too. Having a hard time seeing the gravitational force on an orbitting planet as resultant but not "applied". Probably an issue with definitions I'm not getting.

Unless its saying that the centripetal is generally resultant. In the case of an orbitting planet, the gravitational force is the only force and it is an applied force which results in the centripetal force (consisting of only gravitation).

nasu said:
The distinction between applied and resultant force may be confusing. And even misleading, when you say that the centripetal force cannot be "applied" but only resultant. What if there is only one force acting on the body in circular motion? What if there is a tangential force as well as a radial force? Will their resultant be the centripetal force?

The key word in the definition given is that the centripetal force is a resultant force but not the resultant force. In general, systems don't have a single unique resultant force.
 
Last edited:
Newton's second law says
$$\sum_{i=1}^n \vec{F}_i = \vec{F}_1+\vec{F}_2+\cdots+\vec{F}_n = m\vec{a}.$$ The ##\vec{F}_i##'s are the forces acting on a body — that is, the applied forces. The centripetal force is not an applied force, so it doesn't appear as part of the sum of the forces. Note that in an inertial frame, an applied force should have a reaction counterpart, e.g., the Earth exerts a gravitational force on the Moon, and the reaction force is the Moon exerting a force on the Earth. In general, there is no reaction counterpart to the centripetal force because it's not an applied force.

I agree with the suggestion to avoid the term centripetal force altogether precisely because it leads to the misconception raised here. An object on a curved path instead experiences a centripetal acceleration ##a_c = v^2/r##, where ##v## is the object's speed and ##r## is the radius of curvature.
 
nasu said:
What if there is a tangential force as well as a radial force?
I was careful (I think) to refer always to the radial component of the resultant.
Overt said:
In the case of an orbitting planet, the gravitational force is the only force and it is an applied force which results in the centripetal force (consisting of only gravitation).
Exactly.
Overt said:
In general, systems don't have a single unique resultant force.
They don't? Well, they could reduce to a single force plus a screw ... but otherwise?
vela said:
avoid the term centripetal force altogether
Interesting suggestion. I'll add that advice.
 
I never understood all this buzz about "fictitious forces", or a statement like " Using a non-inertial frame makes the usual kinematic laws fail". No, it does not. The equation of motion just doesn't transform covariantly under (linear or rotational) accelerations, as it does under Galilei transformations. That's the whole deal. And because one can state Newton's laws, just as special or General relativity, in a coordinate-free way using differential geometry, there is no reason to single out inertial frames of reference.

When there are no forces, a particle follows a geodesic in Newtonian spacetime. This is a straight line, because space is flat. One can assign coordinate values to this line, giving that the second time derivative of x vanishes. If you then apply e.g. a time-dependent rotation R(t), such that x'=Rx, then automatically you get the centrifugal and Coriolis force. No talk about 'fictitious'.
 
"Centrifugal view
In the reference frame of the circling object, there is no radial acceleration."
Of course there is radial acceleration: v^2/r.
 
Ranku said:
"Centrifugal view
In the reference frame of the circling object, there is no radial acceleration."
Of course there is radial acceleration: v^2/r.
In the reference frame of a given object, that object has no acceleration by definition.
 
1. Real versus Fictitious

Pseudo, or “fictitious“, forces can arise when a non-inertial frame of reference is used. Using a non-inertial frame makes the usual kinematic laws fail. Pseudo forces must be added into correct them.

This statement is nonsense by definition of the term kinematics. Kinematics is, by definition, the description of motion without regard to forces. It uses whatever coordinate systems are convenient for the problem at hand, some likely to be inertial while other clearly are not, but all of that is irrelevant.
 
  • #10
5. Coriolis Force
A Coriolis force arises from radial motion in a rotating reference frame.

This is muddy thinking. There is a Coriolis acceleration that arises at times, but there is no Coriolis force. When the Coriolis acceleration is multiplied by a mass factor, the result is an inertial reaction term, an M*A term, but it is not a force.

(And no, Newton's Law does not say that any particular M*A term is a force. It says that the sum of all actual forces is equal to mass*acceleration of the cm for a particle (which is the particle location itself). Randomly chosen M*A terms are not forces, certainly not actual forces.)
 
  • #11
OldEngr63 said:
5. Coriolis Force
A Coriolis force arises from radial motion in a rotating reference frame.

This is muddy thinking. There is a Coriolis acceleration that arises at times, but there is no Coriolis force. When the Coriolis acceleration is multiplied by a mass factor, the result is an inertial reaction term, an M*A term, but it is not a force.

(And no, Newton's Law does not say that any particular M*A term is a force. It says that the sum of all actual forces is equal to mass*acceleration of the cm for a particle (which is the particle location itself). Randomly chosen M*A terms are not forces, certainly not actual forces.)
The same objection can be made to the term "centrifugal force". Bear in mind that by definition a fictitious force is one that the observer invents to account for the experience, so it is reasonable to say that there is a Coriolis force. I'll try to make this clearer.
 
  • #12
OldEngr63 said:
1. Real versus Fictitious

Pseudo, or “fictitious“, forces can arise when a non-inertial frame of reference is used. Using a non-inertial frame makes the usual kinematic laws fail. Pseudo forces must be added into correct them.

This statement is nonsense by definition of the term kinematics. Kinematics is, by definition, the description of motion without regard to forces. It uses whatever coordinate systems are convenient for the problem at hand, some likely to be inertial while other clearly are not, but all of that is irrelevant.
Yes, kinematics was the wrong word. I'll correct it.
 
  • #13
I agree with the suggestion that the term term centripetal force be banned. One must understand that he term "centripetal" refers to a situation rather than an interaction. It is like calling some force as forward if it increases the speed and backward if it reduces the speed. Let us consider a point particle. what are the possibilities:
A. it is at rest permanently so a = 0 and resultant applied force on it is zero.
B. momentarily at rest, the one needs to find the direction and magnitude of its acceleration, a. "ma" will then be the the resultant externally applied force on the particle.
C. Moving in a straight line, find the direction and magnitude of its acceleration, a. "ma" will then be the the resultant externally applied force on the particle.
D. If the particle is moving along a curve, then, the resultant force on it may have a tangential component and a normal component. Normal component can change only the direction and not the speed and thecomponent tangential can only change the speed and not direction. This normal component is what we call centripetal force.

Coming to the term fictitious to centrifugal force is also not proper as its effects are real in a non inertial frame. The term pseudo is more preferable. It is the term added to make Newton's laws applicable to non-inertial frames.
 

Similar threads

  • · Replies 34 ·
2
Replies
34
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 87 ·
3
Replies
87
Views
23K
  • · Replies 142 ·
5
Replies
142
Views
14K