To find the length of the given curve, we first need to determine the parameterization of the curve and then use the arc length formula.
The arc length L of a curve defined by a vector function r(t) from a to b is given by the formula:
L = ∫_a^b ||r'(t)|| dt
where r'(t) is the derivative of r(t), and ||r'(t)|| is its magnitude.
Given the curve:
r(t) = cos(4t)i + sin(4t)j + 4ln(cos(t))k
We first compute the derivative:
r'(t) = d/dt [cos(4t)]i + d/dt [sin(4t)]j + d/dt [4ln(cos(t))]k
Using the chain rule:
r'(t) = -4sin(4t)i + 4cos(4t)j + 4[-sin(t)/cos(t)](1/cos(t))k
Which simplifies to:
r'(t) = -4sin(4t)i + 4cos(4t)j - 4tan(t)k
Next, we find the magnitude:
||r'(t)|| = sqrt((-4sin(4t))^2 + (4cos(4t))^2 + (-4tan(t))^2)
Calculating the squares:
||r'(t)|| = sqrt(16sin^2(4t) + 16cos^2(4t) + 16tan^2(t))
Using the identity sin^2(x) + cos^2(x) = 1 simplifies this to:
||r'(t)|| = 4sqrt(1 + tan^2(t))
Knowing that 1 + tan^2(t) = sec^2(t), we get:
||r'(t)|| = 4sec(t)
The arc length is now computed by integrating from 0 to π/4:
L = ∫_0^(π/4) 4sec(t) dt
The integral of sec(t) is ln|sec(t) + tan(t)| + C. Therefore:
L = 4[ln|sec(t) + tan(t)|]_0^(π/4)
Evaluating the limits:
At t = π/4, sec(π/4) = √2 and tan(π/4) = 1. Thus:
ln|√2 + 1|
At t = 0, sec(0) = 1 and tan(0) = 0. Thus:
ln|1| = 0
Therefore, substituting in these values gives:
L = 4[ln(√2 + 1) - 0] = 4ln(√2 + 1)
So the length of the curve from t = 0 to t = π/4 is:
L = 4ln(√2 + 1)