Analyzing the Setup
The problem asks us to analyze how the errors in calculating the slit separation d change as the measured angle θ increases. We are given the relation 2dsinθ=λ, where the wavelength λ is a known constant, and the error in measuring the angle, Δθ, is also constant.
Our first step is to express the quantity we are calculating,
d, in terms of the measured quantity,
θ. Rearranging the given equation, we get:
d=2sinθλ
The Master Equation for Errors
To find the fractional error
dΔd, the most elegant method is logarithmic differentiation. By taking the natural logarithm of both sides, we convert the division into subtraction, which is much easier to differentiate.
lnd=lnλ−ln2−lnsinθ
Now, we differentiate this expression. Remember that
λ and
2 are constants, so their derivatives are zero.
dΔd=0−0−sinθ1⋅cosθ⋅Δθ
dΔd=−cotθ⋅Δθ
When dealing with errors, we are interested in the maximum possible error, so we take the absolute value (magnitude):
Final Calculation and Conclusion
We are given that Δθ is constant. Now we need to see how the fractional error behaves as θ increases from 0∘ to 90∘. In the first quadrant, as the angle increases, the value of the cotangent function (cotθ) strictly decreases. Since the fractional error is directly proportional to cotθ, it must also decrease.
Let's also quickly check the absolute error,
Δd, just to be thorough. We can find it by multiplying the fractional error by
d:
Δd=d⋅cotθ⋅Δθ
Substituting
d=2sinθλ, we get:
Δd=(2sinθλ)(sinθcosθ)Δθ=2sin2θλcosθΔθ
As θ increases from 0∘ to 90∘, the numerator cosθ decreases, while the denominator sin2θ increases. A decreasing numerator divided by an increasing denominator means the entire fraction decreases. Thus, the absolute error Δd also decreases.
Looking at the given options, the only correct statement is that the fractional error in d decreases.