A stone of mass is tied to the end of a massless string of length . If the breaking tension of the string is , then maximum linear velocity the stone can have without breaking the string, while rotating in horizontal plane, is:
- A
- B
- C
- D
A stone of mass is tied to the end of a massless string of length . If the breaking tension of the string is , then maximum linear velocity the stone can have without breaking the string, while rotating in horizontal plane, is:
Correct answer:B
Standard Method
Given: mass of stone , string length , maximum tension .
Find: the maximum linear velocity of the stone without breaking the string.
At the limiting condition, the maximum velocity occurs when the centripetal force equals the maximum tension in the string.
Setting centripetal force equal to tension:
Substitute the given values:
Therefore, the maximum linear velocity is . The solution states the correct option is B, but this value matches option A, so the source has an option-label discrepancy.
Using the tension limit
Given: the stone moves in a horizontal circle and the string can sustain at most tension.
Find: the highest possible speed before the string breaks.
The string provides the required centripetal force. Hence the largest allowed speed is obtained when the required centripetal force becomes exactly equal to the breaking tension.
With and :
Therefore, the correct numerical value is , which corresponds to option A in the listed options.
Using the wrong force relation, such as or a linear-force guess, is incorrect because circular motion requires centripetal force. Use or equivalently .
Choosing by forgetting to take the square root is wrong because from , the speed is , not or .
Treating the breaking tension as an extra force in addition to centripetal force is incorrect because the tension itself provides the centripetal force here. Set the maximum tension equal to the required centripetal force.
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