Motion with frictional force but without driving force

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LockeZz
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Hi guyz... I am having a problem with this question. Hope to get some guideline from here :D

An engine of mass m moves without driving force but under the influence of the frictional force f(v)=(alpha)+(Beta)v2 on horizontal rails. Let the initial velocity be v0.

(a) After which time does the engine come to rest? What is the maximum deceleration time (v0 approaching infinity )

(b)What distance has then been covered?
 
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Sorry... for being short in giving info..

given the frictional force function is f(v)=a+Bv2 .

i tried to substitute the initial velocity in side the function:

f(v0)=a+Bv20
ukFn=a+Bv20.

im stucked at here.. and i was thinking that i might need to get an expression which include the time..
 
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erm.. i want to ask about this.. how should i type in the greek symbol since the expression given a+bv^2 are actually represent by alpha and beta .

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so.. Newton 2nd law given F=ma .
should i substitute into the expression to get :

ma=(alpha)+(Beta)v20

?
 
Sorry for being messing up just now..For i have already edited the 1st post..

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for the general expression for all time, i obtain this :

(alpha)+(beta)v2=ma

a=[((alpha)+(beta)v2)/m]

so, i have try on further which i substitute the final velocity (which is 0) for part (a) and i get :

a=(alpha)/m
 
LockeZz said:
Sorry for being messing up just now..For i have already edited the 1st post..

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for the general expression for all time, i obtain this :

(alpha)+(beta)v2=ma
OK, but you did not write down the definition of the acceleration. That is a = dv/dt. So you get a differential equation

[tex]m\frac{dv}{dt}=\alpha+\beta v^2[/tex]

Can you solve this to get v(t), that is the velocity for any time t?
 
alright, for the v(t) function i derive from:

[tex] m\frac{dv}{dt}=\alpha+\beta v^2[/tex]

[tex] \int\frac{dv}{v^2}=\int(\frac{\alpha+\beta}{m})dt[/tex]

[tex] v=\frac{-m}{(\alpha+\beta)t}[/tex]
 
Haha.. what a silly mistake i have done.. Well i have try again on the derivation and i get this :

[tex] \int \frac {m}{\alpha+\beta v^2} dv =\int dt[/tex]

and I am need help on integrate this.. :cry:
 
Thx for reminding.. i have substitute with tangent theta and get the expression u shown.. then i do the further integration and i get this :

[tex] <br /> v=\alpha(\frac{t}{m}+c)[/tex]
 
i'm not quite sure in that case.. the 1st post shows all the statement given on the example.. and its tricky and confuse for me :(
 
LockeZz said:
i'm not quite sure in that case.. the 1st post shows all the statement given on the example.. and its tricky and confuse for me :(
There are no tricks involved, just organized thinking. Answer these questions

1. Does the velocity change? (Yes/No)
2. Does the force change? (Yes/No)
3. What is an expression for the acceleration in terms of the force?
4. Assuming that you correctly answered all of the above, is the acceleration changing? (Yes/No)
 
kuruman said:
There are no tricks involved, just organized thinking. Answer these questions

1. Does the velocity change? (Yes/No)
2. Does the force change? (Yes/No)
3. What is an expression for the acceleration in terms of the force?
4. Assuming that you correctly answered all of the above, is the acceleration changing? (Yes/No)


(1) yes the velocity is changing.
(2) the force is changing since the velocity is involve in the function of force
(3) F=ma
(4) it should be constant (i think) since it have stated the initial velocity to be v0 and then the engine stop its motion..
 
LockeZz said:
(1) yes the velocity is changing.
Correct.
(2) the force is changing since the velocity is involve in the function of force
Correct.
(3) F=ma
Correct.
(4) it should be constant (i think) since it have stated the initial velocity to be v0 and then the engine stop its motion..
Incorrect. The initial velocity is v0, not the velocity forever and ever. As you stated in (1) the velocity changes, therefore it cannot stay at v0. Now look at (2) and (3)

a = F/m. If F changes and m stays the same, can the acceleration stay the same?
 
hm.. so the acceleration is not constant.. does that means i need to derive acceleration function?
 
LockeZz said:
hm.. so the acceleration is not constant.. does that means i need to derive acceleration function?
You are not thinking. Take a good look at a = F/m. Do you know what F looks like? Yes. Therefore you have the acceleration as a function of velocity. You know that

[tex]a=\frac{dv}{dt}=\frac{1}{m}(\alpha + \beta \: v^2)[/tex]

What you need to do is the integral correctly. Your attempted solution implies that the acceleration is constant which, I hope I have convinced you, cannot be the case.
 
Alright... i think that if the acceleration is not constant.. then the v(t) derived should consist of t2 but. i have attempted to integrate again and i was unable to get it...
 
LockeZz said:
Alright... i think that if the acceleration is not constant.. then the v(t) derived should consist of t2 but. i have attempted to integrate again and i was unable to get it...
Not necessarily. Anyway, I gave you a substitution to try for the integration. What did you do with it? Show your work and I should be able to help you.
 
From :

[tex] v=\sqrt{\frac{\alpha}{\beta}}tan\theta[/tex]
[tex] dv=\sqrt{\frac{\alpha}{\beta}}sec^2\theta d\theta[/tex]

then i substitute into this integral:

[tex] \int \frac{1}{\alpha(1+(\sqrt{\frac{\alpha}{\beta}}v)^2}dv=\frac{1}{m}\int dt[/tex]

[tex] \int \frac{1}{\alpha(1+tan^2\theta)}(\sqrt{\frac{\alpha}{\beta}}sec^2\theta d\theta)=\frac{1}{m}\int dt[/tex]

[tex] \int \frac{1}{\alpha(sec^2\theta)}(\sqrt{\frac{\alpha}{\beta}}sec^2\theta d\theta)=\frac{1}{m}\int dt[/tex]

then i further simplify it..

[tex] \int\frac{1}{\alpha}\sqrt{\frac{\alpha}{\beta}} d\theta=\frac{1}{m}\int dt[/tex]

then integrate i get :
[tex] v=\alpha(\frac{t}{m}+c)[/tex]
 
oops.. i found my mistake..

after integrate i will get:
[tex] <br /> \sqrt{\frac{1}{\alpha\beta}}\theta=\frac{t}{m}+c[/tex]

from:
[tex] v=\sqrt{\frac{\alpha}{\beta}}tan\theta[/tex]
[tex] \theta=tan^-1\sqrt{\frac{\beta}{\alpha}}v[/tex]

then i substitute inside:
[tex] \sqrt{\frac{1}{\alpha\beta}}tan^-1\sqrt{\frac{\beta}{\alpha}}v=\frac{t}{m}+c[/tex]
 
What are your limits of integration? The lower limit for the theta integral is not zero. Remember at t = 0 (the lower limit for the integral on the right) v = v0. This means that the lower limit of the integral on the left is

[tex]\theta_0=ArcTan\left( v_0\sqrt{\frac{\beta}{\alpha}} \right)[/tex]
 
so the upper limit for theta will be 0? since the final velocity will be zero as the engine come to rest??
 
how to simplify the subtraction between the arctangent?