We will use the work-energy principle to solve this problem. The work done by the resistive force \( F_{\text{res}} \) is equal to the change in kinetic energy.
The kinetic energy \( K \) is given by:
\[
K = \frac{1}{2} m v^2
\]
where \( m \) is the mass of the scooter and \( v \) is its speed.
The initial kinetic energy of the scooter before stopping is:
\[
K_i = \frac{1}{2} m v^2
\]
The final kinetic energy \( K_f \) is zero because the scooter is stopped.
The work done by the resistive force is given by:
\[
W = F_{\text{res}} \cdot d
\]
where \( d \) is the distance over which the force acts (10 m).
By the work-energy principle:
\[
F_{\text{res}} \cdot d = \Delta K = K_i - K_f
\]
Substituting the values:
\[
F_{\text{res}} \cdot 10 = \frac{1}{2} m v^2
\]
We know the weight \( W = mg \), so \( m = \frac{W}{g} \).
Substitute this into the equation:
\[
F_{\text{res}} \cdot 10 = \frac{1}{2} \frac{W}{g} v^2
\]
Since \( v = 7 \, \text{m/s} \), substitute that in:
\[
F_{\text{res}} \cdot 10 = \frac{1}{2} \frac{W}{g} (7)^2
\]
Simplifying further:
\[
F_{\text{res}} \cdot 10 = \frac{1}{2} \frac{W}{g} \cdot 49
\]
\[
F_{\text{res}} = \frac{49W}{20g}
\]
Now, to find the total resistance to the motion, we note that the resistance \( F_{\text{res}} \) is proportional to the weight of the scooter \( W \).
Thus, the total resistance \( R \) to the motion of the scooter is:
\[
R = \frac{1}{4} W
\]