To solve this problem, we need to identify the correct form of Bernoulli's equation. Bernoulli's equation is a principle in fluid dynamics that describes the conservation of energy in a flowing fluid. It is applicable to incompressible, non-viscous fluids. The equation relates the pressure energy, kinetic energy per unit volume, and potential energy per unit volume of a fluid flowing along a streamline.
The general form of Bernoulli's equation is given as:
\(P + \frac{1}{2} \rho v^2 + \rho gh = \text{constant}\)
Now let's analyze the given options:
Therefore, the correct form of Bernoulli's equation is represented by option 2: \(P + \rho gh + \frac{1}{2} \rho v^2 = \text{constant}\).
Bernoulli’s equation for fluid flow is:
\[ P + \rho gh + \frac{1}{2} \rho v^2 = \text{constant}. \]
Here:
P is the pressure,
\(\rho\) is the density of the fluid,
g is the acceleration due to gravity,
h is the height,
v is the velocity.
Final Answer: \[ P + \rho gh + \frac{1}{2} \rho v^2 = \text{constant}. \]
$\text{The fractional compression } \left( \frac{\Delta V}{V} \right) \text{ of water at the depth of } 2.5 \, \text{km below the sea level is } \_\_\_\_\_\_\_\_\_\_ \%. \text{ Given, the Bulk modulus of water } = 2 \times 10^9 \, \text{N m}^{-2}, \text{ density of water } = 10^3 \, \text{kg m}^{-3}, \text{ acceleration due to gravity } g = 10 \, \text{m s}^{-2}.$
Let A be a 3 × 3 matrix such that \(\text{det}(A) = 5\). If \(\text{det}(3 \, \text{adj}(2A)) = 2^{\alpha \cdot 3^{\beta} \cdot 5^{\gamma}}\), then \( (\alpha + \beta + \gamma) \) is equal to:
