Step 1: Let the entry times (in minutes after 3 PM) be \(x,y \sim \text{Unif}[0,60]\). Each visitor stays on \([t,\,e(t)]\) where \[ e(t) = \begin{cases} t+20, & 0 \leq t < 40, \\ 60, & 40 \leq t \leq 60. \end{cases} \] Two visits do not overlap iff \(e(x)\le y\) or \(e(y)\le x\).
Step 2: For a fixed \(x \in [0,40)\): \(e(x) = x+20\). Non-overlap occurs for \(y \geq x+20\) or (if \(y<40\)) \(y \leq x-20\). Hence the measure in \(y\) is: \[ L(x) = \begin{cases} 40-x, & 0 \leq x < 20, \\ 20, & 20 \leq x < 40. \end{cases} \]
Step 3: For \(x \in [40,60)\): \(e(x)=60\). Non-overlap requires \(e(y)\leq x \;\Rightarrow\; y \leq x-20\) with \(y<40\). Thus: \[ L(x) = x-20, \quad 40 \leq x < 60. \]
Step 4: Compute the total non-overlap area in the \([0,60]\times[0,60]\) square: \[ A_{\text{no}} = \int_0^{20}(40-x)\,dx + \int_{20}^{40}20\,dx + \int_{40}^{60}(x-20)\,dx. \] Calculation: \[ A_{\text{no}} = 600 + 400 + 600 = 1600. \] Therefore: \[ \mathbb{P}(\text{no overlap}) = \frac{1600}{60^2} = \frac{4}{9}, \qquad \mathbb{P}(\text{overlap}) = 1 - \frac{4}{9} = \frac{5}{9}. \]
Final Answer: \[ \boxed{\; \mathbb{P}(\text{overlap}) = \tfrac{5}{9} \;} \]
The probability distribution of the random variable X is given by
| X | 0 | 1 | 2 | 3 |
|---|---|---|---|---|
| P(X) | 0.2 | k | 2k | 2k |
Find the variance of the random variable \(X\).
An ideal monoatomic gas is contained inside a cylinder-piston assembly connected to a Hookean spring as shown in the figure. The piston is frictionless and massless. The spring constant is 10 kN/m. At the initial equilibrium state (shown in the figure), the spring is unstretched. The gas is expanded reversibly by adding 362.5 J of heat. At the final equilibrium state, the piston presses against the stoppers. Neglecting the heat loss to the surroundings, the final equilibrium temperature of the gas is __________ K (rounded off to the nearest integer).
The residence-time distribution (RTD) function of a reactor (in min$^{-1}$) is 
The mean residence time of the reactor is __________ min (rounded off to 2 decimal places).}
Ideal nonreacting gases A and B are contained inside a perfectly insulated chamber, separated by a thin partition, as shown in the figure. The partition is removed, and the two gases mix till final equilibrium is reached. The change in total entropy for the process is _________J/K (rounded off to 1 decimal place).
Given: Universal gas constant \( R = 8.314 \) J/(mol K), \( T_A = T_B = 273 \) K, \( P_A = P_B = 1 \) atm, \( V_B = 22.4 \) L, \( V_A = 3V_B \).
The following data is given for a ternary \(ABC\) gas mixture at 12 MPa and 308 K:
\(y_i\): mole fraction of component \(i\) in the gas mixture
\(\hat{\phi}_i\): fugacity coefficient of component \(i\) in the gas mixture at 12 MPa and 308 K
The fugacity of the gas mixture is __________ MPa (rounded off to 3 decimal places).