Chain on table - calculate work

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    Chain Table Work
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To calculate the work required to pull a chain with one-fourth of its length hanging over a frictionless table, the work done is equivalent to the change in potential energy of the chain. The method involves integrating the potential energy change of small elements of the chain as it is pulled up. The result shows that the work required is W = Mg/32, considering the center of mass of the hanging portion. Additionally, discussions on a marble rolling along a loop track highlight the need to account for both translational and rotational kinetic energy when calculating the minimum height for maintaining contact at the loop's top. The calculations reveal that the marble must be released from a height of 7/10 of its radius above the bottom of the loop to achieve this.
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1. A chain is help on a frictionless table with one-fourth of its length hanging over the edge. If the chain has length L and mass M, how much work is required to pull the hanging part back on the table?

i don't think i could have W = mgL/4
will the work change each time a new chain ring is on the table?
is there work from the horizontal chain if the table is frictionless?


2. A small solid marble of mass m and radius r rolls without slipping along the loop the loop track having been released from rest somewhere on the straight section of the track.
a) from what minimum height above the the bottom of the track must the marble be released in order that it just stay on the track at the top of the loop? (the radius of the loop is R , assume R>>r )
b) If the marble is released from height 6R above the bottom of the track, what is the horizontal component of the force acting on it when it is at height R in the loop.

Ui + Ki = Uf + Kf
mgh = mg2R
h = 2R
same as height it reaches
how can I account for friction?
 
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I'm a bit short on time, but here's a tip on question #1:

Since the forces are all conservative, the work done is equal in magnitude to the change in potential energy of the chain. The most straightforward way to think about it (neglecting comments about "center of mass" and so forth), is to discretize the hanging part of the chain into small elements of length dy and mass dm=M/L*dy. The change of the potential energy for such an element at point y, once the chain is pulled completely up, is:

dE(y) = dm \times g \times y = \frac{M g y dy}{L}

You must now integrate on the dangling part of the chain, i.e., from 0 to -L/4:

\Delta E = \int_{-L/4}^0 dE(y) = \frac{Mg}{32} (minus signs not withstanding)

This makes sense if you think about the dangling chain as a small, independent chain of length L/4 and mass M/4, with center of mass at -L/8 (half of L/4, the length). Pulling up this center off mass to table height requires work equal to:

W = mass of dangling chain * height of center of mass * g , or

W = \frac{M}{4} \times \frac{L}{8} \times g

which is the same answer.

--------
Assaf
http://www.physicallyincorrect.com/"
 
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Destrio said:
2. A small solid marble of mass m and radius r rolls without slipping along the loop the loop track having been released from rest somewhere on the straight section of the track.
a) from what minimum height above the the bottom of the track must the marble be released in order that it just stay on the track at the top of the loop? (the radius of the loop is R , assume R>>r )
b) If the marble is released from height 6R above the bottom of the track, what is the horizontal component of the force acting on it when it is at height R in the loop.

Ui + Ki = Uf + Kf
mgh = mg2R
h = 2R
same as height it reaches
how can I account for friction?
First figure out how fast the marble needs to be going at the top of the loop in order to maintain contact. (Hint: Use Newton's 2nd law, recognizing that the motion is circular.) Then use conservation of energy, but don't neglect rotational KE. (It's rolling without slipping.)
 
so

F=ma
centripedal force
Fc = mv^2/r
vcm = ωr
Fc = m(ωr)^2/r
Fc = mrω^2 = ma
ω = sqrt(a/r)
since a = g
ω = sqrt(g/r)

v = vcm

K total = (1/2)Mv^2 + (1/2)Iω^2
K total = (1/2)M(ωr)^2 + (1/2)Iω^2
K total = (1/2)M([sqrt(g/r)]r)^2 + (1/2)I[sqrt(g/r)]^2
K total = (1/2)Mgr + (1/2)Ig/r
K total = (1/2)Mgr + (1/2)Ig/r
I of a sphere = (2/5)Mr^2
K total = (1/2)Mgr + (1/2)((2/5)Mr^2)g/r
K total = (1/2)Mgr + (1/5)Mgr
K total = (7/10)Mgr

Etotal = Utotal - Ktotal
Mgh = (7/10)Mgr
h = (7/10)r

is this correct for the first part?

thanks
 
marble a)

Destrio said:
so

F=ma
centripedal force
Fc = mv^2/r
vcm = ωr
Fc = m(ωr)^2/r
Fc = mrω^2 = ma
ω = sqrt(a/r)
since a = g
ω = sqrt(g/r)
OK, you found the speed (and ω) of the marble at the top of the loop. Good!

(I would have left it as: gR = mv^2, but what you did was just fine.)

v = vcm

K total = (1/2)Mv^2 + (1/2)Iω^2
K total = (1/2)M(ωr)^2 + (1/2)Iω^2
K total = (1/2)M([sqrt(g/r)]r)^2 + (1/2)I[sqrt(g/r)]^2
K total = (1/2)Mgr + (1/2)Ig/r
K total = (1/2)Mgr + (1/2)Ig/r
I of a sphere = (2/5)Mr^2
K total = (1/2)Mgr + (1/2)((2/5)Mr^2)g/r
K total = (1/2)Mgr + (1/5)Mgr
K total = (7/10)Mgr
Here you found the total KE of the marble at the top of the loop. Good!

Etotal = Utotal - Ktotal
Mgh = (7/10)Mgr
h = (7/10)r

is this correct for the first part?
Almost. You found the height above the top of the loop, but they wanted the height above the bottom of the loop.
 
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