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A car of mass 1000kg negotiates a banked...

A car of mass `1000kg` negotiates a banked curve of radius `90m` on a fictionless road. If the banking angle is `45^(@)` the speed of the car is:

A

`10ms^(-1)`

B

`20ms^(-1)`

C

`30ms^(-1)`

D

`5ms^(-1)`

Text Solution

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The correct Answer is:
To solve the problem of a car negotiating a banked curve without friction, we can follow these steps: ### Step-by-Step Solution: 1. **Identify Given Values:** - Mass of the car, \( m = 1000 \, \text{kg} \) (not needed for calculations as it cancels out) - Radius of the curve, \( r = 90 \, \text{m} \) - Banking angle, \( \theta = 45^\circ \) - Acceleration due to gravity, \( g = 10 \, \text{m/s}^2 \) 2. **Understand the Forces Acting on the Car:** - The normal force \( N \) acts perpendicular to the surface of the banked road. - The gravitational force \( mg \) acts downward. - There is no friction, so the only forces providing the centripetal acceleration are the components of the normal force. 3. **Set Up the Equations:** - In the vertical direction, the forces must balance: \[ N \cos \theta = mg \] - In the horizontal direction, the centripetal force required for circular motion is provided by the horizontal component of the normal force: \[ N \sin \theta = \frac{mv^2}{r} \] 4. **Express Normal Force \( N \):** - From the vertical force balance: \[ N = \frac{mg}{\cos \theta} \] 5. **Substitute \( N \) into the Horizontal Force Equation:** - Replace \( N \) in the horizontal equation: \[ \frac{mg}{\cos \theta} \sin \theta = \frac{mv^2}{r} \] 6. **Simplify the Equation:** - Cancel \( m \) from both sides: \[ \frac{g \sin \theta}{\cos \theta} = \frac{v^2}{r} \] - This can be rewritten using the tangent function: \[ g \tan \theta = \frac{v^2}{r} \] 7. **Solve for \( v^2 \):** - Rearranging gives: \[ v^2 = g \tan \theta \cdot r \] 8. **Calculate \( \tan \theta \):** - For \( \theta = 45^\circ \): \[ \tan 45^\circ = 1 \] 9. **Substitute Values:** - Now substitute \( g = 10 \, \text{m/s}^2 \), \( \tan 45^\circ = 1 \), and \( r = 90 \, \text{m} \): \[ v^2 = 10 \cdot 1 \cdot 90 = 900 \] 10. **Find \( v \):** - Taking the square root gives: \[ v = \sqrt{900} = 30 \, \text{m/s} \] ### Final Answer: The speed of the car is \( 30 \, \text{m/s} \). ---

To solve the problem of a car negotiating a banked curve without friction, we can follow these steps: ### Step-by-Step Solution: 1. **Identify Given Values:** - Mass of the car, \( m = 1000 \, \text{kg} \) (not needed for calculations as it cancels out) - Radius of the curve, \( r = 90 \, \text{m} \) - Banking angle, \( \theta = 45^\circ \) ...
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Knowledge Check

  • A car of mass 1000 kg negotiates a banked curve of radius 90 m on a frictionless road. If the banking angle is 45^@ , the speed of the car is

    A
    `20 ms^(-1)`
    B
    `30 ms^(-1)`
    C
    `5 ms^(-1)`
    D
    `10 ms^(-1)`
  • A car of mass 1500 kg rounds a curve of radius 250 m , at 90 km / hour . What is the centripetal force acting on it ?

    A
    `2550N`
    B
    `3100N`
    C
    `3750 N`
    D
    `4200N`
  • The banking angle for a curved road of radius 490 m for a vehicle moving at 35 ms^(-1) is

    A
    `tan^(-1) ( 0.25 )`
    B
    ` tan ^(-1) ( 0.35 )`
    C
    `tan^(-1) (1)`
    D
    `tan^(-1) ( 0.65 )`
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