What does a derivative of 0 tell us about a function?

  • Thread starter struggles
  • Start date
  • Tags
    Vectors
In summary: Anyway, the issue is: if ##d^2 f(t)/dt^2 = 0## for all ##t##, what is the most general possible form for ##f(t)##? Well, if you set ##g(t) = df(t)/dt##, you have ##dg(t)/dt = 0##...which is the most general form possible.
  • #1
struggles
50
0

Homework Statement


So my textbook states that F = ma = m(d2r/dt2) can be integrated to give r = r0 + tv0 when F = 0.

Homework Equations

The Attempt at a Solution



I've tried rewriting it as F = m(dv/dt) and integrating that to give Ft = mv + c but this is obviously not in the right form. I've also tried using F = dP/dt but that gives effectively the same answer as above. I have no idea how to get the solution given!
 
Physics news on Phys.org
  • #2
struggles said:

Homework Statement


So my textbook states that F = ma = m(d2r/dt2) can be integrated to give r = r0 + tv0 when F = 0.

Homework Equations

The Attempt at a Solution



I've tried rewriting it as F = m(dv/dt) and integrating that to give Ft = mv + c but this is obviously not in the right form. I've also tried using F = dP/dt but that gives effectively the same answer as above. I have no idea how to get the solution given!

When there is no force, naturally there is no acceleration. The result your textbook shows is just the basic kinematic equation without the acceleration term.

Can you show the steps for your work? How're you actually setting things up? Are you using your initial condition?

So for the work shown, what is Ft and mv? What happens when you take the integral of the constant? What is that constant?
 
Last edited:
  • #3
struggles said:

Homework Statement


So my textbook states that F = ma = m(d2r/dt2) can be integrated to give r = r0 + tv0 when F = 0.

Homework Equations

The Attempt at a Solution



I've tried rewriting it as F = m(dv/dt) and integrating that to give Ft = mv + c but this is obviously not in the right form. I've also tried using F = dP/dt but that gives effectively the same answer as above. I have no idea how to get the solution given!

The vector ##\vec{r}(t) = (x(t),y(t),z(t))##, where x, y and z are its three components. What kind of functions x(t), y(t) and z(t) have second derivatives that are identically 0?
 
  • #4
Ray Vickson said:
The vector ##\vec{r}(t) = (x(t),y(t),z(t))##, where x, y and z are its three components. What kind of functions x(t), y(t) and z(t) have second derivatives that are identically 0?

All function such as 2t have a second derivative of 0 but i don't know where to go with that?
 
  • #5
Student100 said:
When there is no force, naturally there is no acceleration. The result your textbook shows is just the basic kinematic equation without the acceleration term.

Can you show the steps for your work? How're you actually setting things up? Are you using your initial condition?

So for the work shown, what is Ft and mv? What happens when you take the integral of the constant? What is that constant?

F dt = m dv
Ft = mv + c
When F = 0 , c = -mv
Ft = mv - mv = 0 <--- This obviously isn't right but i don't know what else to do!
 
  • #6
struggles said:
F dt = m dv
Ft = mv + c
When F = 0 , c = -mv
Ft = mv - mv = 0 <--- This obviously isn't right but i don't know what else to do!
Why is Ft=0 not right when F=0?
 
  • #7
Samy_A said:
Why is Ft=0 not right when F=0?
Well the equation makes sense when F = 0. But i still can't manipulate it into the form stated in the book.
 
  • #8
struggles said:
Well the equation makes sense when F = 0. But i still can't manipulate it into the form stated in the book.
You have ##c+mv=0##, or ##v=-c/m##.
What does this tell you about ##v##? (By the way, Don't forget that ##v## is a vector, as Ray mentioned. So better write ##\vec v##).

What can you say about ##\frac{d \vec r}{dt}##?
 
  • #9
Samy_A said:
You have ##c+mv=0##, or ##v=-c/m##.
What does this tell you about ##v##? (By the way, Don't forget that ##v## is a vector, as Ray mentioned. So better write ##\vec v##).
What can you say about ##\frac{d \vec r}{dt}##?

so this shows that t##\vec v## is a constant so ##\frac{d \vec r}{dt}## so would integrate to give -c/mt = v0t?
 
  • #10
struggles said:
so this shows that t##\vec v## is a constant so ##\frac{d \vec r}{dt}## so would integrate to give -c/mt = v0t?
t##\vec v## is not constant, ##\vec v## is constant.
Integrating ##\frac{d \vec r}{dt}## should give you ##\vec r## as a function of ##t##.
 
  • #11
struggles said:
All function such as 2t have a second derivative of 0 but i don't know where to go with that?

Are you telling us that you don't know where to go with that, or are you asking us if you don't know where to go with that (which is the effect of using a "?" at the end)?

Anyway, the issue is: if ##d^2 f(t)/dt^2 = 0## for all ##t##, what is the most general possible form for ##f(t)##? Well, if you set ##g(t) = df(t)/dt##, you have ##dg(t)/dt = 0## for all ##t##. What is the most general form of a function whose derivative is identically equal to 0? Once you have answered that, you have a formula for ##df/dt##, which you can then integrate to get ##f(t)##.
 
Last edited:
  • Like
Likes Student100
  • #12
struggles said:
F dt = m dv
Ft = mv + c
When F = 0 , c = -mv
Ft = mv - mv = 0 <--- This obviously isn't right but i don't know what else to do!
You aren't using your initial condition, and it seems like you don't know how to actually take the integral. Is the vector thing confusing you?

##\vec{F} = m\vec{a}## is at it's heart a differential equation. Let's just look at the x direction for now: ##F_x = ma_x## Now let's use the initial condition of no net force: ##0 = ma_x## We know ##a_x = \frac{d^2x(t)}{dt^2}## so go ahead and make that substitution: ##0 = m\frac{d^2x(t)}{dt^2}## Now integrate this looking at the definite integral from 0 to t so we can nicely define C. Whats going to happen to the mass, what expression will you end up with? This should help you answer Ray's question too I hope.
 
  • #13
Student100 said:
You aren't using your initial condition, and it seems like you don't know how to actually take the integral. Is the vector thing confusing you?

##\vec{F} = m\vec{a}## is at it's heart a differential equation. Let's just look at the x direction for now: ##F_x = ma_x## Now let's use the initial condition of no net force: ##0 = ma_x## We know ##a_x = \frac{d^2x(t)}{dt^2}## so go ahead and make that substitution: ##0 = m\frac{d^2x(t)}{dt^2}## Now integrate this looking at the definite integral from 0 to t so we can nicely define C. Whats going to happen to the mass, what expression will you end up with? This should help you answer Ray's question too I hope.

I think I'm getting confused with the integration of a second order differential as I haven't done it in a while. I get t2/2 = mx +c but I'm really not sure if this is correct!
 
  • #14
struggles said:
I think I'm getting confused with the integration of a second order differential as I haven't done it in a while. I get t2/2 = mx +c but I'm really not sure if this is correct!

Not correct at all.

Show me what you're doing from ##0 = m\frac{d^2x(t)}{dt^2} ##
 
  • #15
Student100 said:
Not correct at all.

Show me what you're doing from ##0 = m\frac{d^2x(t)}{dt^2} ##

0 = mdv(t)/dt
∫dt = m∫dv
t = mv
t = mdx/dt
∫txt = m∫dx
t2/2 = mx + c
 
  • #16
struggles said:
0 = mdv(t)/dt
∫dt = m∫dv
t = mv
t = mdx/dt
∫txt = m∫dx
t2/2 = mx + c

First how does 0dt become just dt. Next, you just seem to be dropping the second derivative. You should also look at the definite integral.

$$\int_0^t0dt = m\int_0^t\frac{d^2x(t)}{dt^2}dt$$

Do you know how to take this? What's the fundamental theorem of calculus say?

Further, for the mass we assume two things: It's both non-zero, and doesn't change with time. That's why we can pull it out of the integral. It also how we can get rid of the term all together.
 
  • #17
struggles said:
I think I'm getting confused with the integration of a second order differential as I haven't done it in a while. I get t2/2 = mx +c but I'm really not sure if this is correct!

You are seriously over-thinking the problem. You do not need to know much about differential equations and the like; you just need to remember that a derivative of a function g(t) at t is the slope of the tangent line to the graph of y = g(t). So, if dg(t)/dt = 0 for all t, what does the graph of y = g(t) look like? What does that tell you about the nature of the function g(t)?
 

FAQ: What does a derivative of 0 tell us about a function?

What are vectors in Newton's equation?

Vectors in Newton's equation refer to the quantities that have both magnitude and direction, such as force, velocity, and acceleration. In Newton's Second Law, these vectors are used to describe the relationship between an object's mass, acceleration, and the applied force.

How are vectors represented in Newton's equation?

Vectors in Newton's equation are commonly represented using the notation of bold letters, such as F for force, v for velocity, and a for acceleration. The direction of the vector is typically indicated by an arrow above the letter, and the magnitude is denoted by the size of the vector.

What is the significance of vectors in Newton's equation?

Vectors play a crucial role in Newton's equation as they help describe the relationship between an object's motion and the forces acting on it. They allow scientists to accurately predict the acceleration and movement of an object when subjected to different forces, making them essential in understanding the laws of motion.

Can vectors in Newton's equation be negative?

Yes, vectors in Newton's equation can be negative. This indicates the direction of the vector is opposite to the positive direction, and it is commonly represented by a negative sign in front of the magnitude. For example, a force of -5N would mean the force is acting in the opposite direction as a force of 5N.

How are vectors added in Newton's equation?

In Newton's equation, vectors are added using vector addition. This involves combining the magnitudes and directions of the vectors using geometric methods, such as the parallelogram rule or the head-to-tail method. The resulting vector represents the net force acting on the object and is used to calculate the object's acceleration.

Back
Top