The kinetic energy of an object is given by:
\[
E_k = \frac{1}{2} m v^2,
\]
where \( m \) is the mass and \( v \) is the velocity.
**Energy spent to accelerate from rest to \( u \):**
\[
E_1 = \frac{1}{2} m u^2.
\]
**Energy spent to accelerate from \( u \) to \( 2u \):**
The kinetic energy at \( 2u \) is:
\[
E_2 = \frac{1}{2} m (2u)^2 = \frac{1}{2} m (4u^2) = 2m u^2.
\]
The kinetic energy at \( u \) is:
\[
E_1 = \frac{1}{2} m u^2.
\]
The energy required to go from \( u \) to \( 2u \) is:
\[
\Delta E = E_2 - E_1 = 2m u^2 - \frac{1}{2} m u^2.
\]
Simplify:
\[
\Delta E = \frac{4}{2} m u^2 - \frac{1}{2} m u^2 = \frac{3}{2} m u^2.
\]
We know that \( E_1 = \frac{1}{2} m u^2 \), so:
\[
\Delta E = 3E_1.
\]
Thus, \( n = 3 \), and the energy required to accelerate the car from \( u \, \text{m/s} \) to \( 2u \, \text{m/s} \) is \( \boxed{3E} \).