The Starship Enterprise (variable acceleration problem)

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Homework Help Overview

The discussion revolves around a variable acceleration problem involving the Starship Enterprise, which experiences a deceleration due to an intergalactic meteor shower. The force acting on the ship is described by the equation F = -b*e^([alpha]*v), where b and [alpha] are constants, and the ship's mass is m. Participants are tasked with determining the velocity function v(t), the time required for the ship to stop, and the position function x(t).

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the derivation of the velocity function v(t) from the force equation and question the validity of certain mathematical steps taken. There are attempts to clarify the integration process and the handling of initial conditions. Some participants express confusion over the implications of their results and the definitions of variables used.

Discussion Status

The discussion is ongoing, with participants exploring various interpretations of the problem and the mathematical steps involved. Some have provided guidance on correcting potential mistakes in the derivation process, while others are seeking clarification on specific points. There is no explicit consensus on the correct approach yet.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information they can share or the methods they can use. There is an emphasis on showing work and understanding the reasoning behind each step rather than simply arriving at a solution.

frankR
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The Starship Enterprise initially moving with speed vo hits an intergalctic metero shower and expreiences a deceleration force given by:

F = -b*e^([alpha]*v) where b and [alpha] are constants. The star ships mass is m.

a) Determine v(t).
b) Determine the time required for the Enterprise to stop.
c) Show that x(t) is given by: (a really ugly function I don't want to type)

I've solved it, however my x(t) function isn't like what is given. I certain that my math and physics is right. If someone could do the problem, I'm curious to know what you get.

For a)

Finding v(t)

F = -b*e^([alpha]*v) = m dv/dt

Solving for v(t) I get: ln[m/([alpha]*b*t)] + vo

b)

When the ship stops.

v(t) = 0 = ln[m/([alpha]*b*t)] + vo
t = 1/(b*[alpha])*m*e^(vo*[alpha])

c)

Find x(t):

v(t) = dx/dt = ln[m/([alpha]*b*t)] + vo

Solving for x(t) = t/[alpha]*{ln(m/([alpha]*b*t) + vo*t + 1} + xo

My teacher said this problem was difficult. However it seems very straight forward to me, unless I'm doing something completely wrong.

Thanks
 
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Originally posted by frankR
For a)

Finding v(t)

F = -b*e^([alpha]*v) = m dv/dt

Solving for v(t) I get: ln[m/([alpha]*b*t)] + vo

For starters, you have a glitch here. At some point you would have arrived at the step:

exp(-αv)=(αbt/m)+e(-αv0)

and from there you have to take the natural log to get to v(t). You made a mistake when you did that, namely you employed the step:

ln(a+b)=ln(a)+ln(b),

which is not valid.
 
I'm not sure what you mean. I have to go to class right now, no matter.:wink:

I redid the problem and came to the same answer. I must of made the same mistake.

Sometimes a repeatable result doesn't make you right, it just means you made the same mistake twice.
 
Originally posted by frankR
I'm not sure what you mean. I have to go to class right now, no matter.:wink:

OK, what I'm talking about is this:

exp(-αv)=αbt/m+exp(-αv0)

does not lead to:

-αv=ln(αbt/m)-αv0.

It leads to:

-αv=ln(αbt/m+exp(-αv0)).
 
Perhaps the previous comments will make more sense if you can answer this: What value of t are you using for the "initial" time?

If v(t)= ln[m/([alpha]*b*t)] + vo then v(0) is not defined.

What value of t gives v(t)= 0?

You may have solved the d.e. m dv/dt= -be[alpha]v

to get v(t)= ln(m/([alpha]*b*t) and then simply added vo: you can't do that.

mdv/dt= F= -be^([alpha]v) gives e^(-[alpha]v)dv= (-b/m)dt which integrates to (-1/[alpha])e^(-[alpha]v)= (-b/m)t+ C
or e^(-[alpha]v)= (b[alpha]/m) t+ C. (this C is -[alpha] times the old C but since they are both "undetermined constants" I won't make the distinction.)

We can determine C at this point. When t= 0, v= vo so
e^(-[alpha]vo)= C. Our equation is now
e^(-[alpha]v)= (b[alpha]/m)t+ e^(-[alpha]vo)

Taking logarithms of both sides we get

-[alpha]v= ln((b[alpha]/m)t+ e^(-[alpha]vo))

so v= -(1/[alpha])ln((b[alpha]/m)t+ e^(-[alpha]vo))

To determine when the boat will come to a stop, let v= 0:
-(1/[alpha])ln((b[alpha]/m)t+ e^(-[alpha]vo))=0
so (b[alpha]/m)t+ e^(-[alpha]vo)= 1

t= (1- e^([alpha]vo)(m/b[alpha])

v= dx/dt= -(1/[alpha])ln((b[alpha]/m)t+ e^(-[alpha]vo))

To integrate this, let u= (b[alpha]/m)t+ e^(-[alpha]vo))
then du= (b[alpha]/m)dt or dt= m/(b[alpha])du so
dx= -(m/b[alpha]^2)ln(u)du

Of course, the integral of ln(u) is u ln(u)- u so

x(t)= -(m/b[alpha]^2)(u ln(u)- u)+ C
= -(m/b[alpha]^2)(b[alpha]/m)t+ e^(-[alpha]vo))ln((b[alpha]/m)t+ e^(-[alpha]vo))- (b[alpha]/m)t+ e^(-[alpha]vo))))
 
HallsOfIvy,

Apparently, you have chosen not to receive Private Messages, so I have to post this here.

I appreciate all the time you spend here in the Homework forum. I would only ask you to stop posting complete solutions to the problems. I want the students to show their work and where they get stuck, then we can help through the rough spots. If we just give the solution away, then this will become a place where students run to when they don't feel like thinking, and that's not what I want.

Could you please edit the above solution? Then I will delete this post.

Thanks,
 
Okay.

So:

ln(e^([alpha](v - vo))) != [alpha](v - vo)

ln(e^([alpha](v - vo))) = e^[alpha]v/e^[alpha]vo ?
 
Last edited:

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