Emergency elevator safety feature calculations

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SUMMARY

The forum discussion centers on the calculations for emergency elevator safety features, specifically addressing the application of the work-energy theorem and constant acceleration equations. Participants emphasize the importance of including mass in the force equation, F_y = mv_y(dv_y/dy), and suggest using SUVAT equations for simplification. The conversation highlights the equivalence of energy and force approaches in solving these types of problems, reinforcing the need for clarity in applying fundamental physics principles.

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  • Understanding of Newton's laws of motion
  • Familiarity with SUVAT equations for constant acceleration
  • Knowledge of the work-energy theorem
  • Basic grasp of calculus as it applies to physics
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  • Study the derivation and application of the work-energy theorem in mechanical systems
  • Learn how to apply SUVAT equations to various motion scenarios
  • Explore the implications of mass in force calculations in physics
  • Investigate real-world applications of elevator safety features and their design calculations
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Physics students, engineers involved in elevator design, and safety analysts focused on mechanical systems and their safety features.

Achintya
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Homework Statement
The cable of a 4,000 kg elevator snaps when the elevator is at rest on the first floor so that the bottom is a distance d = 12.0 m. A safety device claps the guide rails so that a constant frictional force of 10,000 opposes the motion of the elevator.(g=10 m/s^2)

a) What is the speed of the elevator just before it hits the ground?
Relevant Equations
PLEASE DON'T SOLVE THIS USING CONSERVATION OF ENERGY METHOD...IF POSSIBLE SOLVE THIS USING THE FORCE VELOCITY RELATION(F=vdv/dx)
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Did you forget the mass in ##F_y = mv_y\frac{dv_y}{dy}##?

It seems you're slightly overcomplicating it too. It's a constant acceleration question, so you can do it in one line of SUVAT!

Also, you say not to solve it using 'energy' methods, but the relation you've derived from considering forces is (save for that missing factor of ##m##) a statement of the work energy theorem. Hopefully you can see that energy approaches and forces approaches are often completely equivalent!
 
etotheipi said:
Did you forget the mass in ##F_y = mv_y\frac{dv_y}{dy}##?

It seems you're slightly overcomplicating it too. It's a constant acceleration question, so you can do it in one line of SUVAT!

Also, you say not to solve it using 'energy' methods, but the relation you've derived from considering forces is (save for that missing factor of ##m##) a statement of the work energy theorem. Hopefully you can see that energy approaches and forces approaches are often equivalent!
thank a lot sir ...i just didn't realize that thing... i know it was silly.
 
etotheipi said:
It seems you're slightly overcomplicating it too. It's a constant acceleration question, so you can do it in one line of SUVAT!
There's an instruction to use F=vdv/dx (which, as you say, should be mvdv/dx).
 
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