The absolute error in measurement using the screw gauge is the least count, i.e., \( 0.05 \) mm.
Fractional error in length measurement: \[ \frac{\Delta L}{L} = \frac{0.05}{5} = 0.01 \]
Fractional error in breadth measurement: \[ \frac{\Delta B}{B} = \frac{0.05}{2.5} = 0.02 \]
Area, \( A = L \times B \)
Maximum fractional error in area: \[ \left( \frac{\Delta A}{A} \right)_{\text{max}} = \left( \frac{\Delta L}{L} + \frac{\Delta B}{B} \right) \] \[ = 0.01 + 0.02 = 0.03 \]
The fractional error is given as \( \frac{x}{100} \). \[ 0.03 = \frac{x}{100} \] \[ x = 3 \]
\[ \boldsymbol{x = 3} \]
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).
Let \( T_r \) be the \( r^{\text{th}} \) term of an A.P. If for some \( m \), \( T_m = \dfrac{1}{25} \), \( T_{25} = \dfrac{1}{20} \), and \( \displaystyle\sum_{r=1}^{25} T_r = 13 \), then \( 5m \displaystyle\sum_{r=m}^{2m} T_r \) is equal to: