Classical mechanics with time dependent force

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Homework Help Overview

The discussion revolves around a point mass subjected to a time-dependent force F(t) and aims to determine its position r(t) given initial conditions. The context is classical mechanics, specifically focusing on the effects of forces and motion over time.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the relationship between force, acceleration, and velocity, questioning how to integrate F(t) without knowing its specific form. There are discussions on simplifying the problem by focusing on vertical forces and the implications of boundary conditions.

Discussion Status

Participants are actively engaging with the problem, offering guidance on how to express velocity and position in terms of the generic force F(t). There is a recognition of the need to clarify the integration process and the importance of consistent notation. Some participants are attempting to derive expressions for v(t) and r(t) while checking their validity against known cases.

Contextual Notes

There is an ongoing discussion about the assumptions made regarding the direction of forces and the treatment of gravity. Participants are also considering the implications of using different symbols during integration to avoid confusion.

shyta
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Homework Statement



A point mass m is exposed to a time dependent force F(t). Determine the position r(t) of the point mass for the initial conditions r(0) = [itex]r_{0}[/itex]and v(0) = [itex]v_{0}[/itex]

Homework Equations





The Attempt at a Solution



[itex]\sum[/itex]F= ma
[itex]F_{z}[/itex](t) - mg = ma

a = 1/m [itex]F_{z}[/itex](t) - g
v = 1/m [itex]\int[/itex][itex]F_{z}[/itex](t) dt - [itex]\int[/itex]g dt
but how do I start to int F(t) without knowing the equation for F itself?
 
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Hi shyta! :smile:

Since you don't know the actual F(t), what you will have to do is to find a generic formula for r(t) that holds true for any F(t).
Basically that's what you've already been doing, so that's good! :smile:

Some comments on your attempt:

Do you have a reason to assume F(t) is vertical, and furthermore that gravity is not included in F(t) itself?

You have been given the boundary condition v = v0.
You should incorporate that in your formula.

And you haven't calculated r(t) yet.
 
shyta said:

Homework Statement



A point mass m is exposed to a time dependent force F(t). Determine the position r(t) of the point mass for the initial conditions r(0) = [itex]r_{0}[/itex]and v(0) = [itex]v_{0}[/itex]

Homework Equations





The Attempt at a Solution



[itex]\sum[/itex]F= ma
[itex]F_{z}[/itex](t) - mg = ma

a = 1/m [itex]F_{z}[/itex](t) - g
v = 1/m [itex]\int[/itex][itex]F_{z}[/itex](t) dt - [itex]\int[/itex]g dt
but how do I start to int F(t) without knowing the equation for F itself?

Consider how much impact you would add to the mass when


m*Vi + integral ( F dt ) [from 0 to t] = m*v(t)

but after you find v(t), find r(t) by integration and please note that you are working with vectors here !
 
Hi both! thanks for the replies.

iloveserena: I was trying to simplify things by considering the z-direction forces first, maybe i was over-simplifying/

Now assuming I follow stallionx's equation,

then v(t) = v_0 + 1/m [itex]\int[/itex]F(t) dt from 0 to T
v(t) = v_0 + [itex]\int[/itex]dv/dt dt from 0 to T
v(t) = v_0 + [itex]\int[/itex] dv from v to v+aT

am I in the correct direction?
 
shyta said:
then v(t) = v_0 + 1/m [itex]\int[/itex]F(t) dt from 0 to T

Yep. That's the formula for v as far as you can define it from the generic F(t).
shyta said:
v(t) = v_0 + [itex]\int[/itex]dv/dt dt from 0 to T
v(t) = v_0 + [itex]\int[/itex] dv from v to v+aT

am I in the correct direction?

No. These formulas basically only say that v=v.
But you need v based on F(t), which is what you already had.

You need to take the next step, by trying to define r(t).
Btw, for these formulas it is irrelevant whether they are vectors or scalars.
The formulas are true for both.
 
v(t) = v_0 + 1/m ∫F(t) dt from 0 to T

r(t) = v_0T + 1/m ∫∫ F(t) dtdt from 0 to T


But it makes not much sense from this equation because there is a last part that says check that you get the familiar results when F(t) = mg is constant in time
 
Well, you should use different symbols when integrating, and use "t" consistently.
Let me rewrite your equation:
[tex]r(t) = v_0 t + {1 \over m} \int_0^t \int_0^{\tau'} F(\tau) d\tau d\tau'[/tex]

Can you work this out for F(t)=mg?
 
I like Serena said:
Well, you should use different symbols when integrating, and use "t" consistently.
Let me rewrite your equation:
[tex]r(t) = v_0 t + {1 \over m} \int_0^t \int_0^{\tau'} F(\tau) d\tau d\tau'[/tex]

Can you work this out for F(t)=mg?

I got the equation :) thanks!

however just a quick query, why is there a need for the different symbols when integrating if it's the same closed intervals?
 
I was not sure if the integration confused you, so I made it more explicit.
I guess in this case the difference is not all to obvious, since the result will come out the same.
To illustrate the difference consider the following 2 integrals:
[tex]\int_0^t t \cdot \tau d\tau = {1 \over 2}t^3[/tex]
versus
[tex]\int_0^t t \cdot t dt = {1 \over 3}t^3[/tex]
See the difference?
Btw, your equation for r(t) is not right yet.
You missed something.
 
  • #10
oh i see i see.

for the r(t) equation do you mean the initial conditions?
 
  • #11
Yep! :wink:
 
  • #12
Hehe I got that! Thanks for the reminder and help! :)
 

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