Isotonic solutions have the same osmotic pressure. The osmotic pressure ($\pi$) is given by:
\[ \pi = CRT \]
where C is the molar concentration, R is the gas constant, and T is the temperature.
For isotonic solutions, $\pi_1 = \pi_2$, so:
\[ C_1RT = C_2RT \]
Since R and T are the same for both solutions, we have $C_1 = C_2$.
First, let's calculate the molar concentration of the urea solution:
Molar mass of urea (NH$_2$CONH$_2$) = (2 $\times$ 14) + (4 $\times$ 1) + 12 + 16 = 60 g/mol
Concentration of urea ($C_1$) = $\frac{mass}{molar mass \times volume} = \frac{15 g}{60 g/mol \times 1 L} = 0.25$ M
Now, we know the molar concentration of the glucose solution must also be 0.25 M. We can use this to calculate the mass of glucose needed:
Molar mass of glucose (C$_6$H$_{12}$O$_6$) = (6 $\times$ 12) + (12 $\times$ 1) + (6 $\times$ 16) = 180 g/mol
Mass of glucose (m) = $C_2 \times molar mass \times volume = 0.25 M \times 180 g/mol \times 1 L = 45$ g
Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity) 
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is : 