Length along ramp from end of spring, picture included

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Homework Help Overview

The problem involves a 2300 g block pushed against a spring on a frictionless incline of 33°. The spring has a constant of 14 N/cm and is compressed by 19 cm. The task is to determine how far the block moves up the ramp after the spring is released, both with and without friction.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the role of the angle in the problem and how it affects the calculations. There are questions about the energy equations and how to properly account for potential energy and work done by non-conservative forces.

Discussion Status

Some participants have provided insights into energy conservation principles and the relationship between potential energy in the spring and gravitational potential energy. Others are exploring the calculations for height and distance along the ramp, with varying degrees of success and some confusion regarding the correct application of trigonometric functions.

Contextual Notes

Participants note the importance of converting units and the implications of friction in the second part of the problem. There is also mention of the need to adjust calculations based on the reference point chosen for potential energy.

gap0063
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Homework Statement


A(n) 2300 g block is pushed by an external
force against a spring (with a 14 N/cm spring
constant) until the spring is compressed by
19 cm from its uncompressed length. The
compressed spring and block rests at the bot-
tom of an incline of 33◦ .
The acceleration of gravity is 9.8 m/s2 .
Note: The spring lies along the surface of
the ramp (see figure).
Assume: The ramp is frictionless.
Now, the external force is rapidly removed
so that the compressed spring can push up
the mass.
[PLAIN]http://img64.imageshack.us/img64/5812/problem6l.jpg
(a)How far up the ramp (i.e., ℓ the length
along the ramp) will the block move (measured
from the end of the spring when the
spring is uncompressed) before reversing di-
rection and sliding back?
Remember, the block is not attached to the
spring.
Answer in units of cm.

(b)Repeat the first part of this question, but
now assume that the ramp has a coefficient of
friction of μ = 0.308 .
Keep all other assumptions the same.
Answer in units of cm.



Homework Equations


\DeltaK= Kf-Ki=1/2mvf2-1/2mvi2
Etotal=1/2mk2+1/2mv2

The Attempt at a Solution


I don't know where the angle comes in...
I know that N=mgcos\theta
 
Last edited by a moderator:
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gap0063 said:

Homework Statement


A(n) 2300 g block is pushed by an external
force against a spring (with a 14 N/cm spring
constant) until the spring is compressed by
19 cm from its uncompressed length. The
compressed spring and block rests at the bot-
tom of an incline of 33◦ .
The acceleration of gravity is 9.8 m/s2 .
Note: The spring lies along the surface of
the ramp (see figure).
Assume: The ramp is frictionless.
Now, the external force is rapidly removed
so that the compressed spring can push up
the mass.

(a)How far up the ramp (i.e., ℓ the length
along the ramp) will the block move (measured
from the end of the spring when the
spring is uncompressed) before reversing di-
rection and sliding back?
Remember, the block is not attached to the
spring.
Answer in units of cm.

(b)Repeat the first part of this question, but
now assume that the ramp has a coefficient of
friction of μ = 0.308 .
Keep all other assumptions the same.
Answer in units of cm.



Homework Equations


\DeltaK= Kf-Ki=1/2mvf2-1/2mvi2
Etotal=1/2mk2+1/2mv2

The Attempt at a Solution


I don't know where the angle comes in...
I know that N=mgcos\theta
Note that the block starts off with no speed, and it has no speed when it comes to a stop at the top of the incline, so delta K =0 . Note also that your energy equation is wrong. W_nc = (delta K + delta U_spring + delta U_gravity), where W_nc = work done by non conservative forces, like friction.
 
PhanthomJay said:
Note that the block starts off with no speed, and it has no speed when it comes to a stop at the top of the incline, so delta K =0 . Note also that your energy equation is wrong. W_nc = (delta K + delta U_spring + delta U_gravity), where W_nc = work done by non conservative forces, like friction.

So

Wnc= 1/2kx2+mgh

is k the 19cm (.19m)?

and do I figure out the height from the angle? and if so how?
 
Last edited:
okay k is the spring constant which is given above 14 N/cm or 1400N/m if you convert it like I did.

so you know that initial potential energy is the potential energy in the spring plus the gravitational potential energy. If you set you reference point there you can say that gravitational potential energy there is 0 because in mgh, h=0.

and we also know that when we get to the top of the slope K=0 and U=mgh
so use the information up to there to solve for the height.

if you've got the max height you can set up a triangle (sin = opp/hyp, and you know the angle and the opposite side) and solve for the distance up the ramp, but the distance you get from that is going to be the distance from the top of the "compressed" spring so compensate for that in your answer. (i.e. subtract the distance that the spring was compressed)
 
Last edited:
AHinkle said:
okay k is the spring constant which is given above 14 N/cm or 1400N/m if you convert it like I did.

so you know that initial potential energy is the potential energy in the spring plus the gravitational potential energy. If you set you reference point there you can say that gravitational potential energy there is 0 because in mgh, h=0.

and we also know that when we get to the top of the slope K=0 and U=mgh
so use the information up to there to solve for the height.

if you've got the max height you can set up a triangle (sin = opp/hyp, and you know the angle and the opposite side) and solve for the distance up the ramp, but the distance you get from that is going to be the distance from the top of the "compressed" spring so compensate for that in your answer. (i.e. subtract the distance that the spring was compressed)
would it be
1/2kx2=mgh
h=kx2/2mg

well i tried and did 1400(.19)2/(2*2.3*9.8)
h=1.12112m

then sin33=o/h
h=o/sin30
h=2.05846

2.05846-.19 m=1.8684m

which is 186.84 cm which is wrong

well I reread the problem and it says when it is uncompressed so .57 m
I misused 2.05846-.57=1.48846

which is 148.46 cm which is wrong
 
Last edited:
We have the same homework service I am pretty sure... mine was due today so here's how I did it.

Since there is no friction on the first part of the problem, mechanical energy is conserved and you can use Ui+Ki=Uf+Kf

Ui= (1/2kx2 + mghi) where hi = 0
I put the reference point a the top of the compressed spring.
x is 19cm or 0.19m the distance the spring was compressed

Ki = 1/2mvi2
but the block is at rest so v=0 so the whole quantity is 0
so Ki=0

Uf = (mgh)
(only mgh because there's no spring potential energy like there was before)

Kf = 1/2 mvf2
but again at the top of the motion the velocity is 0 so
Kf = 0

so...
Ui+Ki=Uf+Kf
(1/2kx2+0) + 0 = mghf + 0

1/2kx2 = mghf
solve for hf

(1/2kx2)/(mg)=hf
(kx2/2) x (1/mg) = hf

hf=(kx2/2mg)
convert everything to meters btw, I don't know why I do it .. i think it has to do with g being
in units of m/s2, and i converted the mass to kilos

k=1400 N/m (14 N/cm)
x=.19m (19cm)
m=2.3Kg (2300g)

hf=((1400N/m)(.19m)2)/(2(2.3Kg)(9.8m/s2))

hf=1.1211 Meters (112.1118 cm)

\theta = 33 degrees
sin(33) = (hf)/d
let d be the distance from the top of the compressed spring to the top of the motion

(d)sin(33) = hf
d = hf/sin(33)

d=112.1118/sin(33) = 205.8460cm

L = d-x (this is the x from earlier, or the distance the spring was compressed)

L = 205.8460 cm - 19cm = 186.846 cm

L = 186.8460 cm

the part with friction is similar but you have to account for energy lost to internal energy
 
Last edited:
gap0063 said:
then sin33=o/h
h=o/sin30
h=2.05846

did you actually do sin(30) ? maybe you just messed up the angle it looks like you did it right for the most part..
 

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