Velocity differential equations

In summary, the 1997 Dodge Viper has a mass of 1547 kg and an engine that can produce a maximum driving force of 12.36 kN. It is assumed that drag is proportional to speed with a constant k = 164 Ns/m. From this information, we can determine the initial acceleration of the Viper from rest to be 7.99 N/kg and the maximum speed (or terminal velocity) to be 75.37 m/s. To calculate the distance and speed for t = 12.2 s, we can use the equation F-kv=ma and integrate to find v = (f*e^{-k t /m} - f) / (-k), which gives us a distance
  • #1
prezmoneymike
17
0
The 1997 Dodge Viper has mass 1547 kg and an engine that can produce a maximum driving force of 12.36 kN. Suppose drag is proportional to speed such that k = 164 Ns/m.
(a) Determine the initial acceleration of the Viper from rest. (b) Determine the maximum speed (i.e. terminal velocity). (c) Calculate the distance and speed for t = 12.2 s. (d) Find time and distance for the car to reach 99% of its top speed.

So basically I found the answers for a and b they are as follows.
A)F=ma 12360N=1547kg(a) a=7.99N/kg
B)F=ma Fcar-Fdrag= 0 Fcar=Fdrag F=kv 12360N=164(v) v=75.37

So those two are checked and fine but c I am havin trouble still
c) F-Fd=ma F-kv=ma F-kv=m dv/dt
integral 1/m dt= integral dv/(f-k(v))
t/m= integral dv/(f-kv)

so I am stuck here. o and i think the integral limit is 0 and V. my teacher said to do
u substitution and make u=F-kv and du=-kdv
thereby making t/m= -1/k integral du/u with limit f and f-kv
i have no idea what to do next with the integration. Basically i need someone to help integrate it and solve for v. then with that equation i can solve for part d. also i have no idea how to calculate the distance. o i need this for tomorow morning so any quick help would be very helpful thanks.
 
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  • #2
Hi prezmoneymike,

From a table of integrals, you can find:

[tex]
\int \frac{du}{u} = \ln |u| + C
[/tex]

where [tex]C[/tex] is the normal additive integration constant. What do you get with this?
 
  • #3
so it would be t/m= -1/k ln (f-kv) + c?
 
  • #4
You have to evaluate [itex]\ln u [/itex] at the beginning and ending points, and then subtract them in the usual way to get the result for the definite integral. What do you get?
 
  • #5
umm I am not sure how to do that because i took calculus last year by a teacher who taught it horribly. so do u think u could show me how to accomplish this?
 
  • #6
Let me show you on a different integral (since the forum rules state I'm not supposed to do work for you).

If your integral is

[tex]
\int\limits_a^b x\ dx
[/tex]

The formula from a table would be:

[tex]
\int\limits x\ dx= \frac{x^2}{2}
[/tex]

up to an additive constant. Then since the limits on your integral are from a to b, you would do:

[tex]
\left. \frac{x^2}{2} \right|_a^b = \frac{b^2}{2} - \frac{a^2}{2}
[/tex]

So you evaluate the expression from the integral at the ending point, then the beginning point, and then subtract (ending point expression - beginning point expression).
 
  • #7
so a= f and b= f-kv. so (f-kv)-f? making just -kv?
 
  • #8
to get rid of the ln don't i have to make something go to the e^??
 
  • #9
prezmoneymike said:
so a= f and b= f-kv. so (f-kv)-f? making just -kv?

You have to keep the natural log there for now. So the result of your integral is:

[tex]
\ln (f-kv) - \ln (f)
[/tex]

Then you can use this in your full expression. You will probably want to combine these natural logs (which is possible since they are being subtracted).

Later on, like you say you'll need to get rid of the ln by using the fact that:

[tex]
e^{\ln x} = x
[/tex]
 
  • #10
so ln(-kv). then take the whole expression to the e. Making it e^t/m= e^(-1/k) * -kv. would this be right?
 
  • #11
The way that these natural logs combine is by using the property:

[tex]
\ln a - \ln b = \ln \left(\frac{a}{b}\right)
[/tex]

so here you will get:

[tex]
\ln \left(\frac{ f-kv}{f}\right)
[/tex]
 
  • #12
ok then you would get e^t/m= e^(-1/k) * ((f-kv)/f)?
then would you solve for v? how would accomplish this?
 
  • #13
prezmoneymike said:
ok then you would get e^t/m= e^(-1/k) * ((f-kv)/f)?
then would you solve for v? how would accomplish this?

Before this step you had:

[tex]
\frac{t}{m} = -\frac{1}{k} \ln \left(\frac{f-kv}{f}\right)
[/tex]

Then move the k to the other side and take the natural log:

[tex]
\begin{align}
\frac{-kt}{m} &= \ln \left(\frac{f-kv}{f}\right)\nonumber\\
e^{-kt/m} &= \frac{f-kv}{f}\nonumber
\end{align}
[/tex]

and solve this for v.
 
  • #14
making it v= (f*e^-kt/m + f)/-k
v= (12360N*e^((-164)(12.25)/1547) + 12360N)/164
v= 95.93 m/s

but this doesn't make sense because in part b the max speed was found to be 75.37. so did i do something wrong? and how would i calculate distance for this and part d?
 
  • #15
prezmoneymike said:
making it v= (f*e^-kt/m + f)/-k
v= (12360N*e^((-164)(12.25)/1547) + 12360N)/164
v= 95.93 m/s

but this doesn't make sense because in part b the max speed was found to be 75.37. so did i do something wrong? and how would i calculate distance for this and part d?

I think your equation should be:

v = ( f e^{-k t /m} - f) / (-k)

because the f that was originally in the numerator on the right side was positive, and so gained a negative sign when you moved it to the left.
 
  • #16
ok now it is 55.34 That makes more sense. ok so how do i figure out the distance?
 
  • #17
Remember how we found the velocity: we had an equation with the acceleration (which is dv/dt), the velocity and the time, and then we integrated it.

So now, find an equation for velocity (which is dx/dt) at an arbitrary time t. (I think you can find one in the work you did in finding the velocity.) Then follow the same type of procedure. What do you get?
 
  • #18
yea i know what u mean i got it. thanks you so much for all your help. I think I've learned more from you than my calculus teacher lol. thanks again.
 

What are velocity differential equations?

Velocity differential equations are mathematical equations that describe the change in velocity of a particle or object over time. They are used in physics and engineering to model the motion of objects in various systems.

What is the significance of velocity differential equations?

Velocity differential equations are important because they allow us to predict the future motion of an object based on its current velocity and the forces acting on it. They are also used to understand the behavior of complex systems and make accurate predictions about their behavior.

What are the variables involved in velocity differential equations?

The variables involved in velocity differential equations are the velocity of the object (v), the time (t), and the acceleration (a). These variables can be expressed as functions of each other to create a differential equation.

What are some real-world applications of velocity differential equations?

Velocity differential equations have many practical applications, such as in predicting the motion of planets in our solar system, analyzing the behavior of fluids in pipes, and understanding the dynamics of moving objects in engineering and robotics.

What are some common methods for solving velocity differential equations?

Some common methods for solving velocity differential equations include separation of variables, Euler's method, and numerical integration. These methods involve breaking down the equation into simpler parts and using mathematical techniques to find a solution.

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