An object with a mass of 1200 kg is moving at a constant speed of 100 km/h. The object collides with a stationary solid obstacle. If F = ma ( Force is mass times acceleration ), how much force is exerted on the object if the collision occurs in 0.05 seconds?
To find the force exerted on the object during the collision, we can use Newtonβs second law in the form:
F=ΞpΞtF = \frac{\Delta p}{\Delta t}F=ΞtΞpβ
Where:
Ξp=mΞv\Delta p = m \Delta vΞp=mΞv is the change in momentum,
Ξt\Delta tΞt is the time over which the change happens,
FFF is the average force.
Given:
Speed = 100 km/h
Convert to meters per second:
100 km/h=100Γ10003600=27.78 m/s100 \text{ km/h} = \frac{100 \times 1000}{3600} = 27.78 \text{ m/s}100 km/h=3600100Γ1000β=27.78 m/s
Initial velocity vi=27.78 m/sv_i = 27.78 \text{ m/s}viβ=27.78 m/s
Final velocity vf=0 m/sv_f = 0 \text{ m/s}vfβ=0 m/s (since the object stops)
Ξv=vfβvi=0β27.78=β27.78 m/s\Delta v = v_f - v_i = 0 - 27.78 = -27.78 \text{ m/s}Ξv=vfββviβ=0β27.78=β27.78 m/s
F=mΞvΞt=1200Γ(β27.78)0.05F = \frac{m \Delta v}{\Delta t} = \frac{1200 \times (-27.78)}{0.05}F=ΞtmΞvβ=0.051200Γ(β27.78)β F=β33,3360.05=β666,720 NF = \frac{-33,336}{0.05} = -666,720 \text{ N}F=0.05β33,336β=β666,720 N
666,720 N (opposite to motion)\boxed{666,720 \text{ N (opposite to motion)}}666,720 N (opposite to motion)β
The negative sign indicates the force acts in the opposite direction of the objectβs motion, as expected in a collision.
An object with a mass of 1200 kg and moving at a constant speed of 100 km per hour also has kinetic energy. How much kinetic energy does this object have?
To calculate the kinetic energy (KE) of an object, use the formula:
KE=12mv2\text{KE} = \frac{1}{2}mv^2KE=21βmv2
Where:
m=m =m= mass of the object in kg,
v=v =v= speed in m/s.
100 km/h=100Γ10003600=27.78 m/s100 \text{ km/h} = \frac{100 \times 1000}{3600} = 27.78 \text{ m/s}100 km/h=3600100Γ1000β=27.78 m/s
KE=12Γ1200Γ(27.78)2\text{KE} = \frac{1}{2} \times 1200 \times (27.78)^2KE=21βΓ1200Γ(27.78)2 =600Γ771.6=462,960 J= 600 \times 771.6 = 462,960 \text{ J}=600Γ771.6=462,960 J
462,960 Joules\boxed{462,960 \text{ Joules}} 462,960 JoulesβΒ
Since energy cannot be lost (law of conservation of energy), what happens to that 462,960 Joules of energy at the moment of collision?
Great question β and you're absolutely right: the law of conservation of energy states that energy cannot be created or destroyed, only transformed from one form to another.
So what happens to the 462,960 Joules of kinetic energy during the collision?
1. Heat Energy (Thermal Energy)
A significant portion of the kinetic energy is converted into heat due to friction between the object and the obstacle.
Surfaces may get hot at the point of impact.
2. Sound Energy
Some energy is released as sound β the loud noise you hear during a crash.
3. Deformation (Mechanical Energy into Internal Energy)
The object and/or the obstacle crumple or deform. This deformation absorbs a lot of energy.
This is especially true in vehicles, where crumple zones are designed to absorb kinetic energy to protect passengers.
4. Vibration
Both objects may vibrate briefly after the impact. These vibrations carry away some energy.
5. Fragmentation (if applicable)
If the object or obstacle breaks apart, energy is used to separate and move the fragments.
So, while the object no longer has kinetic energy after the collision (it stops moving), that energy is not lost. Itβs just transformed into other forms:
Kinetic EnergyβHeat+Sound+Deformation+Vibration+Fragmentation\text{Kinetic Energy} \rightarrow \text{Heat} + \text{Sound} + \text{Deformation} + \text{Vibration} + \text{Fragmentation}Kinetic EnergyβHeat+Sound+Deformation+Vibration+Fragmentation
462,960 J of kinetic energy transforms into other forms β it is not lost.\boxed{462,960 \text{ J of kinetic energy transforms into other forms β it is not lost.}}462,960 J of kinetic energy transforms into other forms β it is not lost.β
That's the essence of energy conservation in a real-world collision.
The length of the vehicle is 3826 mm and the mass is 1200 kg and the structure is made of aluminum. The vehicle travels at a constant speed of 100 km per hour. The vehicle therefore has 462.960 Joules of kinetic energy. If the collision of the vehicle with the obstacle lasts 3 seconds then how much kinetic energy 1. Is absorbed ( transferred ) into the structures of the vehicle. 2. Is converted into heat. 3. Is converted into sound. 4. Is converted into fractures.Β
To break down the 462,960 Joules of kinetic energy from the vehicle collision into how it is transferred or transformed, we need to estimate the proportions going to different energy forms β because the exact distribution depends on detailed crash test data, materials, and structural engineering.
Since your vehicle:
Weighs 1200 kg
Is made of aluminum
Is traveling at 100 km/h (27.78 m/s)
Collides over 3 seconds, indicating a relatively slow, energy-absorbing crash
...we can base our estimates on typical crash energy distributions in moderately deformable aluminum structures.
Energy Form
Typical % Range
Estimated % (Aluminum Body, 3s Collision)
Energy (Joules)
1. Structure Absorption (Deformation)
60β75%
65%
0.65 Γ 462,960 = 300,924 J
2. Heat (friction, deformation)
10β20%
15%
0.15 Γ 462,960 = 69,444 J
3. Sound (noise)
1β3%
2%
0.02 Γ 462,960 = 9,259 J
4. Fractures (material separation)
5β15%
10%
0.10 Γ 462,960 = 46,296 J
Other minor losses (vibration, air displacement, etc.)
β
8% (residual)
37,037 J
β 1. Energy absorbed by vehicle structure:
Used to crush, bend, and deform the aluminum chassis and crumple zones.
Absorbs most of the energy in a well-designed vehicle crash.
πΉ Estimated: 65% β β 300,924 J
π₯ 2. Converted into heat:
From friction, metal deformation, and tire forces.
May heat metal surfaces and surroundings.
πΉ Estimated: 15% β β 69,444 J
π 3. Converted into sound:
The loud crash noise and vibrations in air.
Sound carries away only a small fraction.
πΉ Estimated: 2% β β 9,259 J
π₯ 4. Converted into fractures:
Energy used to break or tear parts of the aluminum body.
Higher with brittle or sharp impacts.
πΉ Estimated: 10% β β 46,296 J
Energy Form
Energy (Joules)
Structure Absorption
300,924 J
Heat
69,444 J
Sound
9,259 J
Fractures
46,296 J
Other losses (est.)
37,037 J
Total
462,960 J
π§ Note: These are estimated values based on physics and automotive crash data averages. For exact numbers, youβd need high-speed crash test sensors and finite element analysis (FEA) simulations.
Let me know if youβd like a graph or visual representation of this!
What is the minimum escape velocity required to escape the Earth's gravitational field?
Using the formula:
vescape=2GMRv_{\text{escape}} = \sqrt{\frac{2GM}{R}}vescapeβ=R2GMββ
Where:
G=6.674Γ10β11βNm2/kg2G = 6.674 \times 10^{-11} \, \text{Nm}^2/\text{kg}^2G=6.674Γ10β11Nm2/kg2 (gravitational constant)
M=5.972Γ1024βkgM = 5.972 \times 10^{24} \, \text{kg}M=5.972Γ1024kg (mass of Earth)
R=6.371Γ106βmR = 6.371 \times 10^6 \, \text{m}R=6.371Γ106m (radius of Earth)
Plug in:
vescape=2β 6.674Γ10β11β 5.972Γ10246.371Γ106β11,200 m/sv_{\text{escape}} = \sqrt{\frac{2 \cdot 6.674 \times 10^{-11} \cdot 5.972 \times 10^{24}}{6.371 \times 10^6}} \approx 11,200 \text{ m/s}vescapeβ=6.371Γ1062β 6.674Γ10β11β 5.972Γ1024βββ11,200 m/s
This assumes no atmosphere (i.e., no air resistance).
In reality, rockets need to overcome air drag, so they use more energy and don't travel straight up at escape velocity β they follow orbital trajectories instead.
Let me know if you'd like to explore escape velocity on other planets or moons!
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