Radiodrome

In geometry, a radiodrome is the pursuit curve followed by a point that is pursuing another linearly-moving point. The term is derived from the Greek words "ῥάδιος" (easier) and "δρόμος" (running). The classic (and best-known) form of a radiodrome is known as the "dog curve"; this is the path a dog follows when it swims across a stream with a current after food it has spotted on the other side. Because the dog drifts downwards with the current, it will have to change its heading; it will also have to swim further than if it had computed the optimal heading. This case was described by Pierre Bouguer in 1732.

A radiodrome may alternatively be described as the path a dog follows when chasing a hare, assuming that the hare runs in a straight line at a constant velocity. It is illustrated by the following figure:

Graph of a radiodrome, also known as a dog curve

Mathematical analysis

Introduce a coordinate system with origin at the position of the dog at time zero and with y-axis in the direction the hare is running with the constant speed V_t. The position of the hare at time zero is (Ax, Ay) and at time t it is

(T_x\ ,\ T_y)\ =\ (A_x\ ,\ A_y+V_t t)

 

 

 

 

(1)

The dog runs with the constant speed V_d towards the instantaneous position of the hare.

The differential equation corresponding to the movement of the dog, (x(t), y(t)), is consequently

 \dot x= V_d\ \frac{T_x-x}{\sqrt{(T_x-x)^2+(T_y-y)^2}}

 

 

 

 

(2)

 \dot y= V_d\ \frac{T_y-y}{\sqrt{(T_x-x)^2+(T_y-y)^2}}

 

 

 

 

(3)

It is possible to obtain a closed-form analytic expression y=f(x) for the motion of the dog, From (2) and (3) it follows that

y'(x)=\frac{T_y-y}{T_x-x}

 

 

 

 

(4)

Multiplying both sides with T_x-x and taking the derivative with respect to x using that

 \frac{dT_y}{dx}\ =\ \frac{dT_y}{dt}\ \frac{dt}{dx}\ =\ \frac{V_t}{V_d}\ \sqrt{{y'}^2+1}

 

 

 

 

(5)

one gets

 y''=\frac{V_t\ \sqrt{1+{y'}^2}}{V_d(A_x-x)}

 

 

 

 

(6)

or

 \frac{y''}{\sqrt{1+{y'}^2}}=\frac{V_t}{V_d(A_x-x)}

 

 

 

 

(7)

From this relation it follows that

 \sinh^{-1}(y')=B-\frac{V_t}{V_d}\ \ln(A_x-x)

 

 

 

 

(8)

where B is the constant of integration determined by the initial value of y' at time zero, y' (0)= sinh(B − (Vt /Vd) lnAx), i.e.,

 B=\frac{V_t}{V_d}\ \ln(A_x)+\ln\left(y'(0)+\sqrt{{y'(0)}^2+1}\right)

 

 

 

 

(9)

From (8) and (9) it follows after some computations that

 y'= \frac{1}{2}\left(\frac{y'(0)+\sqrt{{y'(0)}^2+1}}{(1-\frac{x}{A_x})^{\frac{V_t}{V_d}}}  - \frac{(1-\frac{x}{A_x})^{\frac{V_t}{V_d}}}{y'(0)+\sqrt{{y'(0)}^2+1}}\right)

 

 

 

 

(10)

If, now, Vt ≠ Vd, this relation integrates to

 y= C - \frac{1}{2}\ A_x\left( 
\frac{(y'(0)+\sqrt{{y'(0)}^2+1})\ (1-\frac{x}{A_x}) ^{1 - \frac{V_t}{V_d}} }{1-\frac{V_t}{V_d}} -
\frac{ (1-\frac{x}{A_x}) ^{1 + \frac{V_t}{V_d}} }{ (y'(0)+\sqrt{{y'(0)}^2+1})\ (1 + \frac{V_t}{V_d}) } 
\right)

 

 

 

 

(11)

where C is the constant of integration.

If Vt = Vd, one gets instead

 y= C -\frac{1}{2}A_x\ \left(\left(y'(0)+\sqrt{{y'(0)}^2+1}\right)\ \ln(1-\frac{x}{A_x})   -
\frac{ (1-\frac{x}{A_x})  ^2}{(y'(0)+\sqrt{{y'(0)}^2+1})\ 2}\right)

 

 

 

 

(12)

If Vt < Vd, it follows from (11) that

 \lim_{x \to A_x}y(x) = C = \frac{1}{2}\ A_x\left( \frac{y'(0)+\sqrt{{y'(0)}^2+1} }{1-\frac{V_t}{V_d}} - \frac{1}{ (y'(0)+\sqrt{{y'(0)}^2+1})\ (1 + \frac{V_t}{V_d}) } \right)

 

 

 

 

(13)

In the case illustrated in the figure above, Vt Vd = 11.2 and the chase starts with the hare at position (Ax, −0.6 Ax) which means that y'(0) = −0.6. From (13) it thus follows that the hare is caught at position (Ax, 1.21688Ax), and consequently that the hare will have run the total distance (1.21688 + 0.6) Ax before being caught. The arclength of the dog's path is (13) multiplied by Vd Vt =1.2 .

If Vt ≥ Vd, one has from (11) and (12) that \lim_{x \to A_x}y(x) = \infty, which means that the hare will never be caught, whenever the chase starts.

See also

References

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