\( F = \frac{1}{2} \rho (v_1^2 - v_2^2)A \)
- Where: - \(\rho = 1.2 \, \text{kg/m}^3\) - \(v_1 = 70 \, \text{m/s}\) - \(v_2 = 65 \, \text{m/s}\) - \(A = 2 \, \text{m}^2\)
\( F = \frac{1}{2} \times 1.2 \times (70^2 - 65^2) \times 2 \)
\( F = \frac{1}{2} \times 1.2 \times (4900 - 4225) \times 2 \)
\( F = \frac{1}{2} \times 1.2 \times 675 \times 2 \)
\( F = 810 \, \text{N} \)
So, the correct answer is: \( F = 810 \, \text{N} \)
Step 1: Apply Bernoulli’s principle.
Pressure difference between lower and upper surfaces: \[ P_1 - P_2 = \frac{1}{2}\rho (v_2^2 - v_1^2) \] where \( v_1 = 65\,\text{m/s} \) (lower surface), \( v_2 = 70\,\text{m/s} \) (upper surface), and \( \rho = 1.2\,\text{kg/m}^3 \).
\[ P_1 - P_2 = \frac{1}{2} \times 1.2 \times (70^2 - 65^2) \] \[ = 0.6 \times (4900 - 4225) = 0.6 \times 675 = 405\,\text{N/m}^2 \]
Lift = Pressure difference × Area \[ F = (P_1 - P_2) \times A = 405 \times 2 = 810\,\text{N} \]
\[ \boxed{F = 810\,\text{N}} \]
A cube of side 10 cm is suspended from one end of a fine string of length 27 cm, and a mass of 200 grams is connected to the other end of the string. When the cube is half immersed in water, the system remains in balance. Find the density of the cube.
Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals:
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The dimension of $ \sqrt{\frac{\mu_0}{\epsilon_0}} $ is equal to that of: (Where $ \mu_0 $ is the vacuum permeability and $ \epsilon_0 $ is the vacuum permittivity)