What is the meaning of dy/dt in differential equations?

  • Thread starter Townsend
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In summary: And in summary, the conversation was about understanding how to treat dy/dt in a differential equation and how it can be seen as a fraction or not. Some people argued that it is not a fraction, while others argued that it can be treated like one in certain cases. Ultimately, it was concluded that dy/dt is not a fraction but can be manipulated as one in certain situations.
  • #1
Townsend
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First of all I realize that this question has been asked before and answered before and so I appolgize if I am making any of you feel like you're talking to yourselves. But I am curious and the people here are the smartest people I know and so I want to hear from you guys and gals, an answer for this age old question.

When we have an expression like [tex]\frac{dy}{dt}=y+5[/tex] and we are asked to find a solution to this DE we

treat the numerator and denominator as if they were normal functions. How am I to think of this? I mean at a certain values of y and t [tex]\frac{dy}{dt}[/tex] is infact a number.

Oh, bother... :mad: I don't know how to ask the question correctly. What is this dy/dt thing? A change in y over a change in t or a quotent of funcitons or what?

Any help is appreciated very much. I have no problem working the problems from the text but eventually I will need to really understand what is going on so perhaps this is a good place to start.

thanks
 
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  • #2
IT IS A FUNCTION.It is unknown,just like the functions "y" itself...

Daniel.
 
  • #3
If y is some function of t, given by :

[tex]y = f(t) [/tex]

Then, the derivative of y (w. r. to t) is defined by

[tex]\frac{dy}{dt} \equiv f'(t) = \lim_{\Delta t \rightarrow 0} \frac {f(t + \Delta t) - f(t)}{\Delta t} [/tex]
 
  • #4
dextercioby said:
IT IS A FUNCTION.It is unknown,just like the functions "y" itself...

Daniel.

Ok so
[tex]\frac{dy}{dt}=1[/tex]
This means the solution is just y=t+c. But to get there we multiplied both sides of the equation by dt. So dy=dt. So what is dy? A change y in for a change in t? How would I graph this function then? What does its graph look like?

I don't know, I guess I always thought there was more to it then that. Since a derivate of a function is found using the limit process then I figured it would be something more like

[tex]\frac{dy}{dt}=lim_{h \rightarrow 0} \frac{f(t+h)-f(t)}{h}=1[/tex]

So then dy/dt is not really a quotient of functions that I can see. so how is it that we treat it like one? I mean in terms of limits what does dy=dt look like?
 
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  • #5
By the way the function I am using for an example is of course y(t)=t+c. Just in case someone was wondering why I am saying dy/dt=1 and it was not clear from what I was saying.

In any case I have to goto class so this will have to wait.

I'll be back...

Regards
 
  • #6
Townsend said:
Ok so
[tex]\frac{dy}{dt}=1[/tex]
This means the solution is just y=t+c. But to get there we multiplied both sides of the equation by dt. So dy=dt. So what is dy? A change y in for a change in t? How would I graph this function then? What does its graph look like?

Plot it and see.



Townsend said:
I mean in terms of limits what does dy=dt look like?

I think you've just written how [itex]\frac{dy}{dt}=1 [/itex] looks like in terms of limits...
:wink:
 
  • #7
dy isn't anything. We use it as a symbol to tell us what to do, and it behaves in some isolated cases as if we could separate dy/dtlike a fraction BUT IT ISN'T A FRACTION.

If f(y)dy/dt = g(t), then it follows that int f(y)dy = int g(t)dt

dy and dt are not themselves things that you need to worry about, they are just symbols.

Later on you will learn about differentials, but you do not need those right now.
 
  • #8
The point is that dy/dx is NOT a fraction but it is a limit of a fraction so can be "treated" like a fraction: to prove a "fraction" theorem about dy/dx, go back before the limit, use the fact that the "difference quotient" is a fraction, and then take the limit again.

In order to use that we define the "differential" dx as purely notational and then define the corresponding dy by dy= f '(x)dx (the only time it makes sense to have a "dx" without a corresponding "dy" or vice-versa is when you are integrating).

When you get into functions of several variables, differentials get a whole lot more interesting!
 
  • #9
Townsend said:
Ok so
[tex]\frac{dy}{dt}=1[/tex]
This means the solution is just y=t+c. But to get there we multiplied both sides of the equation by dt.

Like the others said. dy/dt is not a fraction, and in that sense, writing dy/dt=1 as dy=dt and then integrate is a fraudulent way to get the solution of the DE.
For starters, it may be best to think about it as follows. Although it's strictly not allowed. Let's try it anyway. That's the nice thing about differential equations. It doesn't matter HOW you get your answer. You can check whether it is correct afterwards anyway by putting it in the DE.

That being said, the reason why it works because of the substitution rule (which in turn is a result of the chain rule of differentiation).
Note that we can only separate the dy and dt and integrate when we can put the stuff depending on y on one side and the stuff depending on t on the other side. The equation is then seperable.
It is then always of the form: f(y)dy/dt=g(t), for some functions f of y and g of t. Now if we integrate both sides wrt t:

[tex]\int f(y)\frac{dy}{dt}dt=\int g(t) dt[/tex]

by the substitution rule, this equals:
[tex]\int f(y)dy = \int g(t)dt[/tex]

which is exactly the same result you get by treating dy/dt as a fraction.
It is therefore justified to treat them like fractions in this case.
 
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  • #10
what you said was right, it is the change in y with respect to the change in t.
we limit t to become a very small number, and see what difference is it compared with y in a given function. because dy = dt, then you will get a graph where a small change in y (within the y axis) will give an EQUIVALENT small change in t (in the t axis)
i believe it is the same as saying y = t, which is just a unit of y compared with a unit of t. well, it can be proven using integration as well.
 
  • #11
Galileo said:
Like the others said. dy/dt is not a fraction...

Everyone, thankyou for your replies...That being said Galileo, your reply really made things clear for me. I can relate what you said to the chain rule and actually I don't like to use a u sub to solve integrals. I try to see things in terms of the chain rule.

[tex]\frac{d}{dt}f(g(t))=f'(g(t))*g'(t)[/tex]

Good thing we have the chain rule to use. It seems like so much of calculus depends on it.

Regards
 
  • #12
This is the best explanation I could come up with which is composed of ideas from various calc books, and from the explanations of some of the people here at PF. I would appreciate it if someone could look this over and make sure its right.

Just to add to what has been said here...
As Galileo and others have mentioned, when we treat [itex] \frac{dy}{dx}[/itex] as if it were a fraction to solve differential equations, we use this simply as a notational device to hide the messy details of the chain rule.


To give an example:
suppose [itex] y = f(x) [/itex] ,

Let [itex]g[/itex] be a function of [itex]x[/itex] and [itex]G[/itex] be an antiderivative of [itex]g[/itex], therefore...

[tex] \frac{d}{dx}G(x) = g(x) \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ (1)[/tex]


Let [itex]h[/itex] be a function of [itex]y[/itex], and [itex]H[/itex] be an antiderivative of [itex]h[/itex], therefore...

[tex] \frac{d}{dy}H(y) = h(y) \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ (2)[/tex]


also realize that [itex]H[/itex] and [itex]h[/itex] are both composite functions of [itex]x[/itex] (since [itex]y = f(x)[/itex])
therefore (2) can be written as

[tex] \frac{d}{dy}H(f(x)) = h(f(x)) \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ (3)[/tex]


we can use the chain rule on (3) to find the derivative of [itex]H[/itex] wrt [itex]x[/itex],

[tex] \frac{d}{dx}H(f(x)) = H'(f(x))f'(x) [/tex]

but from (2), [itex] H'(f(x)) = h(f(x))[/itex] so this becomes

[tex] \frac{d}{dx}H(f(x)) = h(f(x))f'(x) \ \ \ \ \ \ \ \ \ (4) [/tex]


Now here comes an example of how the Liebeniz notatin is useful when we reverse the process and are given a derivative and are asked to find the original function ( A differential equation ).

suppose were asked to solve:
[tex] \frac{dy}{dx} = \frac{g(x)}{h(y)} [/tex]

we usually use the method of separation of variables withouth hesitation to rewrite this as

[tex] h(y)dy = g(x)dx [/tex]

and solve

[tex] \int h(y)dy = \int g(x)dx \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ (5)[/tex]

since [itex]H(y)[/itex] is an antiderivative of [itex]h(y)[/itex]
and [itex]G(x)[/itex] is an atiderivative of [itex]g(x)[/itex]
the solution to (5) is

[tex] H(y) = G(x) + C \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ (6)[/tex]


now it looks like we were able to treat [itex]dy[/itex] and [itex]dx[/itex] as if they were components of a fraction, but if we look under the covers, its just the chain rule in reverse. We can see this by rewriting the LHS of (5) subsituting [itex]y = f(x) [/itex] and [itex]dy = f'(x)dx. [/itex]

[tex] \int h(f(x))f'(x)dx = \int g(x)dx \ \ \ \ \ (7) [/tex]

our goal is still to find the antiderivative of each side

but looking at (4) we see that [itex]H(f(x))[/itex] is an antidiverative of [itex]h(f(x))f'(x)[/itex] ( this is just the reverse of the chain rule ).

Thus our solution is

[tex] H(f(x)) = G(x) + C [/tex]

again, subsituting y = f(x) we get the same result

[tex] H(y) = G(x) + C [/tex]

so you see,,, Libeniz's notational device is an easier method to solve such problems because it let's us hide all the messy details of the chain rule.



There is also another common use for Liebeniz's differential notation which allows us to approximate changes in a function [itex] \Delta y [/itex] with a corresponding change in the indepent variable(s) [itex] \Delta x [/itex]. This method is known as the linear approximation, and is given by

[tex] dy = f'(x)dx [/tex]

where it is defined that [itex] dx = \Delta x [/itex]

here [itex]dy[/itex] and [itex]dx[/itex] are assigned values, and we use dy to approximate the value of [itex] \Delta y [/itex], ( where the approximation gets better, the smaller the [itex] \Delta x [/itex] ).


These two devices for the Liebeniz notation are not to be confused with each other, they are used for separate purposes.


Let me know if this is any help. I tried to make it as explicit as possible, but I'm afraid it might have become too lengthy in the process. Also please correct me if I am wrong somewhere or if you think there is more that should be added.

Thanks,
-MS
 
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  • #13
MathStudent said:
[tex] \frac{d}{dy}H(f(x)) = h(f(x)) \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ (3)[/tex]

I am not sure number 3 is really correct, or maybe I am not seeing it right...

But overall everything looks really good and you managed to make the undercover work very explicit.

Thanks
 

FAQ: What is the meaning of dy/dt in differential equations?

What is the meaning of dy/dt in differential equations?

The notation dy/dt is used to represent the derivative of a function y with respect to time t in differential equations. It represents the instantaneous rate of change of y with respect to t.

Why is dy/dt important in differential equations?

In differential equations, dy/dt is important because it helps us to model and understand the behavior of a system over time. It allows us to calculate the rate at which a variable changes and how it affects other variables in the system.

How is dy/dt calculated?

Dy/dt is calculated by taking the limit as the change in y (Δy) approaches 0, divided by the change in t (Δt). This can be represented as dy/dt = lim(Δy/Δt) as Δt → 0. In simpler terms, it is the slope of the tangent line to the graph of y at a specific point.

What is the physical interpretation of dy/dt?

The physical interpretation of dy/dt depends on the context of the problem. In general, it represents the rate of change of a physical quantity with respect to time. For example, in physics, dy/dt can represent the velocity of an object at a given time.

Where is dy/dt used in real life?

Dy/dt is used in various fields, such as physics, engineering, economics, and biology, to model and analyze systems that change over time. It is also used in everyday situations, such as calculating the speed of a moving object or the growth rate of a population.

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