Car-Truck Collision: Finding Initial Car Velocity

by Dimemap Team 50 views

Alright, physics enthusiasts! Let's dive into a fascinating collision scenario. We've got a car and a truck meeting in an unfortunate event, and our mission is to figure out the car's initial speed. This problem combines concepts of momentum, energy, and friction, making it a real brain-teaser. So, let's break it down step by step and see how we can unravel this physics puzzle.

Understanding the Problem Setup

First, let's get crystal clear on what we know. We're dealing with a car and a truck. The mass of the car (McarM_{car}) is 1075 kg, and the mass of the truck (MtruckM_{truck}) is a hefty 15 tons, which translates to approximately 15,000 kg. That's quite a difference in size! The truck is initially moving at a speed (V0truckV_{0 truck}) of 20 m/s. After the collision, both vehicles stick together and move as one unit, reaching a final velocity (Vcarβ€²V'_{car} = Vtruckβ€²V'_{truck} = VcombinedV_{combined}) of 10 m/s. The combined wreckage skids to a stop over a distance (s) of 30 meters, and we know the coefficient of friction (ΞΌ\mu) between the tires and the road is 0.5. Our ultimate goal? To determine the initial velocity of the car (V0carV_{0 car}). So, with all these details in mind, let's get started with applying conservation laws.

Applying the Conservation of Momentum

The principle of conservation of momentum is our first key tool. In a closed system, the total momentum before a collision is equal to the total momentum after the collision. Mathematically, this looks like:

Mcarβˆ—V0car+Mtruckβˆ—V0truck=(Mcar+Mtruck)βˆ—VcombinedM_{car} * V_{0 car} + M_{truck} * V_{0 truck} = (M_{car} + M_{truck}) * V_{combined}

We know McarM_{car}, MtruckM_{truck}, V0truckV_{0 truck}, and VcombinedV_{combined}. What we're after is V0carV_{0 car}. Plugging in the values, we get:

1075kgβˆ—V0car+15000kgβˆ—20m/s=(1075kg+15000kg)βˆ—10m/s1075 kg * V_{0 car} + 15000 kg * 20 m/s = (1075 kg + 15000 kg) * 10 m/s

This equation is our first major step. Let's simplify it:

1075βˆ—V0car+300000=16075βˆ—101075 * V_{0 car} + 300000 = 16075 * 10

1075βˆ—V0car+300000=1607501075 * V_{0 car} + 300000 = 160750

Now, isolate the term with V0carV_{0 car}:

1075βˆ—V0car=160750βˆ’3000001075 * V_{0 car} = 160750 - 300000

1075βˆ—V0car=βˆ’1392501075 * V_{0 car} = -139250

Finally, solve for V0carV_{0 car}:

V0car=βˆ’139250/1075V_{0 car} = -139250 / 1075

V0carβ‰ˆβˆ’129.53m/sV_{0 car} β‰ˆ -129.53 m/s

Wow, that's a fast car! The negative sign tells us that the car was moving in the opposite direction to the truck, which makes sense in a collision scenario. But before we declare victory, let's consider the next part of the problem: the stopping distance.

Incorporating Work and Energy with Friction

Now, let's bring in the concept of work and energy. After the collision, the combined mass of the car and truck skids to a halt due to friction. The work done by friction is equal to the change in kinetic energy of the combined mass. The work done by friction can be expressed as:

Wfriction=βˆ’fβˆ—sW_{friction} = -f * s

where ff is the friction force and ss is the stopping distance. The negative sign indicates that friction acts in the opposite direction to motion, doing negative work and reducing the kinetic energy. Friction force (ff) is given by:

f=ΞΌβˆ—Nf = \mu * N

where ΞΌ\mu is the coefficient of friction and NN is the normal force. On a flat surface, the normal force is equal to the gravitational force, so:

N=(Mcar+Mtruck)βˆ—gN = (M_{car} + M_{truck}) * g

where gg is the acceleration due to gravity (approximately 9.8 m/sΒ²). Plugging in the values:

N=(1075kg+15000kg)βˆ—9.8m/s2N = (1075 kg + 15000 kg) * 9.8 m/sΒ²

N=16075kgβˆ—9.8m/s2N = 16075 kg * 9.8 m/sΒ²

Nβ‰ˆ157535NN β‰ˆ 157535 N

Now we can calculate the friction force:

f=0.5βˆ—157535Nf = 0.5 * 157535 N

fβ‰ˆ78767.5Nf β‰ˆ 78767.5 N

And the work done by friction:

Wfriction=βˆ’78767.5Nβˆ—30mW_{friction} = -78767.5 N * 30 m

Wfrictionβ‰ˆβˆ’2363025JW_{friction} β‰ˆ -2363025 J

This work done by friction is equal to the change in kinetic energy. The change in kinetic energy (Ξ”KE\Delta KE) is:

Ξ”KE=KEfinalβˆ’KEinitial\Delta KE = KE_{final} - KE_{initial}

Since the final velocity is 0, KEfinalKE_{final} is 0. The initial kinetic energy (KEinitialKE_{initial}) is:

KEinitial=0.5βˆ—(Mcar+Mtruck)βˆ—Vcombined2KE_{initial} = 0.5 * (M_{car} + M_{truck}) * V_{combined}Β²

KEinitial=0.5βˆ—16075kgβˆ—(10m/s)2KE_{initial} = 0.5 * 16075 kg * (10 m/s)Β²

KEinitial=0.5βˆ—16075kgβˆ—100m2/s2KE_{initial} = 0.5 * 16075 kg * 100 mΒ²/sΒ²

KEinitial=803750JKE_{initial} = 803750 J

Therefore:

Ξ”KE=0βˆ’803750J\Delta KE = 0 - 803750 J

Ξ”KE=βˆ’803750J\Delta KE = -803750 J

Now, equate the work done by friction to the change in kinetic energy:

βˆ’2363025J=βˆ’803750J-2363025 J = -803750 J

Wait a minute! These values don't match. This discrepancy suggests there might be a different way to approach the problem or an error in the initial assumptions. The work-energy principle seems to contradict our momentum calculation. Let's rethink our approach.

Re-Evaluating the Problem

The mismatch between the results from the conservation of momentum and the work-energy principle suggests we need to revisit our assumptions or look for a different approach. The initial calculation using momentum conservation gave us a car velocity of approximately -129.53 m/s, which seems quite high. The work-energy principle, while logically sound, didn't align with this result. Perhaps there's a detail we've overlooked or a simplification we've made that's causing this discrepancy.

Considering an Inelastic Collision

We've treated the collision as perfectly inelastic (the vehicles stick together), which is correct. However, we might need to consider the energy lost during the collision itself. In a real-world collision, some kinetic energy is converted into other forms of energy, such as heat, sound, and deformation of the vehicles. This means the kinetic energy immediately after the collision might be less than what we calculated solely based on momentum conservation.

A Step-by-Step Breakdown Revisited

Let's backtrack and reassess our steps:

  1. Momentum Conservation: We correctly applied the conservation of momentum to find the combined velocity after the collision. The formula is:

    Mcarβˆ—V0car+Mtruckβˆ—V0truck=(Mcar+Mtruck)βˆ—VcombinedM_{car} * V_{0 car} + M_{truck} * V_{0 truck} = (M_{car} + M_{truck}) * V_{combined}

    We used this to solve for V0carV_{0 car}, and that's where we got the potentially high value.

  2. Work-Energy Theorem: We then used the work-energy theorem to relate the friction force and stopping distance to the change in kinetic energy. This is also a valid approach. However, the mismatch in values indicates an issue.

Potential Sources of Error or Misinterpretation

Before we proceed, let's pinpoint potential sources of error:

  • High Initial Velocity: The car's initial velocity of -129.53 m/s seems unusually high. This could indicate an error in our calculations or an issue with the given data.
  • Energy Loss During Collision: We assumed all the kinetic energy after the collision was dissipated by friction. However, some energy might have been lost during the collision itself.
  • Coefficient of Friction: The coefficient of friction (ΞΌ\mu = 0.5) seems reasonable, but it's a simplification. The actual friction force could vary depending on factors like tire condition and road surface.

Adjusting Our Approach: Iterative Method

Given the uncertainties, let's try a slightly different approach. Instead of directly solving for V0carV_{0 car} using momentum conservation alone, let's combine the momentum conservation equation with the work-energy theorem in an iterative manner.

The Iterative Process

  1. Assume an Initial V0carV_{0 car}: Let's start by assuming a more reasonable value for V0carV_{0 car}. For instance, let's assume V0carV_{0 car} is -30 m/s (approximately -67 mph), which is still quite fast but more plausible than -129.53 m/s.

  2. Calculate VcombinedV_{combined}: Using the momentum conservation equation, calculate the combined velocity (VcombinedV_{combined}) based on this assumed V0carV_{0 car}:

    1075kgβˆ—(βˆ’30m/s)+15000kgβˆ—20m/s=(1075kg+15000kg)βˆ—Vcombined1075 kg * (-30 m/s) + 15000 kg * 20 m/s = (1075 kg + 15000 kg) * V_{combined}

    βˆ’32250+300000=16075βˆ—Vcombined-32250 + 300000 = 16075 * V_{combined}

    267750=16075βˆ—Vcombined267750 = 16075 * V_{combined}

    Vcombinedβ‰ˆ16.66m/sV_{combined} β‰ˆ 16.66 m/s

  3. Calculate Kinetic Energy After Collision: Calculate the kinetic energy (KEcombinedKE_{combined}) of the combined mass immediately after the collision:

    KEcombined=0.5βˆ—(Mcar+Mtruck)βˆ—Vcombined2KE_{combined} = 0.5 * (M_{car} + M_{truck}) * V_{combined}Β²

    KEcombined=0.5βˆ—16075kgβˆ—(16.66m/s)2KE_{combined} = 0.5 * 16075 kg * (16.66 m/s)Β²

    KEcombinedβ‰ˆ2231531JKE_{combined} β‰ˆ 2231531 J

  4. Calculate Work Done by Friction: Calculate the work done by friction (WfrictionW_{friction}) over the stopping distance of 30 m:

    Wfriction=βˆ’fβˆ—s=βˆ’ΞΌβˆ—Nβˆ—s=βˆ’ΞΌβˆ—(Mcar+Mtruck)βˆ—gβˆ—sW_{friction} = -f * s = -\mu * N * s = -\mu * (M_{car} + M_{truck}) * g * s

    Wfriction=βˆ’0.5βˆ—16075kgβˆ—9.8m/s2βˆ—30mW_{friction} = -0.5 * 16075 kg * 9.8 m/sΒ² * 30 m

    Wfrictionβ‰ˆβˆ’2363025JW_{friction} β‰ˆ -2363025 J

  5. Compare Kinetic Energy and Work: Compare the kinetic energy immediately after the collision (KEcombinedKE_{combined}) with the absolute value of the work done by friction (∣Wfriction∣|W_{friction}|). If these values are close, our assumed V0carV_{0 car} is likely a good approximation. If not, adjust the assumed V0carV_{0 car} and repeat steps 2-5.

    In this case, KEcombinedKE_{combined} (2231531 J) and ∣Wfriction∣|W_{friction}| (2363025 J) are relatively close. This suggests that our assumed V0carV_{0 car} of -30 m/s is a reasonable starting point. We could iterate further by adjusting V0carV_{0 car} slightly to see if we can get the values even closer, but for the sake of this explanation, let's consider -30 m/s a reasonable estimate.

Discussion and Conclusion

This collision problem beautifully illustrates the interplay between fundamental physics principles like conservation of momentum and the work-energy theorem. We started with a straightforward application of these concepts but encountered a discrepancy, highlighting the complexities of real-world scenarios. By carefully re-evaluating our assumptions and employing an iterative approach, we arrived at a more plausible solution for the car's initial velocity.

The initial calculation, assuming direct momentum transfer, yielded a very high speed for the car, which raised a red flag. Incorporating the work-energy theorem and friction helped us refine our estimate. The iterative method allowed us to converge on a solution that balanced the momentum change during the collision with the energy dissipated by friction during the skidding process.

It's important to recognize the limitations of our model. We've made simplifying assumptions, such as a constant coefficient of friction and a perfectly inelastic collision. In reality, factors like energy loss due to vehicle deformation and variations in road conditions could influence the outcome. However, our analysis provides a solid framework for understanding the dynamics of car-truck collisions and the importance of considering multiple physical principles in problem-solving.

So, what did we learn today, guys? Physics problems often require more than just plugging numbers into formulas. Critical thinking, careful consideration of assumptions, and a willingness to iterate are crucial for success. Keep questioning, keep exploring, and keep those physics gears turning!