Block dropped onto a spring down an incline

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Homework Help Overview

The discussion revolves around a block of mass released from rest on a frictionless incline, which compresses a spring upon reaching it. The problem involves concepts from energy conservation and dynamics, specifically focusing on the calculations related to the distance moved down the incline and the speed of the block as it contacts the spring.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of conservation of energy to find the distance moved and the speed of the block. There are attempts to clarify the spring constant's units and its implications on calculations. Questions arise regarding the sign convention used in height calculations.

Discussion Status

Some participants have provided guidance on the calculations and the interpretation of energy conservation principles. There is acknowledgment of differing definitions for potential energy reference points, but no explicit consensus has been reached regarding the sign convention for height.

Contextual Notes

Participants are navigating through the implications of unit conversions and the definitions of potential energy in their calculations. The original poster expresses uncertainty about the correctness of their approach, particularly concerning the sign used in height calculations.

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A block of mass m = 12 kg is released from rest on a frictionless incline of angle theta = 30 degrees. Below the block is a spring that can be compressed 2.0 cm by a force of 270 N. The block momentarily stops when it compresses the spring by 5.5 cm.

a) How far does the block move down the incline from its rest position to this stopping point?
b) What is the speed of the block just as it touches the spring?


Okay, so I got the answer to part a like this:
k = F/x = 270/2.0 = 135 N/m​
h = ((1/2)kx^2)/(mg) = 17.4 cm (used law of conservation of energy for this one)​
(L + x) = h/sin(30) = 35 cm​

But I'm having some trouble with part b :frown:.

Anyone think they can help me out a bit with part b?
 
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The units for your k are not N/m, so be careful what you do next. You have everything you need to find L and L is proportional to the change in height of the mass from the initial point to where it touches the spring. Use conservation of energy again to find the KE and the velocity.
 
Oh..yeeeah, meant to type N/cm sorry lol.

K, so I found L
L = (h/sin(30)) - x = 0.29 m​
(switched to meters b/c the answer in the book switched to meters, though I don't know why)​


and then used that to find the new h
h = Lsin(30) = 0.29sin(30) = 0.15 m​


which I then plugged into mgh = (1/2)mv^2 to find the velocity
v^2 = 2gh = 2(9.8)(0.15) = 2.94​
v = 1.7 m/s​


and I found the mgh = 1/2mv^2 by using the following
KE initial + PE initial = KE final + PE final​
0 + mgh = ((1/2)mv^2) + 0​


I know the answer is right, but did I find it the right way?
B/c someone was telling me that the h should = -Lsin(30) rather than +Lsin(30)...
 
The way you defined things, the + sign is correct. Someone else might have defined the zero of potental energy at the top and used negatives from there. Your approach and calculation are fine.
 
Ah, okay :smile:.


Thanks for the help ^_^.
 

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