Step 1: Understanding the relationship between electric field and velocity.
The velocity \( v(t) \) of a charged particle in an electric field can be derived from the electric field \( E(t) \) by integrating it over time. The relationship is given by:
\[
v(t) = \frac{q}{m} \int E(t) \, dt
\]
where \( q \) is the charge of the particle, \( m \) is the mass, and \( E(t) \) is the electric field as a function of time.
Step 2: Substituting the given electric field.
We are given \( E(t) = 108t - 22 \), so we substitute this into the equation:
\[
v(t) = \frac{q}{m} \int (108t - 22) \, dt
\]
Step 3: Performing the integration.
Integrating \( 108t - 22 \) with respect to time:
\[
\int (108t - 22) \, dt = \frac{108t^2}{2} - 22t + C
\]
Step 4: Final expression for velocity.
Thus, the velocity as a function of time is:
\[
v(t) = \frac{q}{m} \left( \frac{108t^2}{2} - 22t + C \right)
\]
Step 5: Conclusion.
This is the expression for the velocity of the particle derived from the electric field.