Collision problem using vectors

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Homework Help Overview

The discussion revolves around a collision problem involving two particles moving along defined trajectories represented by vector equations. The participants are tasked with demonstrating the conditions under which the particles collide and deriving an expression for the time of collision based on given vectors.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore vector relationships and coplanarity conditions to derive expressions for time and collision criteria. There are attempts to manipulate vector equations through cross products and dot products to reach the desired results. Some participants express uncertainty about the equivalence of derived expressions and the correctness of the book's answer.

Discussion Status

The discussion is ongoing, with participants sharing various approaches and partial solutions. Some have provided guidance on manipulating the equations, while others are questioning the validity of certain steps and the accuracy of the reference material. There is no explicit consensus on the final solution, but productive lines of reasoning are being explored.

Contextual Notes

Participants are working under the constraints of homework guidelines, which may limit the extent of assistance they can provide to one another. The condition v.(bxu)=v.(axu) is a focal point of discussion, with implications for the collision criteria being examined.

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Homework Statement



Two particles are moving on trajectories given by r=a+ut and r=b+vt respectively where a, b, u and v are constant vectors and t is the time. Show that the particles will collide if v.(bxu)=v.(axu) Obtain an expression for the time of the collision in terms of a, b, u and v. (I think I've done the parts so far.) Hence, or otherwise, show that the collision will take place at position r=b+((a.(bxu))/(v.(bxu))v

Homework Equations



If three vectors a, b, c are linearly dependent, a.(bxc)=o

The Attempt at a Solution



a+ut=b+vt
ut=(b-a)+vt
ut, vt, and b-a are coplanar. Since t is a scalar multiple, u, v, and b-a are coplanar.
v.((b-a)xu)=0
v.(bxu-axu)=o
v.(bxu)=v.(axu)

ut-vt=b-a
(u-v)t=b-a
t=mod(b-a)/mod(u-v)

I can't see how this expression for to is equivalent to ((a.(bxu))/(v.(bxu)), so I'm stuck.
 
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Any suggestions would be great. :)
 
Ok, here's a sample of how to do it. I haven't worked through the permutations to show that the answer is what same as what the book gives but here's a start.

(u-v)t=(b-a)

cross both sides with a, so,

(uxa-vxa)t=(bxa)

Now we want to turn both sides into scalars so we can divide, let's dot with v.

((uxa).v-(vxa).v))t=(bxa).v

(vxa).v=0 so,

(uxa).v)t=(bxa).v, hence,

t=((bxa).v)/((uxa).v). Now use cyclic permutations and the result from the first part to turn that into the books answer, if you can. You might. I'm not sure. I haven't chased it that far yet. Nor am I sure the book answer is even right. I haven't checked that either.
 
Dick said:
Ok, here's a sample of how to do it. I haven't worked through the permutations to show that the answer is what same as what the book gives but here's a start.

(u-v)t=(b-a)

cross both sides with a,
Start to cross both sides with u instead:
-(uxv)t=(uxb)-(uxa),

then dot product with a :

-a(uxv)t=a(uxb)

as (uxa) is perpendicular to a. The triple products are scalars, so

t=-a(uxb)/a(uxv)=a(bxu)/a(uxv).

You need to change the denominator to v(bxu) by cyclical permutation of the vectors and using the condition v.(bxu)=v.(axu)

ehild
 
ehild said:
Start to cross both sides with u instead:
-(uxv)t=(uxb)-(uxa),

then dot product with a :

-a(uxv)t=a(uxb)

as (uxa) is perpendicular to a. The triple products are scalars, so

t=-a(uxb)/a(uxv)=a(bxu)/a(uxv).

You need to change the denominator to v(bxu) by cyclical permutation of the vectors and using the condition v.(bxu)=v.(axu)

ehild

Yeah, I figured there was some permutation of those things that would work. But I was kind of hoping Lucy Yeats would figure it out instead.
 
Dick said:
Ok, here's a sample of how to do it. I haven't worked through the permutations to show that the answer is what same as what the book gives but here's a start.

(u-v)t=(b-a)

cross both sides with a, so,

(uxa-vxa)t=(bxa)

Now we want to turn both sides into scalars so we can divide, let's dot with v.

((uxa).v-(vxa).v))t=(bxa).v

(vxa).v=0 so,

(uxa).v)t=(bxa).v, hence,

t=((bxa).v)/((uxa).v). Now use cyclic permutations and the result from the first part to turn that into the books answer, if you can. You might. I'm not sure. I haven't chased it that far yet. Nor am I sure the book answer is even right. I haven't checked that either.
Instead of dotting with v, dot with u.

I.E. look at:
[itex]((\vec{u}\times\vec{a})\cdot\vec{u}-(\vec{x}\times\vec{a})\cdot\vec{u})t=(\vec{b} \times\vec{a})\cdot\vec{u}[/itex]​
Of course, [itex](\vec{u}\times\vec{a})\cdot\vec{u}=0[/itex]

Added in Edit:

I must have been asleep (as in not paying attention) when ehild made this same suggestion!
Sorry about that !
 
Last edited:
Dick said:
Yeah, I figured there was some permutation of those things that would work. But I was kind of hoping Lucy Yeats would figure it out instead.

Sorry Dick. But you directed the OP to a more difficult way than necessary, and I did not say more than you.

ehild
 
Last edited:
ehild said:
Sorry Dick. But you directed the OP to a more difficult way then necessary, and I did not say more than you.

ehild

Just trying to explain why I was being too lazy to work out the exact solution.
 
ehild said:
Start to cross both sides with u instead:
-(uxv)t=(uxb)-(uxa),

then dot product with a :

-a(uxv)t=a(uxb)

as (uxa) is perpendicular to a. The triple products are scalars, so

t=-a(uxb)/a(uxv)=a(bxu)/a(uxv).

You need to change the denominator to v(bxu) by cyclical permutation of the vectors and using the condition v.(bxu)=v.(axu)

ehild

BTW:

The condition v.(bxu)=v.(axu), can be obtained in a similar manner. Start with
[itex]\vec{a}+\vec{u}t=\vec{b}+\vec{v}t[/itex]​
Cross that with vector [itex]\vec{u}[/itex] then dot that with vector [itex]\vec{v}\,.[/itex]
 

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