Oriako said:
My teacher said that the deceleration of the car does not matter during the 0.25s. The force would just be whatever his initial velocity was (4.25m/s) and his final velocity (relative to the interior of the car) is surely 0 since his initial velocity of 4.25m/s is relative to the interior of the car.
Therefore:
F x t = m (Vf - Vi)
F x t = (73kg)(0 - 4.25m/s)
F = (73kg)(-4.25m/s) / (0.25s)
F = 1241N
...Can someone please disprove me? And just do out the work for the whole question and explain why.
Well, I humbly beg to differ, but would welcome being corrected. To me that's a bit like saying the swing of the bat doesn't affect the force that the baseball experiences, it's all in the pitch. The car frame of reference is not an inertial one while the crash is ongoing. A pseudo-force representing the acceleration would have to be invoked in order to make calculations in that frame of reference work.
First contact of student and dashboard occurs at time t1 = 0.306s into the crash.
At that time the student is traveling at v1 = 100 kph (forward).
0.25 seconds later (t2 = t1 + 0.25s) the student has matched velocities with the car. The car's speed at that time is (given the previously calculated value for the car's acceleration, a, over the 2s crash),
v2 = 100 kph - a*t2 = 72.20 kph (forward)
The student's change of velocity with respect to an inertial frame of reference (in this case either the ground or his/her initial uniform 100 kph state) is ∆v = (v2 - v1) = -7.721 m/s, or -27.80 kph for those who like consistent units used throughout.
That is the change in velocity that the student undergoes as viewed from any inertial reference frame (in Classical Newtonian mechanics). The force that this change in velocity represents is:
f = M*∆v/dt = 2250N
where dt is the 0.25 second interval and M is the 73kg mass of the student.