Related Formula
By Hooke's Law, the tension (T$T$) in a stretched elastic string is proportional to its change in length:
T = k · Δ L = k(L - L₀)$$T = k \cdot \Delta L = k(L - L_0)$$
where:
k$k$ = spring constant of the string
L$L$ = current stretched length
L₀$L_0$ = natural original length
Core Logic
We can set up two algebraic equations using the given conditions:
- Case 1: Tension T₁ = 5 N$T_1 = 5 \ \mathrm{N}$ produces stretched length L₁ = 1.4 m$L_1 = 1.4 \ \mathrm{m}$:
5 = k(1.4 - L₀) (1)$$5 = k(1.4 - L_0) \quad \dots (1)$$
- Case 2: Tension T₂ = 7 N$T_2 = 7 \ \mathrm{N}$ produces stretched length L₂ = 1.56 m$L_2 = 1.56 \ \mathrm{m}$:
7 = k(1.56 - L₀) (2)$$7 = k(1.56 - L_0) \quad \dots (2)$$
Step 1: Solve for natural length
Divide equation (1) by equation (2) to eliminate the spring constant k$k$:
(5)/(7) = (1.4 - L₀)/(1.56 - L₀)$$\frac{5}{7} = \frac{1.4 - L_0}{1.56 - L_0}$$
Cross-multiply and solve for L₀$L_0$:
5(1.56 - L₀) = 7(1.4 - L₀)$$5(1.56 - L_0) = 7(1.4 - L_0)$$
7.8 - 5 L₀ = 9.8 - 7 L₀$$7.8 - 5 L_0 = 9.8 - 7 L_0$$
Rearrange to isolate the variable:
2 L₀ = 9.8 - 7.8 = 2$$2 L_0 = 9.8 - 7.8 = 2$$
L₀ = 1 m$$L_0 = 1 \ \mathrm{m}$$
Thus, the original length of the string is 1 ~m$1 \mathrm{~m}$.
Pattern Recognition
Sees: Elastic stretching of a string/wire under variable load.
Trap: Attempting to resolve details like Young's modulus or cross-sectional area. Taking ratios allows the spring constant k$k$ to cancel cleanly, saving computational effort.
Shortcut: Use the ratio equation (T₁)/(T₂) = (L₁ - L₀)/(L₂ - L₀)$\frac{T_1}{T_2} = \frac{L_1 - L_0}{L_2 - L_0}$ directly. Solving the linear equation yields L₀ = 1 m$L_0 = 1\text{ m}$.
Chapter Mix
Class 11 Physics: Mechanical Properties of Solids