Concept:
Frequency response analysis evaluates how a system reacts to stable sinusoidal inputs. For a given input frequency \( \omega \), the output of a linear system is also a sinusoid of the same frequency, but shifted in phase by an angle \( \phi \).
Step 1: Finding the standard expression for a first-order phase shift.
The standard transfer function of a first-order process is represented in the Laplace domain as:
\[
G(s) = \frac{K}{\tau s + 1}
\]
Where \(\tau\) is the process time constant. Substituting \( s = j\omega \) to perform the frequency domain mapping gives:
\[
G(j\omega) = \frac{K}{j\omega\tau + 1}
\]
The phase angle \(\phi\) is calculated as the argument of the complex transfer function:
\[
\phi = \angle G(j\omega) = \angle K - \angle(1 + j\omega\tau)
\]
Since \(K\) is a real positive constant scalar, its angle is \(0^\circ\). Thus:
\[
\phi = 0 - \tan^{-1}(\omega\tau) = -\tan^{-1}(\omega\tau)
\]
Step 2: Substituting the given numerical values.
The problem statement provides the following specific operational values:
• Time constant, \( \tau = 1 \text{ minute} \)
• Input frequency, \( \omega = 1 \text{ radian/minute} \)
Plugging these metrics directly into our phase shift equation:
\[
\phi = -\tan^{-1}(1 \times 1) = -\tan^{-1}(1)
\]
Since \(\tan(45^\circ) = 1\), the inverse tangent of 1 is \(45^\circ\) (or \(\frac{\pi}{4}\) radians):
\[
\phi = -45^\circ
\]
The negative sign indicates a phase lag, meaning the output sine wave trails behind the input sine wave by \(45^\circ\).