Step 1: State the given data.
The initial pressure inside the tyre, \( P_i \), is 4 times the atmospheric pressure \( P_a \):
\[
P_i = 4P_a
\]
The initial temperature, \( T_i \), is given as:
\[
T_i = 300K
\]
Step 2: Apply the adiabatic process for an ideal gas.
For an adiabatic process, the relation between pressure and temperature is given by:
\[
P_i T_i^{\frac{2}{7}} = P_f T_f^{\frac{2}{7}}
\]
where \( P_f \) is the final pressure and \( T_f \) is the final temperature.
Since the tyre bursts, the final pressure \( P_f \) will be equal to the atmospheric pressure \( P_a \):
\[
P_f = P_a
\]
Step 3: Substitute the known values into the adiabatic equation.
Substitute \( P_i \), \( T_i \), and \( P_f \) into the equation:
\[
4P_a \cdot 300^{\frac{2}{7}} = P_a \cdot T_f^{\frac{2}{7}}
\]
Step 4: Solve for the final temperature \( T_f \).
Divide both sides by \( P_a \):
\[
4 \cdot 300^{\frac{2}{7}} = T_f^{\frac{2}{7}}
\]
Raise both sides to the power of \( \frac{7}{2} \) to solve for \( T_f \):
\[
T_f = \left( 4 \cdot 300^{\frac{2}{7}} \right)^{\frac{7}{2}}
\]
Step 5: Simplify the expression.
Using the property of exponents, we can simplify the expression:
\[
T_f = 300 \cdot (4)^{\frac{7}{2} - 1}
\]
\[
T_f = 300 \cdot 4^{\frac{5}{2}} \cdot 4^{-27}
\]
\[
T_f = 300 \cdot (4)^{-27}
\]
Thus, the final temperature is:
\[
T_f = 300 \cdot (4)^{-27}
\]