Step 1: The Arrhenius equation.
The Arrhenius equation relates the rate constant \( k \) to temperature \( T \) and the activation energy \( E_a \):
\[
k = A e^{\frac{-E_a}{RT}}
\]
Taking the natural logarithm of both sides, we get:
\[
\ln k = \ln A - \frac{E_a}{RT}
\]
This is a linear equation of the form \( y = mx + b \), where the slope \( m \) is \( -\frac{E_a}{R} \). Thus, the activation energy can be found from the slope of the line.
Step 2: Using the slope to find activation energy.
The slope \( m = -\frac{E_a}{R} \), where \( R \) is the universal gas constant (\( R = 8.314 \, \text{J/mol·K} \)). The given slope is \( -2.55 \times 10^4 \, \text{K} \).
We can solve for \( E_a \) as follows:
\[
E_a = -mR = 2.55 \times 10^4 \times 8.314 = 2.12 \times 10^5 \, \text{J/mol}
\]
Step 3: Conclusion.
Thus, the activation energy is \( 2.12 \times 10^5 \, \text{J/mol} \), which corresponds to option (1).
A weight of $500\,$N is held on a smooth plane inclined at $30^\circ$ to the horizontal by a force $P$ acting at $30^\circ$ to the inclined plane as shown. Then the value of force $P$ is:
A steel wire of $20$ mm diameter is bent into a circular shape of $10$ m radius. If modulus of elasticity of wire is $2\times10^{5}\ \text{N/mm}^2$, then the maximum bending stress induced in wire is: