5. When a road is dry, a particular car can safely navigate a turn with a 155 m radius of curvature at a maximum speed of 26.0 m/s without slipping. What is the coefficient of static friction between the tires and the road?

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**Physics Problem: Coefficient of Static Friction**

**Problem Statement:**

When a road is dry, a particular car can safely navigate a turn with a 155 m radius of curvature at a maximum speed of 26.0 m/s without slipping. What is the coefficient of static friction between the tires and the road?

**Solution:**

To find the coefficient of static friction (\(\mu_s\)), we can use the formula for centripetal force, which must be provided by the frictional force for the car to navigate the turn safely:

\[ f_{\text{friction}} = \mu_s \cdot F_{\text{normal}} = \mu_s \cdot (m \cdot g) \]

The centripetal force (\(F_{\text{centripetal}}\)) necessary for the car to navigate the turn is given by:

\[ F_{\text{centripetal}} = \frac{m \cdot v^2}{r} \]

Where:
- \(m\) is the mass of the car
- \(v\) is the speed of the car (26.0 m/s)
- \(r\) is the radius of curvature (155 m)
- \(g\) is the acceleration due to gravity (approximately 9.8 m/s²)

Since \(f_{\text{friction}} = F_{\text{centripetal}}\), we have:

\[ \mu_s \cdot (m \cdot g) = \frac{m \cdot v^2}{r} \]

The masses (\(m\)) cancel out, leaving:

\[ \mu_s \cdot g = \frac{v^2}{r} \]

Solving for \(\mu_s\):

\[ \mu_s = \frac{v^2}{r \cdot g} \]

Plug in the values:

\[ \mu_s = \frac{(26.0 \, \text{m/s})^2}{155 \, \text{m} \cdot 9.8 \, \text{m/s}^2} \]

\[ \mu_s = \frac{676 \, \text{m}^2/\text{s}^2}{1519 \, \text{m}^2/\text{s}^2} \]

\[ \mu_s = 0.445 \]

Thus, the coefficient of static
Transcribed Image Text:**Physics Problem: Coefficient of Static Friction** **Problem Statement:** When a road is dry, a particular car can safely navigate a turn with a 155 m radius of curvature at a maximum speed of 26.0 m/s without slipping. What is the coefficient of static friction between the tires and the road? **Solution:** To find the coefficient of static friction (\(\mu_s\)), we can use the formula for centripetal force, which must be provided by the frictional force for the car to navigate the turn safely: \[ f_{\text{friction}} = \mu_s \cdot F_{\text{normal}} = \mu_s \cdot (m \cdot g) \] The centripetal force (\(F_{\text{centripetal}}\)) necessary for the car to navigate the turn is given by: \[ F_{\text{centripetal}} = \frac{m \cdot v^2}{r} \] Where: - \(m\) is the mass of the car - \(v\) is the speed of the car (26.0 m/s) - \(r\) is the radius of curvature (155 m) - \(g\) is the acceleration due to gravity (approximately 9.8 m/s²) Since \(f_{\text{friction}} = F_{\text{centripetal}}\), we have: \[ \mu_s \cdot (m \cdot g) = \frac{m \cdot v^2}{r} \] The masses (\(m\)) cancel out, leaving: \[ \mu_s \cdot g = \frac{v^2}{r} \] Solving for \(\mu_s\): \[ \mu_s = \frac{v^2}{r \cdot g} \] Plug in the values: \[ \mu_s = \frac{(26.0 \, \text{m/s})^2}{155 \, \text{m} \cdot 9.8 \, \text{m/s}^2} \] \[ \mu_s = \frac{676 \, \text{m}^2/\text{s}^2}{1519 \, \text{m}^2/\text{s}^2} \] \[ \mu_s = 0.445 \] Thus, the coefficient of static
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