Solving $\vec F = m\vec a$: How is $\vec F = -mkv$ Possible?

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In summary: My answer would be because Newton's law is not ##F_{avg}=ma_{avg}##. Perhaps @haruspex has some other...
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Homework Statement
Please see below
Relevant Equations
Please see below
For this problem,
1676331350534.png

My working is

## \vec F = m\vec a##
## \vec F = \frac {m(v - v_i)}{\Delta t} ##
## \vec F = \frac {-mkx}{\Delta t} ##

However, the solution said ##\vec F = -mkv ##. I don't understand how this is possible since ## v ≠\frac {x}{\Delta t} ## since ##v =\frac {\Delta x}{\Delta t} ##?

Many thanks!
 
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  • #2
Callumnc1 said:
Homework Statement:: Please see below
Relevant Equations:: Please see below

For this problem,
View attachment 322236
My working is

## \vec F = m\vec a##
## \vec F = \frac {m(v - v_i)}{\Delta t} ##
## \vec F = \frac {-mkx}{\Delta t} ##

However, the solution said ##\vec F = -mkv ##. I don't understand how this is possible since ## v ≠\frac {x}{\Delta t} ## since ##v =\frac {\Delta x}{\Delta t} ##?

Many thanks!
You do not take a finite difference, you take the derivative of v with respect to t to get acceleration.
 
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  • #3
Frabjous said:
You do not divide by δt, you take the derivative of v with respect to t to get acceleration.
Thank you for your reply @Frabjous!

I was trying to solve this problem using the algebra definition of velocity only. It's possible to solve this problem without calculus right?

Many thanks!
 
  • #4
Callumnc1 said:
It's possible to solve this problem without calculus right?
Yes, but you took the finite difference wrong. You want start with Δv/Δt.
Hint: Δvi=0 since it is a constant.
 
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Frabjous said:
Yes, but you took the finite difference wrong. You want start with Δv/Δt.
Hint: Δvi=0 since it is a constant.
Thank you for your reply @Frabjous !

I though ##\Delta v = v_f - v_i = v - v_i ## since they drop the ##f## for ##v##

Many thanks!
 
  • #6
Callumnc1 said:
Thank you for your reply @Frabjous !

I though ##\Delta v = v_f - v_i = v - v_i ## since they drop the ##f## for ##v##

Many thanks!
vi is just a constant. It could have just as easily been labeled a. vf is not in the original problem.
Δv=Δvi-Δ(kx)
Since k is also a constant you can pull it outside the Δ.
 
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  • #7
I wouldn't try it without calculus. Calculus is your friend here.
Might this be of help?$$a=\frac{dv}{dt}=\frac{dv}{dx}\frac{dx}{dt}=v\frac{dv}{dx}.$$
 
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  • #8
Callumnc1 said:
I was trying to solve this problem using the algebra definition of velocity
The "algebra definition" ##\frac{\Delta x}{\Delta t}## is for the average velocity over the time interval ##\Delta t##. You need to use the definitions of instantaneous velocity and instantaneous acceleration, which can only be expressed in calculus.
 
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Thank you for your replies @Frabjous, @kuruman and @haruspex !

I have figured out how solve to the problem using algebra. The calculus way as a lot faster thought!

## v_i = v(x_i) = v_i - kx_i ##
## v_f = v(x_f) = v_i - kx_f ##
## \Delta v = v_f - v_i= v_i - kx_f - (v_i - kx_i) = -kx_f + kx_i = k(x_i - x_f) = -k\Delta x ##

Then plug ##\Delta v## into Newton II to get their answer :)
 
  • #10
Callumnc1 said:
Thank you for your replies @Frabjous, @kuruman and @haruspex !

I have figured out how solve to the problem using algebra. The calculus way as a lot faster thought!

## v_i = v(x_i) = v_i - kx_i ##
## v_f = v(x_f) = v_i - kx_f ##
## \Delta v = v_f - v_i= v_i - kx_f - (v_i - kx_i) = -kx_f + kx_i = k(x_i - x_f) = -k\Delta x ##

Then plug ##\Delta v## into Newton II to get their answer :)
I assume your final steps are
##\frac{ \Delta v }{\Delta t}= -k\frac{ \Delta x }{\Delta t}##
##a=-kv##
But as I pointed out, that doesn’t quite work because the final line above should read
##a_{avg}=-kv_{avg}##, where the averages are taken over the time interval.
To get the target answer you need to apply the calculus principle of letting the deltas tend to zero.
 
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  • #11
haruspex said:
I assume your final steps are
##\frac{ \Delta v }{\Delta t}= -k\frac{ \Delta x }{\Delta t}##
##a=-kv##
But as I pointed out, that doesn’t quite work because the final line above should read
##a_{avg}=-kv_{avg}##, where the averages are taken over the time interval.
To get the target answer you need to apply the calculus principle of letting the deltas tend to zero.
Thank you for your reply @haruspex!

Your assumption of my finial steps is correct

I agree that I should has used average notation including ##F_{avg}##

However, would you please know why are looking for the instantaneous force not average force from the question?

Many thanks!
 
  • #12
Callumnc1 said:
However, would you please know why are looking for the instantaneous force not average force from the question?
My answer would be because Newton's law is not ##F_{avg}=ma_{avg}##. Perhaps @haruspex has some other answer.
 
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  • #13
kuruman said:
My answer would be because Newton's law is not ##F_{avg}=ma_{avg}##. Perhaps @haruspex has some other answer.
Thank you for your reply @kuruman !
 
  • #14
Callumnc1 said:
why are looking for the instantaneous force not average force
Because the question does not specify average it should be taken as meaning instantaneous.
 
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  • #15
haruspex said:
Because the question does not specify average it should be taken as meaning instantaneous.
Thank you for your reply @haruspex !
 

FAQ: Solving $\vec F = m\vec a$: How is $\vec F = -mkv$ Possible?

What does $\vec F = m\vec a$ represent?

$\vec F = m\vec a$ is Newton's second law of motion, which states that the force acting on an object is equal to the mass of the object times its acceleration. It is a fundamental principle describing how objects behave under the influence of forces.

How can $\vec F = -mkv$ be derived from $\vec F = m\vec a$?

$\vec F = -mkv$ represents a resistive force that is proportional to the velocity of the object, often encountered in scenarios involving drag or friction. To derive it from $\vec F = m\vec a$, consider a situation where the resistive force is the only force acting on the object, and it is proportional to the velocity. Here, $k$ is a positive constant, and the negative sign indicates that the force opposes the direction of motion.

What is the physical meaning of the constant $k$ in $\vec F = -mkv$?

The constant $k$ in the equation $\vec F = -mkv$ represents a coefficient of proportionality that characterizes the strength of the resistive force relative to the velocity. It depends on factors like the medium through which the object is moving and the object's properties, such as shape and surface area.

In which scenarios is $\vec F = -mkv$ commonly applied?

The equation $\vec F = -mkv$ is commonly applied in scenarios involving linear drag forces, such as an object moving through a fluid (air or water) at low speeds, where the drag force is linearly proportional to the velocity. It is also used in modeling damping forces in mechanical systems like springs and dampers.

How does $\vec F = -mkv$ affect the motion of an object?

When $\vec F = -mkv$ is applied, the resistive force causes the object to decelerate over time. The object's velocity decreases exponentially, approaching zero as time progresses if no other forces act on it. This results in an exponential decay of motion, leading to a gradual halt.

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