The Physical Setup
Stretching a Wire
Imagine you are in a physics laboratory, tasked with determining the Young's modulus of a metallic wire. You suspend the wire from a rigid support and attach a heavy mass to its free end. As gravity pulls the mass downwards, the wire experiences a stretching force, causing it to elongate slightly.
This simple setup is the foundation of our problem. We are given four key measurements: the original length of the wire (L), its radius (R), the mass attached (m), and the resulting elongation (Δl). However, no measurement is perfect. Each instrument used—whether it's a meter scale, a vernier caliper, or a screw gauge—has a least count, which represents the maximum possible absolute error in that measurement.
The Mathematical Engine
Young's Modulus
To understand how these individual errors affect our final result, we first need the mathematical relationship connecting them. Young's modulus (Y) is defined as the ratio of longitudinal stress to longitudinal strain.
The stress is the restoring force per unit area. Here, the force is the weight of the mass (mg), and the cross-sectional area of the wire is πR2. The strain is the fractional change in length, given by LΔl. Substituting these into our definition, we get the master equation:
The Art of Error Propagation
Now comes the crucial step: translating our physical formula into an error propagation equation. When physical quantities are multiplied or divided, their maximum fractional (or relative) errors add up.
We take the relative error of each variable in our master equation. Constants like the acceleration due to gravity (g) and π are exact values in this context, so their error contribution is zero.
There is a vital trap to avoid here: the radius (R) is squared in the formula. According to the rules of error analysis, the power of a quantity becomes a multiplier for its relative error. Therefore, the fractional error equation becomes:
YΔY=mΔm+LΔL+2RΔR+ΔlΔ(Δl)
Taming the Units
Substitution
Before we plug in the numbers, we must carefully extract the measured values and their absolute errors (least counts) from the problem statement.
- Radius: R=0.2 cm, ΔR=0.001 cm
- Length: L=1 m=1000 mm, ΔL=1 mm
- Mass: m=1 kg=1000 g, Δm=1 g
- Elongation: Δl=0.5 cm, Δ(Δl)=0.001 cm
Notice that we don't necessarily need to convert everything to standard SI units (like meters and kilograms). Because fractional error is a ratio (e.g., mΔm), the units will perfectly cancel out as long as the numerator and denominator of each individual term share the same unit.
Substituting these values into our error equation:
YΔY=1000 g1 g+1000 mm1 mm+2(0.2 cm0.001 cm)+0.5 cm0.001 cm
The Final Tally
Calculating the Error
Now, we execute the arithmetic. Let's simplify each fraction step-by-step to avoid any silly mistakes.
YΔY=10001+10001+2(2001)+5001
Converting these fractions into decimals makes the final addition straightforward:
YΔY=0.001+0.001+0.010+0.002
Adding them all together yields the total fractional error:
The question asks for the fractional error, but a quick glance at the options reveals they are all in percentages. To convert a fractional error to a percentage error, we simply multiply by 100%.
Percentage Error=0.014×100%=1.4%
A Crucial Insight
The Dominant Error
Before we move on, let's look at the numbers we just added. The term for the radius (0.010) contributed the vast majority of the total error (0.014).
Why? Because the radius is a very small value, making its relative error large, and it is squared in the formula, which doubles its impact! If you were an engineer trying to improve the accuracy of this experiment, your primary focus should be on measuring the radius of the wire with a much more precise instrument.