Hi,
I doing some work on "Acceleration depending on time". I cannot do
part (b) of the following question. Can anyone help out? It would
be helpful to me if you could also show your steps and a small
commentary to help my understanding. Thanks.
A particle P moves along the positive x-axis. Its acceleration is
(x + 3)ms-2 when its displacement from the origin O is x
metres. Given that initially, when t=0, the velocity of P is
3ms-1 in the direction of Ox and x=0 , obtain
(a) the speed v ms-1 of P as a function of x
(b) x as a function of t
(a)
here's what I did:
0.5v2 = ò
(x+3) dx + A
if x=0 and v=3
after evaluation, v = x + 3
(b)
not sure of what do here
Thanks in advance for any help.
Hi,
First, your answer to part (a) is correct, and it looks like you're
going about it the right way. Here's how I did it:
KE gained by particle = work done on particle
mv2/2 - mu2/2 = ò F.dy = ò
ma.dy
v2 - u2 = 2.ò a.dy
v2 - 32 = 2.ò (x + 3).dy = 2[y2/2 + 3y],
evaluated between y = x and y = 0
v2 - 32 = 2(x2/2 + 3x) =
x2 + 6x
v2 = x2 + 6x + 9 = (x + 3)2
v = ±(x + 3)
But you know to take the +ve square root because v = 3 (not -3)
when x = 0.
For part (b), we have
dv/dt = a = x + 3 = v
and so we have the differential equation
dv/dt - v = 0
with solutions
v = Aet
Then v = x + 3 and so x = v - 3, so
x = Aet - 3
but since x = 0 when t = 0, 0 = A - 3, so A = 3 and
x = 3et - 3
I hope that was clear enough. If not, please let me know.
If you couldn't do that then please be reassured by the fact that
it took me about half an hour to realise how to do that question
(it's been quite a long time since I did any of these sort of
questions).
James.
Another way to do (b) is:
You have v=dx/dt=x + 3
So ò1/(x + 3) dx =ò 1 dt
so ln(x+3)=t+c
x=et+c-3
x=Aet-3
and apply the initial conditions like James has.
I don't know whether you have done enough calculus for this, but if
you have then I think this is generally a nicer way of doing it.
You can often apply what you had in a previous part of the problem
to later parts like this. When you can it tends to be faster.
Hope that gives you some more insight.
Susan
Cool! - 2 methods to get to the solution.
Thanks James and Susan! Your help very much appreciated.
I can't figure out part (b), can anyone help.
A particle P of mass 1.5kg moves in a straight line through a fixed
point O. At time t sec after passing through O the distance of P
from O is x cm and the force acting on P has magnitude (3x + 6)N
and directed away from O. Given that P passes through O with speed
2(2)0.5 ms-1 calculate, (a) speed of P then
x=5, (b) the value of t when x=20
(a) f=ma, ò 3x + 6 dx =
0.5mv2 ==> (3/2)x2 6x + c =
(1/2)(3/2)v2, but c=6, when v=2(2)0.5 and x
=0, hence (3/2)x2 6x + 6 = (1/2)(3/2)v2 and v
= 9.90ms/sec
(b) not sure what to do?
Thanks
I have a feeling I've made an error, but I'll go ahead and post
just to see if I have.
here's my logic:
If
v=
dx/dt=3x2+6x+6
then
dt/dx=1/(3x2/2+6x+6
let u=3x2/2+6x+6
then dx=u-1/2du
So
t=òu-1(u-1/2 du)
Thus
t=-2u-1/2+c
=-2(3x2+6x+6)-1/2+c
At t=0, x=0
So
c=2/sqrt(6)
and at x=20,
this equals
t=2/(13261/2+61/2)
(remembering a sqrt can be either plus or minus)
This isn't a very nice solution, which leads me to believe I've
made a mistake, but I can find none, so I'll post to see what
others have to say about this. Sorry if this isn't much of a help,
at least this method should work.
Brad
Hi Brad,
Thanks! I am gonna read through your logic to see if I understand.
The answer that they give in the book is 1.70sec if thats any help.
Okay, I think I've come up with a niceish
way of doing b):
a=F/m=(3x+6)/1.5=2x+4
so d2x/dt2-2x=4
Solve this differential equation:
Particular Integral is -2
Complimentrary function is
Ae20.5t+Be-20.5t
So x=Ae20.5t+Be-20.5t-2
But when t=0, x=0 and v=21.5
so A+B=2 and
v=A×20.5e20.5t-B×20.5e
-20.5t
so 21.5=A×20.5-B×20.5
sp A-B=2
so x=2e20.5t-2
so at x=20, e20.5t=11 so
t=ln(11)/20.5=1.70(3sf)
Hope this helps. Using this method does assume you have done some
differential equations though.
Okay, I've now looked over what you two
have done and have got some comments.
Firstly, anon: Why is c=6? You seem to have lost a plus between
(3/2)x2 and 6x. Why can you differentiate over x less
than 0? The initial conditions don't seem to allow that.
So this is I would integrate the energy change since time 0:
ò0 x3x+6
dx=0.5mv2-0.5mu2=(3/4)v2-(3/4)×8
(as u=21.5 so u2=8)
so (3/2)x2+6x=(3/4)v2-6
v2=2x2+8x+8
so when x=5 v2=98 and v>0 as accelaration always
positive and initial v positive. so v=9.90(3sf). It looks like you
just forgot about the plus, but this is a sounder method as you
don't integrate below x=0. It's not that critical though...
So, Brad, where did that expression for v come from? Where did that
expression for dx come from? There are also several arithmetical
errors along the way. For instance in the final expression of t,
you seem to have lost a minus sign (and no you shouldn't really
just say the sqrt is plus or minus like that, you could have
choosen the correct root earlier or mained a ± thoughout)
and the fact that they are two separate fractions.
Sorry to be harsh, so points are being fairly picky, so feel free
to ignore those that seem unimportant if you want.
Susan
I got the expression for v from looking at anon's post and not
seeing the 1/2×3/2v2 part. Oops. (I was in
somewhat of a hurry, so I didn't bother to do the integration
myself) And I really hadn't had a problem like this before, so I
had no idea what to do with the square roots.
Thanks for clearing that up,
Brad
Hi Susan,
c=6 came from the eqn when v^2 had still a coefficient to it. but
the way you did this part (a) is also correct! since you do not get
a constant of integration on int (F(x)) = 0.5mv2 -
0.5mu2, no c exits!
I still don't understand how you solved part b), can anyone explain
it any simpler methods. thanks,
OK, we have
v(dv/dx)=4+2x, v=2sqrt(2) when x=0, giving
v2=2(x+2)2
Square rooting both side and remember v is positive when x=0, we
obtain
v=(x+2)×sqrt(2)
but v=dx/dt, substitute and rearrange the equation to give
ò0 20dx/(x+2)=sqrt(2)t
Evaluating the integral, we have
t=sqrt(0.5)×ln(11)=1.70 seconds, to 3 s.f.
Kerwin
Gee whiz. Thanks, you people are great!
Thanks Kerwin!
Also thanks to Brad & Susan!
I think I sort of got into trouble when I thought "how do I get V
on its own, so I can sub in dx/dt" I sqrooted the whole lot and saw
it looked very messy. You factorised it good, i did'nt see that,
becuase I left in in the form where v still had its coefficient.
But now its all clear! Kerwin, in the step where you integrated, I
am not sure why we don't include a constant on integration, can you
briefly explain for me? Thanks.
Well, I am a bit lazy that I don't want to
work out constants. Instead, I substitute the initial conditions as
the lower limit for the integral, to save writing arbitrary
constants all over the place.
Kerwin