Math Problem Statement

A flow line (or streamline) of a vector field F is a curve r(t) such that dr dt = F(r(t)). If F represents the velocity field of a moving particle, then the flow lines are paths taken by the particle. Therefore, flow lines are tangent to the vector field. Show that the given curve c(t) is a flow line of the given velocity vector field F(x, y, z). c(t) =

e4t, ln(|t|), 1 t

, t ≠ 0; F(x, y, z) =

4x, z, −z2

Solution

To determine if the curve c(t)=(e4t,ln(t),1t)c(t) = \left( e^{4t}, \ln(|t|), \frac{1}{t} \right) is a flow line of the vector field F(x,y,z)=(4x,z,z2)F(x, y, z) = (4x, z, -z^2), we need to show that drdt=F(r(t))\frac{dr}{dt} = F(r(t)). Here, r(t)=c(t)r(t) = c(t), and we’ll differentiate c(t)c(t) with respect to tt and compare it to F(c(t))F(c(t)).

  1. Differentiate c(t)c(t): c(t)=(e4t,ln(t),1t)c(t) = \left( e^{4t}, \ln(|t|), \frac{1}{t} \right) We’ll find dcdt\frac{dc}{dt} by differentiating each component of c(t)c(t) with respect to tt:

    • For the xx-component: x(t)=e4tx(t) = e^{4t}. dxdt=ddte4t=4e4t\frac{dx}{dt} = \frac{d}{dt} e^{4t} = 4e^{4t}

    • For the yy-component: y(t)=ln(t)y(t) = \ln(|t|). dydt=ddtln(t)=1t\frac{dy}{dt} = \frac{d}{dt} \ln(|t|) = \frac{1}{t}

    • For the zz-component: z(t)=1tz(t) = \frac{1}{t}. dzdt=ddt(1t)=1t2\frac{dz}{dt} = \frac{d}{dt} \left( \frac{1}{t} \right) = -\frac{1}{t^2}

    Therefore, the derivative dcdt\frac{dc}{dt} is: dcdt=(4e4t,1t,1t2)\frac{dc}{dt} = \left( 4e^{4t}, \frac{1}{t}, -\frac{1}{t^2} \right)

  2. Evaluate F(c(t))F(c(t)): Now, we substitute x=e4tx = e^{4t}, y=ln(t)y = \ln(|t|), and z=1tz = \frac{1}{t} into F(x,y,z)F(x, y, z): F(x,y,z)=(4x,z,z2)F(x, y, z) = (4x, z, -z^2) Substituting, we get: F(c(t))=(4e4t,1t,(1t)2)F(c(t)) = \left( 4 \cdot e^{4t}, \frac{1}{t}, -\left( \frac{1}{t} \right)^2 \right) Simplifying the last component: F(c(t))=(4e4t,1t,1t2)F(c(t)) = \left( 4e^{4t}, \frac{1}{t}, -\frac{1}{t^2} \right)

  3. Compare dcdt\frac{dc}{dt} and F(c(t))F(c(t)): We have: dcdt=(4e4t,1t,1t2)\frac{dc}{dt} = \left( 4e^{4t}, \frac{1}{t}, -\frac{1}{t^2} \right) and F(c(t))=(4e4t,1t,1t2)F(c(t)) = \left( 4e^{4t}, \frac{1}{t}, -\frac{1}{t^2} \right)

    Since dcdt=F(c(t))\frac{dc}{dt} = F(c(t)), this confirms that c(t)c(t) is indeed a flow line of the vector field F(x,y,z)F(x, y, z).

Would you like further clarification on this result or additional details?

Here are some related questions for further exploration:

  1. How would the flow line change if the vector field F(x,y,z)F(x, y, z) were different?
  2. What is the physical interpretation of flow lines in fluid dynamics?
  3. Can flow lines intersect in a vector field? Why or why not?
  4. How would you find the flow line through a different initial point in the same vector field?
  5. What are streamlines, and how are they related to flow lines?

Tip: Always check if the vector field’s dimensions and the curve’s dimensions match to ensure the possibility of them being flow lines.

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Math Problem Analysis

Mathematical Concepts

Vector Fields
Differentiation
Parametric Curves
Flow Lines

Formulas

dr/dt = F(r(t))
c(t) = (e^{4t}, ln(|t|), 1/t)

Theorems

Differentiation of Parametric Equations

Suitable Grade Level

Undergraduate