Understanding the Physical Constraint
Imagine a brass rod hanging from the ceiling, supporting a heavy load of 400 N. We are tasked with finding out exactly how thin this rod can be without undergoing permanent deformation.
To prevent this permanent stretching, the internal stress developed within the rod must strictly not exceed its elastic limit. The elastic limit is the maximum stress a material can withstand and still return to its original shape once the load is removed.
The Mathematics of Stress
Stress is defined as the internal restoring force per unit cross-sectional area. Mathematically, it is expressed as:
σ=AF
For the rod to remain within its elastic behavior, we enforce the condition:
σ≤σlimit
Since the rod is cylindrical, its cross-sectional area
A can be written in terms of its diameter
d as:
A=4πd2
Substituting this area into our stress inequality gives us a direct relationship between the applied force, the elastic limit, and the required diameter:
πdmin24F=σlimit
Calculating the Minimum Diameter
Now, we rearrange our equation to solve for the minimum diameter squared. By cross-multiplying, we isolate the diameter term:
dmin2=πσlimit4F
It is time to plug in our known values. The applied force
F is
400 N, and the elastic limit
σlimit is
379 MPa. Remember that the prefix "Mega" stands for
106, so we must convert this to standard SI units:
dmin2=π×379×1064×400
Evaluating this expression yields the square of the diameter:
dmin2≈1.343×10−6 m2
Taking the square root gives us the final minimum diameter:
dmin≈1.16×10−3 m
Converting this to millimeters, we get 1.16 mm. If the rod were any thinner than this, the stress would exceed 379 MPa, and the brass would permanently deform!