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Suppose a car is molded as a cylinder mo...

Suppose a car is molded as a cylinder moving on earth at a speed v. If A is the area of cross section of the car and `phi` is the density of air then

A

Power loss due to air resistance is `(A rho v^(3))/(2)`

B

Power loss due to air resistance is A `rho v^(3)`

C

drag force is `( A rho v^(2))/(2)`

D

charge force is `A rho v^(2)`

Text Solution

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The correct Answer is:
To solve the problem regarding the power loss due to air resistance for a car modeled as a cylinder moving at speed \( v \), we will follow these steps: ### Step 1: Understand the Drag Force Formula The drag force \( F_D \) acting on an object moving through a fluid (in this case, air) can be expressed using the formula: \[ F_D = \frac{1}{2} C_D \rho A v^2 \] where: - \( C_D \) is the drag coefficient (approximately 1 for a cylindrical shape), - \( \rho \) is the density of the fluid (air), - \( A \) is the cross-sectional area of the object, - \( v \) is the velocity of the object relative to the fluid. ### Step 2: Substitute the Values Since the car is modeled as a cylinder and we are given that the drag coefficient \( C_D \) is approximately 1, we can simplify the drag force to: \[ F_D = \frac{1}{2} \rho A v^2 \] ### Step 3: Calculate the Power Loss Due to Drag The power loss \( P \) due to air resistance can be calculated using the formula: \[ P = F_D \cdot v \] Substituting the expression for \( F_D \) from Step 2: \[ P = \left(\frac{1}{2} \rho A v^2\right) \cdot v \] This simplifies to: \[ P = \frac{1}{2} \rho A v^3 \] ### Step 4: Conclusion The power loss due to air resistance for the car moving at speed \( v \) is given by: \[ P = \frac{1}{2} \rho A v^3 \] ### Summary Thus, the power loss due to air resistance as the car moves through the air can be expressed in terms of the air density \( \rho \), the cross-sectional area \( A \), and the speed \( v \). ---
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