Trajectories with Conserved Quantities

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Homework Help Overview

The discussion revolves around the motion of a particle along a trajectory with constant velocity and angular momentum. Participants are exploring the implications of these conserved quantities on the possible shapes of the trajectory, including straight lines, circles, and helices.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the implications of constant angular momentum and the conditions under which it can be maintained. Questions arise about the relationship between position and velocity vectors and how these affect the trajectory's shape.

Discussion Status

The conversation is ongoing, with participants providing insights into the nature of angular momentum and its effects on trajectory shapes. Some guidance has been offered regarding the mathematical relationships involved, but there is no consensus on the completeness of the identified trajectory types.

Contextual Notes

Participants are considering the constraints imposed by the problem's conditions, such as the requirement for constant velocity and angular momentum, and are questioning the completeness of the identified trajectory options. There is also mention of the need for initial conditions in solving differential equations related to the trajectories.

tvolanth
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Homework Statement


A particle moves along a trajectory with constant magnitude of the velocity |[itex]\stackrel{→}{v}[/itex]|=[itex]\stackrel{→}{v<sub>0</sub>}[/itex] and constant angular momentum L⃗ = L⃗0. Determine the possible trajectories.

Homework Equations



d(L⃗)/(dt)=[itex]\stackrel{→}{N}[/itex] where [itex]\stackrel{→}{N}[/itex]=torque

[itex]\stackrel{→}{N}[/itex]=[itex]\stackrel{→}{r}[/itex]x[itex]\stackrel{→}{F}[/itex]

F=ma

The Attempt at a Solution



I thought that there would be 3 paths that it could take

(i) a strait line if its in a strait line it can have constant velocity and no change in angular momentum, because torque is 0, because there is no Force.

(ii) a circle because force is parallel to the radius, there is no torque, means no change in angular momentum, and uniform circular motion has a constant |v|.

(iii) helix just like a combination of a strait line and a circle. both there is no change in angular momentum, so together there should be no change as well. (no force in any direction besides parallel to radius). also since there is constant |v| in the uniform circle, and now you are applying a constant v in a direction perpendicular to the v of the circle, the new |v| magnitude should be constant as well.

So my question is, are these are correct? if so are they the only three? and also if so, how do I know there all no others? (is there anyway to prove these are the only 3)

if it helps at all the title to this problem as my teacher gave is (Trajectory with conserved quantities)

Thank you for your help!
 
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I would start by analysing the implications of constant angular momentum. What restrictions does that impose on the trajectory?
 
I am thinking that implies that there is no torque, which would mean that the angular velocity remains constant? so that would mean that there either needs to me no external force or a force that is always in the direction of of the radius.
 
Note that my question was about implications on the trajectory. How does that affect its shape?
 
Well it would mean that the radius of the curve would either have to stay constant, or the velocity would need to change with it. So that combined with the constant velocity stipulation would mean that the particle would have to keep a constant radius from some origin.

But I don't this isn't entirely true, because the angle between the radius and the velocity can change as the length of the radius changes, keeping rxmv a constant. I think this is the case for a strait line.
 
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I do not think it implies that "either - or" statement. I cannot see how you arrived at that conclusion, anyway. A more specific question, with a bit of a hint: what does that mean about mutual orientation of the position and velocity vectors?
 
hmm. well the parallelogram that the vectors of position and velocity make would have to remain a constant area...

if R*M*V*sin(theta) remains a constant that angular momentum is conserved. but wouldn't that mean that any of those 4 values could change if one of the other changes inversely to it. so the angle between the position and velocity vectors can change if say the velocity or radius changes. since V and M are constant in this example, then R*sin(theta)=constant so either R and theta stay the same, or the both change at the same rate.
 
Remember that angular momentum is a vector. It has a direction. And because the vector is constant, the direction is constant. What does that mean about the position and the velocity? How are they related to the direction of the angular momentum?
 
means that velocity vector and position vector always have to lie on the same 2 diminutional plane. which would mean angular momentum isn't constant in a helix.
 
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  • #10
Exactly. (Dimensional is the correct word.) What does that tell you about the third options you enumerated originally?

Now, there is a catch. What if angular momentum is zero? There is no direction in that case. Do we have a useful relationship between position and velocity in this case?
 
  • #11
so angular momentum would not be constant in the helix.
If angular momentum is zero then the position and velocity vectors would either have to be parallel (or antiparallel) or one of them would have to be zero. doesn't make sense that a moving particles position or velocity vectors would be zero, so there fore they would have to be parallel.

and since the origin location is arbitrary, for any strait line you can place the origin so the position vector and velocity vectors are always parallel.
 
  • #12
So, when angular momentum is zero, the trajectory is?

Now let's go back to the case when it is not zero and we have a plane of motion. Because we have the plane, we can describe the trajectory in that plane using two coordinates, x and y. What is the magnitude of angular momentum in these coordinates? And what about the magnitude of velocity?
 
  • #13
Magnitude of velocity is Sqrt([itex]\dot{x}[/itex]^2+[itex]\dot{y}[/itex]^2)

the magnitude of the angular momentum would be ([itex]\dot{x}[/itex]y- [itex]\dot{y}[/itex]x)m

I got this just by taking the cross product of the velocity and position vectors

v={[itex]\dot{x}[/itex],[itex]\dot{y}[/itex],0}

r={x,y,0}
 
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  • #14
Well, at this stage you should just try and solve the differential equations you got. If you get really stuck, come back.
 
  • #15
so i took the derivative of x'y-y'x and set it equal to zero. (no change in angular momentum) and got x''y=y''x.

and the derivative of sqrt(x'^2+y'^2) and got ((x'x''+y'y'')/(sqrt(x'^2+y^2))=0

the problem is i don't really know what I'm looking for. I am not sure what the equation can tell me about the trajectories or what value i am trying to solve for.

how do I go about solving a diff equation were there are 2 variables both derived with respect to t?

also wouldn't i need some type of initial condition? I really have no idea what to do at this point
 
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  • #16
Very well. The final equation implies ## \dot x \ddot x + \dot y \ddot y = 0 ##. Its left hand side is the time derivative of ## \frac 1 2 (x^2 + y^2) ##.
 
  • #17
is that supposed to be ½([itex]\dot{x}[/itex]^2+[itex]\dot{y}[/itex]^2)? which would equal some constant.

And I'm still unsure as to what that then tells me. I am really struggling to understand where this is headed. I'm assuming in the end I want some equation for r(x,y;t) Sorry for being so difficult lol
 
  • #18
In the end you should obtain an equation or equations linking ##x## and ##y## and some constants. That will give you the (families of) trajectories. I think you can test with the equations obtained in #13 that options (i) and (ii) of #1 are valid. But to prove that no other options are possible, you have to solve those equations.

In my post #16, I made a mistake because I hoped very much to see ## x^2 + y^2 = c^2 ## (without dots) in your results. It can be derived from the basic equations of #13. And the steps you took - differentiating those equations - are steps in the right direction. You just need some more symbol gymnastics to get there.
 

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