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Question: In the determination of acceleration due to gravity ( \( g \) ) using the formula \( T = 2\pi \sqrt ...

In the determination of acceleration due to gravity ( gg ) using the formula T=2πLgT = 2\pi \sqrt {\dfrac{L}{g}} , the errors in measurement of L and T are 1% and 2% respectively. The maximum percentage error in the value of gg is
(A) 5%
(B) 4%
(C) 3%
(D) 1.5%1.5\%

Explanation

Solution

Hint Percentage error can be given as the error divided by the true or used value (usually the mean value) multiplied by one hundred per cent. We need to derive an expression for error in gg as a function of error in LL , and TT .
Formula used: In this solution we will be using the following formula;
T=2πLg\Rightarrow T = 2\pi \sqrt {\dfrac{L}{g}} where TT is the period, LL is the length, gg is the acceleration due to gravity.
P.Ev=ΔVV×100%\Rightarrow P.{E_v} = \dfrac{{\Delta V}}{V} \times 100\% , where VV is a variable, ΔV\Delta V is the error in the variable, and P.EvP.{E_v} is the percentage error of the variable

Complete step by step answer
From the question, we have that
T=2πLg\Rightarrow T = 2\pi \sqrt {\dfrac{L}{g}} where TT is the period, LL is the length, gg is the acceleration due to gravity. We are to look for the percentage error in the determination of gg based on the error in the measurement of the period TT and length LL .
First, we must make gg subject of the formula.
Hence, squaring both sides we have
T2=4π2(Lg)\Rightarrow {T^2} = 4{\pi ^2}\left( {\dfrac{L}{g}} \right) . Multiplying by both sides by gg and dividing by T2{T^2} , we have
g=4π2(LT2)\Rightarrow g = 4{\pi ^2}\left( {\dfrac{L}{{{T^2}}}} \right)
From mathematical principles, it can be proven that
Δgg=(ΔLL+2ΔTT)\Rightarrow \dfrac{{\Delta g}}{g} = \left( {\dfrac{{\Delta L}}{L} + 2\dfrac{{\Delta T}}{T}} \right)
Multiplying all through by one hundred per cent we have
Δgg×100%=(ΔLL×100%+2ΔTT×100%)\Rightarrow \dfrac{{\Delta g}}{g} \times 100\% = \left( {\dfrac{{\Delta L}}{L} \times 100\% + 2\dfrac{{\Delta T}}{T} \times 100\% } \right)
From the expression of percentage error which is given by
P.Ev=ΔVV×100%\Rightarrow P.{E_v} = \dfrac{{\Delta V}}{V} \times 100\% , where VV is a variable, ΔV\Delta V is the error in the variable, and P.EvP.{E_v} is the percentage error of the variable. We have that
P.Eg=(P.EL+2×P.ET)\Rightarrow P.{E_g} = \left( {P.{E_L} + 2 \times P.{E_T}} \right) ,
According to the question P.EL=1%P.{E_L} = 1\% and P.ET=2%P.{E_T} = 2\% hence, replacing into formula above, we have
P.Eg=(1%+2×2%)=5%\Rightarrow P.{E_g} = (1\% + 2 \times 2\% ) = 5\% .
P.Eg=5%\therefore P.{E_g} = 5\%
Hence the correct answer is option A.

Note
To avoid confusions, we shall prove that Δgg=(ΔLL+2ΔTT)\dfrac{{\Delta g}}{g} = \left( {\dfrac{{\Delta L}}{L} + 2\dfrac{{\Delta T}}{T}} \right) as follows:
Mathematically,
dg=gldl+gTdT\Rightarrow dg = \dfrac{{\partial g}}{{\partial l}}dl + \dfrac{{\partial g}}{{\partial T}}dT
Hence, from g=4π2(LT2)g = 4{\pi ^2}\left( {\dfrac{L}{{{T^2}}}} \right) , differentiating gg we have,
dg=4π2T2dl+(24π2T3dT)\Rightarrow dg = \dfrac{{4{\pi ^2}}}{{{T^2}}}dl + \left( { - 2\dfrac{{4{\pi ^2}}}{{{T^3}}}dT} \right) , factorising out 4π24{\pi ^2} , we have
dg=4π2[1T2dl+(2LT3dT)]\Rightarrow dg = 4{\pi ^2}\left[ {\dfrac{1}{{{T^2}}}dl + \left( { - 2\dfrac{L}{{{T^3}}}dT} \right)} \right]
Now, observe from g=4π2(LT2)g = 4{\pi ^2}\left( {\dfrac{L}{{{T^2}}}} \right) that
1T2=g4π2L\Rightarrow \dfrac{1}{{{T^2}}} = \dfrac{g}{{4{\pi ^2}L}} and LT2=g4π2\dfrac{L}{{{T^2}}} = \dfrac{g}{{4{\pi ^2}}} . Hence, replacing these in gg , we have
dg=4π2[g4π2LdL+(2g4π2dT)]dg = 4{\pi ^2}\left[ {\dfrac{g}{{4{\pi ^2}L}}dL + \left( { - 2\dfrac{g}{{4{\pi ^2}}}dT} \right)} \right] .
Dividing through by gg and cancelling 4π24{\pi ^2}
We have that
dgg=4π2[dLL+(2dTT)]\Rightarrow \dfrac{{dg}}{g} = 4{\pi ^2}\left[ {\dfrac{{dL}}{L} + \left( { - 2\dfrac{{dT}}{T}} \right)} \right] .
Hence,
Δgg=[ΔLL+(2(ΔT)T)]\Rightarrow \dfrac{{\Delta g}}{g} = \left[ {\dfrac{{\Delta L}}{L} + \left( { - 2\dfrac{{( - \Delta T)}}{T}} \right)} \right] ( dT=ΔTdT = - \Delta T because, in this case, for increase in Δg\Delta g there’s a corresponding decrease in ΔT\Delta T as obvious in the expression for gg )
Hence, finally,
Δgg=(ΔLL+2ΔTT)\Rightarrow \dfrac{{\Delta g}}{g} = \left( {\dfrac{{\Delta L}}{L} + 2\dfrac{{\Delta T}}{T}} \right) .