Fantastic Physics Explains a Heroic Deed in Argentina
By: Rachel Valdivieso
Topic: Forces and Work
In February 2010, BBC news reported that an Argentine man
saved a van, which was parked in the middle of the train tracks, from being
crushed by an oncoming train. The man was able to quickly jump off his friend’s
motorcycle and push the van from the tracks and avoid the oncoming train within
seconds. This is an example of fantastic
physics, because he must have applied a very large magnitude of force to push
the van from the train tracks.
In appreciation of his courageous deed, his applied force on
the van will be calculated:
Assuming the net-work
done on the 2250 kg van is 9.58 107 J and its displacement is 178.87 ft. and the coefficient of kinetic friction (μk)
is 0.4, the force the man applied can be calculated. (Assume g=9.8m/s2 )
The first step in solving this problem is to convert the
units: 178.87 ft. must be converted to meters. Given the unit conversion 1ft.=0.3408m:
178.87ft. ×.3408m/ft.=60.96m=the van’s displacement
(d)
All the forces acting on the van must be considered: FG, FN, FApp,
and FFr
FG, the force due to gravity,
does not account for any work being done on the van, because it acts downwards
in the y-direction, which is perpendicular to the van’s displacement in the
x-direction.
FG×d×Cos(θ)=(2250kg)(9.8m/s2)(60.96m)[cos(90°)]=OJ=WG,
since cos(90°)=0.
FN, the normal force that the ground
exerts upwards on the van, also does not account for any work being done on the
van, because it acts upwards in the y-direction, perpendicular to the van’s displacement
in the x-direction. Since the normal force is perpendicular to the van’s
displacement, θ=90°, so multiplying cos(90°) by the FN
and d gives 0J of work done by the normal force.
FApp, the force applied by the
man on the van, does account for a portion of the net-work being done on the
van, because it acts parallel to the van’s displacement in the x-direction.
FApp×d×cos(0°)=WApp
FFr, the force of friction due
to the van’s contact with the ground, also accounts for a portion of the
net-work being done on the van, because it acts parallel to the van’s
displacement in the x-direction.
FFr×d×cos(180°)=WFr
Summing up the Forces in the y-direction
and setting them equal to zero, since the van does not accelerate in the
y-direction, ay=0.
ΣFy=may=0=FN-FG,
so FN=FG
WNet=WApp+WFr
WFr=[cos(180°)]×(FFr)×(d),
since FFr=FNμ
and FN=FG=mg, so FFr=μmg;
WFr=[cos(180°)]×μ × m ×
g × d
WFr=
(-1)×(0.4)×(2250kg)×(9.8m/s2)×(60.96m)≈-5.3767×105J
WApp=FApp×d×cos(0°)=FApp×60.96m×1=60.96FApp
Summing up FApp and FFr:
9.58×107J=60.96FApp-5.3767×105J
Solve for FApp:
FApp=1.58×106N
The answer should be given to one significant
figure:
FApp≈2×106N
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