Rigid Bodies and rotatational motion

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Homework Help Overview

The discussion revolves around a static equilibrium problem involving a sign suspended from a uniform rod, with a focus on calculating the tension in a support cable at an angle. The problem includes forces acting on the rod and the need to analyze torque and forces in both x and y directions.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the setup of the problem, questioning the application of torque and the equilibrium of forces. There is discussion about breaking down the tension into components and the correct approach to summing forces in different directions.

Discussion Status

Some participants have offered guidance on the importance of torque in the problem and suggested drawing a free body diagram. There is acknowledgment of the need to consider multiple forces and torques, with some participants expressing confusion about the setup and calculations involved.

Contextual Notes

Participants note the complexity of the problem due to the presence of multiple forces and the requirement to analyze both torque and force equilibrium. There is a mention of the need for clarity on the role of the wall's force and how it interacts with the other forces in the system.

in10sivkid
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yea...i'm having trouble today with my HW lol

a sign weighing 400 N is suspended at the end of a uniform rod 4.00 m weighing 500 N. what is the tension in the support cable if it makes an angle 40 with the rod?

now I'm curious i don't think Tclockwise = Tcounterclockwise comes into play

so i thought of this as a typical static equilibrium problem, but there is only 1 unknown that is the T in the cable that needs to be broken up into a vector

so exactly how does this get setup then

sum of Fx = Cos40F1 = 500 N + 500 N?
sum of Fy = Sin40F1 = 500 N + 400 N?

i know i am missing something
 
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help please?
 
in10sivkid said:
yea...i'm having trouble today with my HW lol

a sign weighing 400 N is suspended at the end of a uniform rod 4.00 m weighing 500 N. what is the tension in the support cable if it makes an angle 40 with the rod?

now I'm curious i don't think Tclockwise = Tcounterclockwise comes into play

so i thought of this as a typical static equilibrium problem, but there is only 1 unknown that is the T in the cable that needs to be broken up into a vector

so exactly how does this get setup then

sum of Fx = Cos40F1 = 500 N + 500 N?
sum of Fy = Sin40F1 = 500 N + 400 N?

i know i am missing something

Torque does come into play in this problem. There are forces acting where the rod is connected to the wall that are unkown in addition to the tension being unknown. Draw a free body diagram for the rod.
 
Last edited:
so curious would the summation of the forces in the y direction be

Sin40T + F1 (force rod is connected to the wall) = 400 N + 500 N
and but then the sum of the torque is getting me mixed up

if i choose the point where the rod is connected to the wall as the axis of rotation do I include Sin40T as well?


...also I'm having a hard time figuring out exactly how to setup the Torque if i do that...some help would be great
 
in10sivkid said:
so curious would the summation of the forces in the y direction be

Sin40T + F1 (force rod is connected to the wall) = 400 N + 500 N
and but then the sum of the torque is getting me mixed up

if i choose the point where the rod is connected to the wall as the axis of rotation do I include Sin40T as well?


...also I'm having a hard time figuring out exactly how to setup the Torque if i do that...some help would be great

Forget what I said (and deleted) about not needing the torque. It would apply only to a massless rod. Your equation for the vertical forces is correct. Choosing the point of contact of the rod and wall for the axis of rotation leaves you with three forces to consider for the torque calculation. This is the only equation you need. You would need the equation you wrote if you wanted to find the force the wall applies to the rod.

Calculate two clockwise torques: (1) the 400N sign at distance 4m and (2) the 500N weight of the rod at distance 2m (the center of the rod). Calculate the counterclockwise torque: the vertical component of tension Tsin40 at 4m. Equate the clockwise torques to counterclockwise torque and solve for T.
 

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