To solve this problem, we need to understand the relationship between Young's modulus, stress, and strain.
The Young's modulus (Y) is a measure of the ability of a material to withstand changes in length when under lengthwise tension or compression. It is defined as the ratio of tensile stress to tensile strain:
Y = \frac{\text{Stress}}{\text{Strain}}
The formula for extension (\(\Delta L\)) of a wire under a load is given by:
\Delta L = \frac{F \cdot L}{A \cdot Y}
where:
Given that the Young's modulus of steel is twice that of brass, we have:
Y_{\text{steel}} = 2Y_{\text{brass}}
Since the extensions for the wires need to be the same (so their lower ends remain at the same level), we set up the equation:
\frac{F_{\text{steel}} \cdot L}{A \cdot 2Y_{\text{brass}}} = \frac{F_{\text{brass}} \cdot L}{A \cdot Y_{\text{brass}}}
On simplifying, we find:
\frac{F_{\text{steel}}}{2} = F_{\text{brass}}
This implies:
F_{\text{steel}} = 2F_{\text{brass}}
Thus, the weights added to the steel and brass wires must be in the ratio 2:1.
The correct answer is 2:1.
A 2 $\text{kg}$ mass is attached to a spring with spring constant $ k = 200, \text{N/m} $. If the mass is displaced by $ 0.1, \text{m} $, what is the potential energy stored in the spring?
