Does distance affect torque in hanging sign problem?

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Distance significantly affects torque in the hanging sign problem, as torque is a product of force and the perpendicular distance from the pivot point. When the sign is moved farther from the wall, the torque increases, resulting in a greater force on the hinge. The tension in the cables supporting the sign is evenly distributed, calculated to be 13 N for each cable. The equilibrium of forces and torques must be maintained, leading to a net reaction force from the wall that balances these tensions. Understanding these relationships is crucial for solving the problem accurately.
  • #31
haruspex said:
Does the textbook not teach the moments equivalent of ΣF=ma, namely, Στ=Iα (the sum of the moments about an axis equals the moment of inertia about that axis multiplied by the angular acceleration)?
In the special case of rotational stasis, the angular acceleration is zero, so it reduces to Στ=0, the net moment about the axis is zero.
Yes, they do teach on balance of moments. Why there is a need to understand about symmetry? Can you explain it in detail. Just curious to learn!
 
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  • #32
kuruman said:
The same way you found it before except that the left chain is at some distance ##x## from the hinge and the right change is at distance (##x+0.3 ## m) from the hinge. The idea is to get an expression for ##R_y## as you did before and see whether it increases or decreases as ##x## increases for part (c) and then plot ##R_y## vs. ##x## for part (d).

However, before you do all that, it is important to answer the question that @haruspex has been trying to get you to answer, "How does the equality of the distances from the edge of the chain imply that th tensions are the same?" To help you, here is another way to look at this is by answering the following question.

The sign is 0.4 m wide and has weight 26 N. The left chain is 0.1 m from the left edge and the right chain is right on the edge at 0.4 m from the left chain. Are the tensions ##T_L## and ##T_R## equal? Why? If they are not equal, find the teo tensions.

Related to all this is the equation you posted in #7 $$\begin{align}\sum\tau & = Mg\cdot d_B + mg\cdot d_S - T_C\cdot d_C \nonumber \\ & = 34\cdot 0.8 +26\cdot 1.15 - T_C\cdot 1.2 \nonumber \\T_C & = 47.58~\rm{N} \nonumber \end{align}$$I can see that in the second line 26 is the weight of the sign, but where did the ##1.15## come from? One chain is at 1.00 m and the other at 1.30 m from the hinge.
Do I need to find the net torque with this change in distances of left and right chain?
 
  • #33
paulimerci said:
Do I need to find the net torque with this change in distances of left and right chain?
Yes, and my hope is that you will get the same answer and see what is going on and why. If not, we can help you see it, but you have to do the work first.
 
  • #34
kuruman said:
Yes, and my hope is that you will get the same answer and see what is going on and why. If not, we can help you see it, but you have to do the work first.
Okay, should I take the left chain as ##x## and for right chain ##x+3.0##?
 
  • #35
Yes. Find an expression for ##R_y## containing ##x##. Then substitute ##x=1.00## m and see if you get the answer that you already got in part (b).

Correction to your work: The right chain should be ##x+0.3~##m.
 
  • #36
kuruman said:
Yes. Find an expression for ##R_y## containing ##x##. Then substitute ##x=1.00## m and see if you get the answer that you already got in part (b).

Correction to your work: The right chain should be ##x+0.3~##m.
Okay, if there are changes in distances does the values of ##T_c##, ##T_L##, and ##T_R## remains the same? If there is no change, then in the torque equation can I substitute for the values i calculated earlier for ##T_c##, ##T_L##, ##T_R##?
 
  • #37
paulimerci said:
Okay, if there are changes in distances does the values of ##T_c##, ##T_L##, and ##T_R## remains the same? If there is no change, then in the torque equation can I substitute for the values i calculated earlier for ##T_c##, ##T_L##, ##T_R##?
$$\sum\tau= T_c \cdot d_c-Mg \cdot d_B-T_L \cdot x-T_R \cdot (x+0.30)$$
$$1.2 \cdot T_c = 27.2+ 13 \cdot x + 13 \cdot(x+0.3)$$
$$T_c = \frac {31.1 +26 \cdot x} {1.2}$$
Substitute ##T_c## in the equation of ##R_y## we get,
$$ R_y = Mg +T_L+T_R-T_c$$
$$ R_y = 34+13+13- \frac{31.1+26\cdot x} {1.2}$$
$$ R_y = 60 - \frac{31.1+26\cdot x} {1.2}$$
have I done it right?
 
  • #38
Very good. Now you can answer parts (c) and (d) based on the equation you derived for ##R_y.##
 
  • #39
kuruman said:
Very good. Now you can answer parts (c) and (d) based on the equation you derived for ##R_y.##
Thanks for your guidance.
Part C,
Therefore, from the equation of ##R_y## we can justify that as the distance of the sign is moved farther away from the wall, the magnitude of the force on the hinge decreases.
 
  • #40
paulimerci said:
Thanks for your guidance.
Part C,
Therefore, from the equation of ##R_y## we can justify that as the distance of the sign is moved farther away from the wall, the magnitude of the force on the hinge decreases.
Correct. Now for the plot. Use a spreadsheet if you know how.
 
  • #41
kuruman said:
Correct. Now for the plot. Use a spreadsheet if you know how.
Screen Shot 2022-11-30 at 2.35.09 PM.png
 
  • #42
I think you're done. Congratulations! I hope you learned something from this experience.
 
  • #43
paulimerci said:
Looks like I plotted for ##T_c## vs ##x##. S
kuruman said:
I think you're done. Congratulations! I hope you learned something from this experience.
Definitely! It was a humongous problem and I didn't believe I can do it and I thank you so much for guiding me throughout! Thanks to @haruspex for his guidance too!
 
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