What should be the force constant of the spring?

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SUMMARY

The discussion focuses on determining the force constant of a spring designed to stop a 1100 kg car moving at 0.66 m/s, compressing the spring by 0.09 m. The correct calculation involves equating the kinetic energy of the car to the potential energy stored in the spring, leading to a force constant (k) of 59155.5 N/m. Alternative methods using kinematics were deemed inappropriate due to the non-constant acceleration of the car as the spring compresses. The integration of Hooke's Law is suggested as a valid approach to derive the energy relationship.

PREREQUISITES
  • Understanding of kinetic energy (KE) and potential energy (PE) concepts
  • Familiarity with Hooke's Law and spring mechanics
  • Knowledge of basic kinematics and equations of motion
  • Ability to perform integration in the context of physics
NEXT STEPS
  • Study the derivation of the work-energy theorem in relation to variable forces
  • Learn about Hooke's Law and its application in spring systems
  • Explore integration techniques for calculating work done by variable forces
  • Investigate differential equations in the context of motion under varying forces
USEFUL FOR

Physics students, mechanical engineers, and anyone involved in designing safety mechanisms in automotive applications will benefit from this discussion.

David112234
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Homework Statement


You are asked to design spring bumpers for the walls of a parking garage. A freely rolling 1100 kg car moving at 0.66 m/s is to compress the spring no more than 9.0×10−2m before stopping.

What should be the force constant of the spring? Assume that the spring has negligible mass.
Express your answer using two significant figures.

Homework Equations


F=ma
w=F*d
w=ΛKE

The Attempt at a Solution



I Know that the KE o the car is transferred into the PE of the spring
.5mv2=.5kx2
Using this method I found the right answer = 59155.5

But this question is in a chapter before PE is mentioned so Id like to see how else it can be solved. I initially tried this method, and would like to know why it is wrong:

The car must decelerate during this displacement so using kinematics:
02=662 + 2a(.09)
-.4356=2a(.09)
a= -2.42

F=ma
F=1100*-2.42
F=-2695
so the spring must apply the same force in the opposite direction to stop the cart
29577=k(.09)
k= 29577.8 (wrong answer)
So why is this method not applicable to this problem?

Also should integration be involved here somewhere? Where?
 
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The acceleration of the car and the force of the spring won't be constant, you cannot apply formulas that assume this.
 
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David112234 said:
But this question is in a chapter before PE is mentioned so Id like to see how else it can be solved. I initially tried this method, and would like to know why it is wrong:

The car must decelerate during this displacement so using kinematics:
02=662 + 2a(.09)
-.4356=2a(.09)
a= -2.42

F=ma
F=1100*-2.42
F=-2695
so the spring must apply the same force in the opposite direction to stop the cart
29577=k(.09)
k= 29577.8 (wrong answer)
So why is this method not applicable to this problem?

Also should integration be involved here somewhere? Where?
The acceleration is not constant for this problem since the force increases as the spring compresses. The formula that you've chosen is one of the SUVAT equations which only apply when the acceleration is constant.

Two of your relevant equations involve work. Are those equations fair game for solving the problem?
 
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gneill said:
The acceleration is not constant for this problem since the force increases as the spring compresses. The formula that you've chosen is one of the SUVAT equations which only apply when the acceleration is constant.

Two of your relevant equations involve work. Are those equations fair game for solving the problem?
Well, the formula for work, KE_f - KE_i was derived by plugging one of the SUVAT equations into W=m*a*d
But, that equation can also be found by integration, so does Change in KE hold even when acceleration is not constant?

So how would I solve this problem not using spring PE and using integration?
 
David112234 said:

Homework Statement


You are asked to design spring bumpers for the walls of a parking garage. A freely rolling 1100 kg car moving at 0.66 m/s is to compress the spring no more than 9.0×10−2m before stopping.

What should be the force constant of the spring? Assume that the spring has negligible mass.
Express your answer using two significant figures.

Homework Equations


F=ma
w=F*d
w=ΛKE

The Attempt at a Solution



I Know that the KE o the car is transferred into the PE of the spring
.5mv2=.5kx2
Using this method I found the right answer = 59155.5

But this question is in a chapter before PE is mentioned so Id like to see how else it can be solved. I initially tried this method, and would like to know why it is wrong:

The car must decelerate during this displacement so using kinematics:
02=662 + 2a(.09)
-.4356=2a(.09)
a= -2.42

F=ma
F=1100*-2.42
F=-2695
so the spring must apply the same force in the opposite direction to stop the cart
29577=k(.09)
k= 29577.8 (wrong answer)
So why is this method not applicable to this problem?

Also should integration be involved here somewhere? Where?
you have taken average deceleration 'a' throughout the motion but the the spring force builds up during its compression -its proportional to change in length- so 'a' will vary.
 
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David112234 said:
Well, the formula for work, KE_f - KE_i was derived by plugging one of the SUVAT equations into W=m*a*d
But, that equation can also be found by integration, so does Change in KE hold even when acceleration is not constant?
Yes, but you need to use a method that takes the changing acceleration into account, or bypasses it altogether (such as using conservation of energy and the change in PE).
So how would I solve this problem not using spring PE and using integration?
You know the expression for the force for a given distance of compression of the spring (Hooke's Law). Look at integrating F*d to find the work done; it's one of your relevant equations.
 
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gneill said:
Yes, but you need to use a method that takes the changing acceleration into account, or bypasses it altogether (such as using conservation of energy and the change in PE).

You know the expression for the force for a given distance of compression of the spring (Hooke's Law). Look at integrating F*d to find the work done; it's one of your relevant equations.

integrating hooks law i get :
∫kx
.5kx2

what can I do with this?
 
David112234 said:
integrating hooks law i get :
∫kx
.5kx2

what can I do with this?
Does it remind you of an energy formula that you used for your first attempt? :wink:
 
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gneill said:
Does it remind you of an energy formula that you used for your first attempt? :wink:

Hm, the potential energy of the spring. This represents the work since the integration is of Force over dl, so I set that to equal the negative work the car does on the spring and I end up with .5mv2=.5kx2 again. So it seems this is the only way to solve it?
 
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David112234 said:
Hm, the potential energy of the spring. This represents the work since the integration is of Force over dl, so I set that to equal the negative work the car does on the spring and I end up with .5mv2=.5kx2 again. So it seems this is the only way to solve it?
You may be able to write a differential equation for the motion and solve it. But that would probably be more effort than is warranted.
 
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  • #11
gneill said:
You may be able to write a differential equation for the motion and solve it. But that would probably be more effort than is warranted.
I prefer work energy theorem over differential equations. Can I ask for assistance in one more question very closely related to this in this thread?
 
  • #12
David112234 said:
I prefer work energy theorem over differential equations. Can I ask for assistance in one more question very closely related to this in this thread?
You can ask. Once I see your question I'll tell you if it needs a separate thread.

Edit: After seeing the new material I decided that a new thread was in order.
 
Last edited:

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