Mechanics - Work-Energy Principle Question

AI Thread Summary
The discussion focuses on a physics problem involving the work-energy principle applied to a car's motion under different conditions. Part a) confirms the time taken for the car to accelerate from 12 m/s to 20 m/s without resistance is approximately 5.376 seconds. In part b), participants analyze the impact of a constant resistance force while the engine maintains a power output of 25 kW, leading to confusion about calculating the resistive force and work done against it. The conversation emphasizes that the work-energy principle can be applied even with non-conservative forces, and the net work done can be determined by comparing the energy supplied by the engine to the change in kinetic energy. Ultimately, the key takeaway is the importance of focusing on energy changes rather than assumptions about forces or acceleration.
AntSC
Messages
65
Reaction score
3

Homework Statement



a) A car of mass 1050kg moves along a straight horizontal road with its engine working at a constant rate of 25kW. Its speed at a point A on the road is 12ms-1. Assuming that there is no resistance to motion, calculate the time taken for the car to travel from A until it reaches a speed of 20ms-1.

b) Assume now that there is a constant resistance to motion and that the car's engine continues to work at 25kW. It takes 10.7s for the car's speed to increase from 12ms-1 to 20ms-1. During this time the car travels 179m. Calculate the work done against resistance and hence find the magnitude of the resistance.

c) Later the car moves up a straight hill, inclined at 2° to the horizontal. The engine works at 25kW as before, and there is a constant resistance of the same magnitude as before. The car travels a distance of 393m while its speed increases from 12ms-1 to 20ms-1. Calculate the time taken by the car to travel this distance.


Homework Equations



I'm lost at part b). I don't know what i am missing with my understanding.

The Attempt at a Solution



a)
Given that gravitational force is conservative, the work-energy principle can be used.
P=\frac{E}{t}=\frac{m\left ( v^{2}-u^{2} \right )}{2t}
t=\frac{m\left ( v^{2}-u^{2} \right )}{2P}
t=\frac{1050\left ( 20^{2}-12^{2} \right )}{2\times 25000}
t=5.376s
This answer is confirmed correct

b)
P=Fv so F=\frac{P}{v}. F=ma so with a resistive force
\frac{P}{v}-R=ma
Given that work done W=Fd and the net force in the system is now \frac{P}{v}-R then
W=\left ( \frac{P}{v}-R \right )d
So we need the magnitude of R before we can find work done. To find R we need to know the acceleration.
a=\frac{v-u}{t}
a=\frac{20-12}{10.7}
a=0.748ms^{-2}
Now can find R
R=\frac{P}{v}-ma
R=\frac{25000}{12}-1050\left ( 0.748 \right )
R=1297.9N
This is incorrect. Don't know what I'm missing here. Any help would be great. Cheers
 
Physics news on Phys.org
AntSC said:

Homework Statement



a) A car of mass 1050kg moves along a straight horizontal road with its engine working at a constant rate of 25kW. Its speed at a point A on the road is 12ms-1. Assuming that there is no resistance to motion, calculate the time taken for the car to travel from A until it reaches a speed of 20ms-1.

b) Assume now that there is a constant resistance to motion and that the car's engine continues to work at 25kW. It takes 10.7s for the car's speed to increase from 12ms-1 to 20ms-1. During this time the car travels 179m. Calculate the work done against resistance and hence find the magnitude of the resistance.

c) Later the car moves up a straight hill, inclined at 2° to the horizontal. The engine works at 25kW as before, and there is a constant resistance of the same magnitude as before. The car travels a distance of 393m while its speed increases from 12ms-1 to 20ms-1. Calculate the time taken by the car to travel this distance.


Homework Equations



I'm lost at part b). I don't know what i am missing with my understanding.

The Attempt at a Solution



a)
Given that gravitational force is conservative, the work-energy principle can be used.
P=\frac{E}{t}=\frac{m\left ( v^{2}-u^{2} \right )}{2t}
t=\frac{m\left ( v^{2}-u^{2} \right )}{2P}
t=\frac{1050\left ( 20^{2}-12^{2} \right )}{2\times 25000}
t=5.376s
This answer is confirmed correct

b)
P=Fv so F=\frac{P}{v}. F=ma so with a resistive force
\frac{P}{v}-R=ma
Given that work done W=Fd and the net force in the system is now \frac{P}{v}-R then
W=\left ( \frac{P}{v}-R \right )d
So we need the magnitude of R before we can find work done. To find R we need to know the acceleration.
a=\frac{v-u}{t}
a=\frac{20-12}{10.7}
a=0.748ms^{-2}
Now can find R
R=\frac{P}{v}-ma
R=\frac{25000}{12}-1050\left ( 0.748 \right )
R=1297.9N
This is incorrect. Don't know what I'm missing here. Any help would be great. Cheers
There is no need to assume that acceleration is constant .
 
SammyS said:
There is no need to assume that acceleration is constant .

How else can i find R without knowing the acceleration? And wouldn't the acceleration be constant given that the resistive force is constant?
 
AntSC said:
How else can i find R without knowing the acceleration? And wouldn't the acceleration be constant given that the resistive force is constant?
It may be constant, but you're making a assumption about that.

The resistive force is constant, but is the NET force constant?


How much work is done by the resistive force?


What is the net work done on the car?
 
SammyS said:
The resistive force is constant, but is the NET force constant?

If the engine continues to work at a constant rate then won't the force generated by the engine also be constant? Therefore the net force is constant.

SammyS said:
How much work is done by the resistive force?

I don't see how i can find the work done by the resistive force because i can't use the work-energy principle as frictional forces are not conservative.
 
AntSC said:
If the engine continues to work at a constant rate then won't the force generated by the engine also be constant? Therefore the net force is constant.



I don't see how i can find the work done by the resistive force because i can't use the work-energy principle as frictional forces are not conservative.
You can determine the Net work done on he system.

Then, you can set up an equation with the resistive force being the only unknown.
 
How do i find the net work done if i don't know the net force? I can't used work-energy principle as friction is not conservative.
If i just use F=\frac{P}{v} then aren't i assuming v is constant? Clearly it's not as it's increasing over the distance.
Definitely not getting this :(
 
Hey Ant, I think you are going about this with a bit of calculus pretty easily. Considering you have a constant resisting force and your engine is providing a constant power, I think it is safe to say that you WILL have a constant acceleration. So, remember that the derivative of your work and energy equation with respect to time will give you your power equation.

So, if you set it up,

1/2mv^2 + ∑W = 1/2mv^2

So, the two forces doing work on your object are the force coming from the engine which is working WITH the direction of motion, and the resisting force which is working against it (that means watch your signs). Both of those are unknowns, and after you set that up, take the time derivative of the entire equation and you will be able to work with values that you already know. Remember the chain rule when you take the derivative of the kinetic energy, so that your acceleration pops up.

After that, I would consider working backwards from that point keeping in mind that:

P = W/t (when the power is constant, which is looks like it is)

and

W = F*d

I hope that helped!
 
AntSC said:
How do i find the net work done if i don't know the net force? I can't used work-energy principle as friction is not conservative.
If i just use F=\frac{P}{v} then aren't i assuming v is constant? Clearly it's not as it's increasing over the distance.
Definitely not getting this :(
The Work-Energy theorem does not require the forces to be conservative.

The engine power is constant, so it's easy to find the work it does in 10.7 seconds.

You can calculate the change in Kinetic Energy.

The difference must be equal to the work done by the resistive force, R.

You also know the distance traveled during the 10.7 seconds.
 
  • #10
I thought W-E theorum does require conservative forces. Better check that out again.

For the work done by the engine:
W_{E}=Fd=\frac{P}{v}d=\frac{25000}{12}\cdot 179=372916J
So the net work done:
W_{N}=\frac{1}{2}m\left ( v^{2}-u^{2} \right )=\frac{1050}{2}\left ( 20^{2}-12^{2} \right )=134400J
Work done by resistance:
W_{R}=W_{N}-W_{E}=372916-134400=238516J
Magnitude of resistive force:
F=\frac{W_{R}}{d}=\frac{238516}{179}=1332N
This isn't right, comparing with the answers.
 
  • #11
That first formula is incorrect. The force in not constant so you cannot calculate the work done as
W=F*d.

But you don't need to go through this. You know the power and the time. What is the definition of power?

And you don't need conservative forces to apply work-energy theorem. It works for friction forces too.
Or engine forces, as here.
The conservation of energy requires conservative forces.
 
  • #12
nasu said:
That first formula is incorrect. The force in not constant so you cannot calculate the work done as
W=F*d.

But you don't need to go through this. You know the power and the time. What is the definition of power?

And you don't need conservative forces to apply work-energy theorem. It works for friction forces too.
Or engine forces, as here.
The conservation of energy requires conservative forces.

Ok so for the energy burn from the engine we have
W_{E}=Pt=25000\times 10.7=267500J
And for the net energy burn of the system we have
W_{N}=\frac{1}{2}m\left ( v^{2}-u^{2} \right )=\frac{1050}{2}\left ( 20^{2}-12^{2} \right )=134400J
The difference is the work done by the resistive force
W_{R}=267500-134400=133100
So
F_{R}d=133100\; \Rightarrow \; F_{R}=\frac{133100}{179}=744N
 
  • #13
This looks OK.
 
  • #14
Work Energy Principle

Hi Ant.
This problem works out fine. Many people’s problem is that they think analysing acceleration because they assume F=ma is relevant. It is not relevant. WE principle is all about energies at certain times or positions (distances/heights). And that is it.
Don’t get involved in what is happening between these energy ‘points’. No assumptions should be made that the access are linear or anything else. This is all about velocity changes, distance changes (against resistive forces) and/or height changes. Energy sources balanced against energy sinks if you will. In this case gravity is not the energy source. The engine is. And it provides energy at a rate of 25000J/s. power x time = energy supplied.
Energy sinks are increase in KE, increase in GPE and work done against resistive forces over particular distances. That’s all. Forget conservative arguments, red herring.

Happy to discuss
 
Back
Top