Respuesta :
Answer:
[tex]\theta = 22.29[/tex]
Explanation:
Taking summation of force at perpendicular to the plane
[tex]\sum F_p = 0[/tex]
[tex]2N_A +2N_B -mgcos\theta = 0[/tex]
[tex]N_A +N_B - mgcos\theta = 0
[/tex]
[tex]N_A +N_B = mgcos\theta[/tex]
Taking summation along the plane, therefore we have
[tex]\sum Fa = 0[/tex]
[tex]f_A +f_B -mgsin\theta = 0[/tex]
[tex]\mu N_A+\mu N_B - mgsin\theta = 0[/tex]
[tex]\mu(N_A +N_B) = mgcos\theta[/tex]
from equation 1 and 2 we have
[tex]\mu =\frac{sin\theta}{cos\theta}[/tex]
[tex]\mu = 0.41[/tex]
[tex]\mu = tan\theta
[/tex]
[tex]\theta = tan^{-}\mu[/tex]
[tex]\theta = 22.29[/tex]
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The greatest slope the shoulder can have without causing the car to slip or tip over is 22.3⁰.
The given parameters;
- mass of the car, m = 1.6 Mg
- coefficient of static friction, [tex]\mu_ s[/tex] = 0.41
The greatest slope of the shoulder is determined by taking net force on the car as shown below;
[tex]\Sigma F= ma \\\\Wsin\theta - \mu_s Wcos \theta = ma[/tex]
at constant velocity, acceleration, a, = 0
[tex]Wsin\theta - \mu_s W cos \theta = 0\\\\W sin\theta = \mu_s Wcos \theta \\\\\mu_s = \frac{Wsin\theta }{W cos \theta } \\\\\mu_s = tan \theta \\\\\theta = tan^{-1}(\mu_s)\\\\\theta = tan^{-1}(0.41)\\\\\theta =22.3\ ^0[/tex]
Thus, the greatest slope the shoulder can have without causing the car to slip or tip over is 22.3⁰.
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