The duration required for the stone to reach the ground.
\(t=\sqrt{\frac{2 L}{g}}+\frac{L}{C}\)
Here,C represents the speed of sound.
Now, differentiating the above equation
\(\frac{d t}{d L}=\sqrt{\frac{L}{g}} \times \frac{1}{2 \sqrt{L}}+\frac{1}{C}\)
\(dL =\frac{ dt }{\frac{1}{\sqrt{2 gL }}+\frac{1}{ C }}\)
We hat dt=0.01
\(\Rightarrow \frac{ dL }{ L } \times 100=\left(\frac{ dt }{\frac{1}{\sqrt{2 gL }}+\frac{1}{ C }}\right) \frac{1}{ L } \times 100\)
\(=\frac{15}{16 \%} \approx 1 \%\)
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____
Let $ S $ denote the locus of the point of intersection of the pair of lines $$ 4x - 3y = 12\alpha,\quad 4\alpha x + 3\alpha y = 12, $$ where $ \alpha $ varies over the set of non-zero real numbers. Let $ T $ be the tangent to $ S $ passing through the points $ (p, 0) $ and $ (0, q) $, $ q > 0 $, and parallel to the line $ 4x - \frac{3}{\sqrt{2}} y = 0 $.
Then the value of $ pq $ is
The physical world includes the complications of the natural world around us. It is a type of analysis of the physical world around us to understand how it works. The fundamental forces that control nature are: