Calculating the Lioness' Meal: v_{L}>v_{G}

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A hungry lioness runs after a gazelle. [tex]v_{L}>v_{G}[/tex] are the constant magnitudes of the velocities of the two animals. The lioness always directs it's velocity towards the gazelle, the latter always runs in a straight line. Calculate when will the lioness eat the gazelle, as a function of the initial positions of the two animals in the savannah (the horizontal xy plane) and of the direction of the gazelle's speed.
 
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Sorry, I can only solve a similar problem where a cat chases a mouse.

You have to help me out here:

SHOW ME YOUR HOMEWORK SO FAR!
 
...it's about 10 years I don't have to do homework, luckily...:smile:

Anyway...
...in the rest frame of the gazelle, or the mouse, or the thief...
...in plane polar coordinates [tex]r,\alpha[/tex]...
...I found...

[tex]\dot r=-v_L-v_G\cos\alpha[/tex]

[tex]r\dot\alpha=-v_G\sin\alpha[/tex]

Theese should be the equations of motion.
The first one can be replaced by

[tex]v_G\ddot\alpha\sin\alpha+v_L\dot\alpha^2=0[/tex]

But I can't go any further!
 
Now, I am unsure as to why polar coordinates would be your salvation here.

I suggest that you first try the following special case:

The direction the gazelle will run in is orthogonal to the line connecting the initial positions of the gazelle and lioness.

Try and set up a set up equations of motion in the ground's rest frame; let for example the gazelle run up along the y-axis.

I'll help you out if you get stuck.
 
In the rest frame it should be [tex](x_G,y_G)=(0,v_Gt)[/tex] and

[tex]\dot x=\frac{-vx}{[x^2+(v_Gt-y)^2]^{1/2}}[/tex]

[tex]\dot y=\frac{v(v_Gt-y)}{[x^2+(v_Gt-y)^2]^{1/2}}[/tex]

(I suppressed the index L for readability).
I thought this looked awful, that's why I used polar coordinates. But maybe you have got the clue here?

EDIT:

Oh yeah and you can write

[tex]\frac{\dot x}{x}=\frac{\dot y}{y-v_Gt}[/tex]

that looks better, but I still can't solve!
 
Last edited:
Petr Mugver said:
Oh yeah and you can write

[tex]\frac{\dot x}{x}=\frac{\dot y}{y-v_Gt}[/tex]

that looks better, but I still can't solve!

1. This can be written as:
[tex]x\frac{\dot{y}}{\dot{x}}=(y-v_{G}t)(1)[/tex]

2. Now we have:
[tex]\frac{\dot{y}}{\dot{x}}=\frac{dy}{dx}(2)[/tex]

Now, we need to eliminate "t" from (1)!
Remember that:
[tex]\int_{0}^{t}\sqrt{\dot{x}^{2}+\dot{y}^{2}}dt=v_{L}t[/tex]
The integral, can, however, be rewritten, in terms of an arbitrary x as:
[tex]t=\frac{1}{v_{L}}\int_{x_{0}}^{x}\sqrt{1+(\frac{dy}{dx})^{2}}dx[/tex]
whereby we get:
[tex]\frac{dt}{dx}=\frac{\sqrt{1+(\frac{dy}{dx})^{2}}}{v_{L}}[/tex]

Now, let us differentiate (1) with respect to x:
[tex]\frac{dy}{dx}+x\frac{d^{2}y}{dx^{2}}=\frac{dy}{dx}-\frac{v_{G}}{v_{L}}\sqrt{1+(\frac{dy}{dx})^{2}}[/tex]
which is, at first a separable equation for the variable Y=dy/dx:
[tex]x\frac{dY}{dx}=-\frac{v_{G}}{v_{L}}\sqrt{1+Y^{2}}[/tex]