Step 1: Weight of the sphere The weight of the sphere w is given by:
\( w = \frac{4}{3} \pi \left( D^3 - \frac{d^3}{8} \right) \sigma g, \)
where:
Step 2: Buoyant force The buoyant force \( F_b \) is given by:
\( F_b = \frac{4}{3} \pi \left( \frac{D^3}{8} \right) g, \)
where \( \frac{D^3}{8} \) is the volume of displaced water.
Step 3: Equilibrium condition For the sphere to just float, the weight equals the buoyant force:
\( w = F_b. \)
Substitute expressions for \( w \) and \( F_b \):
\( \frac{4}{3} \pi \left( D^3 - \frac{d^3}{8} \right) \sigma g = \frac{4}{3} \pi \left( \frac{D^3}{8} \right) g. \)
Cancel common terms:
\( \left( D^3 - d^3 \right) \sigma = D^3. \)
Simplify:
\( D^3 - d^3 = \frac{D^3}{\sigma}. \)
Step 4: Solve for \(\frac{d}{D}\) Divide through by \( D^3 \):
\( 1 - \frac{d^3}{D^3} = \frac{1}{\sigma}. \)
Rearrange:
\( \frac{d^3}{D^3} = 1 - \frac{1}{\sigma}. \)
Take the cube root:
\( \frac{d}{D} = \left( 1 - \frac{1}{\sigma} \right)^{\frac{1}{3}}. \)
Invert to find \( \frac{D}{d} \):
\( \frac{D}{d} = \left( \frac{\sigma}{\sigma - 1} \right)^{\frac{1}{3}}. \)
Final Answer: \( \frac{D}{d} = \left( \frac{\sigma}{\sigma - 1} \right)^{\frac{1}{3}}. \)
Which of the following statements are true?
A. The same Bernoulli's equation is applicable to all the points in the flow field if the flow is irrotational.
B. The value of "Constant in the Bernoulli's equation" is different for different streamlines if the flow is rotational.
C. When a nozzle is fitted at the end of a long pipeline, the discharge increases.
D. The velocity of flow at the nozzle end is more than that in the case of a pipe without a nozzle, the head in both cases being the same.
Choose the most appropriate answer from the options given below:
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: