The problem asks for the maximum safe speed with which a car can navigate a banked circular turn, considering the forces of gravity, normal reaction, and static friction.
When a car is taking a turn on a banked road, the necessary centripetal force is provided by the horizontal components of the normal force and the frictional force. For the car to move at the maximum safe speed (\(v_{\text{max}}\)), it has a tendency to slide up the incline. Therefore, the force of static friction (\(f_s\)) acts down the incline.
By balancing the forces in the vertical direction and equating the net horizontal force to the required centripetal force (\( \frac{mv^2}{R} \)), we can derive the formula for the maximum safe speed:
\[ v_{\text{max}} = \sqrt{gR \left( \frac{\mu_s + \tan \theta}{1 - \mu_s \tan \theta} \right)} \]where:
Step 1: List the given parameters.
Step 2: Calculate the value of \(\tan\theta\).
\[ \tan \theta = \tan 30^\circ = \frac{1}{\sqrt{3}} = \frac{1}{1.73} \approx 0.578 \]Step 3: Substitute the given values into the formula for maximum speed.
\[ v_{\text{max}} = \sqrt{10 \times 300 \left( \frac{0.2 + 0.578}{1 - 0.2 \times 0.578} \right)} \]Step 4: Perform the numerical calculation step-by-step.
First, calculate the value of the expression in the parenthesis:
\[ \text{Numerator} = 0.2 + 0.578 = 0.778 \] \[ \text{Denominator} = 1 - (0.2 \times 0.578) = 1 - 0.1156 = 0.8844 \] \[ \frac{\text{Numerator}}{\text{Denominator}} = \frac{0.778}{0.8844} \approx 0.8797 \]Now, substitute this back into the main equation:
\[ v_{\text{max}} = \sqrt{3000 \times 0.8797} \] \[ v_{\text{max}} = \sqrt{2639.1} \]Step 5: Calculate the final value of the maximum speed.
\[ v_{\text{max}} \approx 51.37 \, \text{m/s} \]Rounding to one decimal place, we get 51.4 m/s.
The maximum speed with which the car can negotiate the turn safely is approximately 51.4 m/s.
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Find speed given to particle at lowest point so that tension in string at point A becomes zero. 


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