Step 1: Substitute \( t = 1 \) into the expression.
We start by substituting \( t = 1 \) into the limit expression: \[ \lim_{t \to 1} \frac{\ln t}{t^2 - 1} = \frac{\ln(1)}{1^2 - 1} = \frac{0}{0}. \] This results in an indeterminate form of \( \frac{0}{0} \), so we need to apply L'Hopital's Rule.
Step 2: Apply L'Hopital's Rule.
L'Hopital's Rule states that if the limit results in a \( \frac{0}{0} \) indeterminate form, we differentiate the numerator and denominator separately and then take the limit. Let's differentiate the numerator and denominator:
The derivative of \( \ln t \) is \( \frac{1}{t} \).
The derivative of \( t^2 - 1 \) is \( 2t \).
Therefore, applying L'Hopital's Rule, we get: \[ \lim_{t \to 1} \frac{\ln t}{t^2 - 1} = \lim_{t \to 1} \frac{\frac{1}{t}}{2t}. \] Step 3: Simplify and evaluate the limit.
Now simplify the expression: \[ \frac{\frac{1}{t}}{2t} = \frac{1}{2t^2}. \] Substitute \( t = 1 \): \[ \frac{1}{2(1)^2} = \frac{1}{2}. \] Thus, the value of the limit is \( 1 \).
Step 4: Conclusion.
Therefore, the correct value of the limit is \( 1 \), so the answer is \( \boxed{A} \).
A closed system is undergoing a reversible process 1–P–2 from state 1 to 2, as shown in the figure, where X and Y are thermodynamic properties. An irreversible process 2–Q–1 brings the system back from 2 to 1. The net change in entropy of the system and surroundings during the above-mentioned cycle are _______ respectively.
A ship of 3300 tonne displacement is undergoing an inclining experiment in seawater of density 1025 kg/m\(^3\). A mass of 6 tonne is displaced transversely by 12 m as shown in the figure. This results in a 0.12 m deflection of a 11 m long pendulum suspended from the centerline. The transverse metacenter of the ship is located at 7.25 m above the keel.
The distance of the center of gravity from the keel is ________ m (rounded off to two decimal places).
A multi-cell midship section of a ship with \( B = 40 \, {m} \) and \( D = 20 \, {m} \) is shown in the figure. The shear-flows are given as \( q_1 = q_2 = q_3 = 0.9376 \, {MN/m} \). The applied twisting moment on the midship section is ___________ MN·m (rounded off to two decimal places).
Consider a weightless, frictionless piston with a 2 kg mass placed on it as shown in the figure. At equilibrium in position 1, the cylinder contains 0.1 kg of air. The piston cross-sectional area is 0.01 m2. The ambient pressure in the surroundings outside the piston-cylinder arrangement is 0 bar (absolute). When the mass above the piston is removed instantaneously, it moves up and hits the stop at position 2, which is 0.1 m above the initial position.
Assuming \( g = 9.81 \, {m/s}^2 \), the thermodynamic work done by the system during this process is ________ J (answer in integer).