Consider a random experiment where a spinner is spun, and the continuous random variable \(X\) represents the angle spun, measured in degrees over the interval \([0, 360)\).

The probability that \(X\) assumes any precise value, such as \(x = 125.333\ldots\), is zero due to the infinite number of possible outcomes within a continuous range. However, we can calculate the probability that \(X\) lies within an interval, such as \([90, 180]\). We can think of this as summing the probabilities over tiny subintervals within this range:$$\begin{aligned}P(90 \leq X \leq 180) &= \sum_{x \in [90, 180]} P(x \leq X < x + dx) \\
&= \sum_{x \in [90, 180]} \frac{P(x \leq X < x + dx)}{dx} \cdot dx\end{aligned}$$Here, \(dx\) represents an infinitesimally small interval, and the ratio, \(\frac{P(x \leq X < x + dx)}{dx}\) is the probability per unit length. We define this as the probability density function, \(f(x)=\frac{P(x \leq X < x + dx)}{dx}\). By the definition of integration, this summation becomes:$$P(90 \leq X \leq 180) = \int_{90}^{180} f(x) \, dx$$For a uniform spinner, the probability is evenly distributed across all angles, so the pdf is constant: \(f(x) = \frac{1}{360}\) for \(x \in [0, 360)\). Thus:$$\begin{aligned}P(90 \leq X \leq 180) &= \int_{90}^{180} \frac{1}{360} \, dx \\
&= \left[ \frac{x}{360} \right]_{90}^{180} \\
&= \frac{180}{360} - \frac{90}{360} \\
&= \frac{1}{4}\end{aligned}$$Hence, the probability of spinning an angle between 90 and 180 degrees is \(\frac{1}{4}\).