Air resistance

On a free highway, a car accelerates uniformly with constant acceleration a = 1 m s 2 a = 1 \, \frac{\text{m}}{\text{s}^2} . Taking into account the air resistance, the equation of motion for the velocity v v reads

m d v d t = m a 1 2 c w ρ A v 2 m \cdot \frac{d v}{dt} = m \cdot a - \frac{1}{2} \cdot c_w \cdot \rho \cdot A \cdot v^2

with the mass m = 800 kg m = 800 \,\text{kg} and cross-sectional area A = 2 m 2 A = 2 \text{m}^2 of the car and the density ρ = 1.25 kg m 3 \rho = 1.25 \frac{\text{kg}}{\text{m}^3} of the air. The dimensionless factor c w c_w describes the drag coefficient, that depend on the actual shape of the car.

After a few minutes of acceleration the car reaches its top speed of v = lim t v ( t ) = 144 m s v_\infty = \lim_{t \to \infty} v(t) = 144 \, \frac{\text{m}}{\text{s}} . What is the value of the drag coefficient c w c_w ?

Bonus question: What is the actual solution for the differential equation?

0.4 0.67 1 0.15 1.33

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1 solution

Markus Michelmann
Sep 11, 2017

In the limiting case t t \to \infty the velocity approches a constant value v v_\infty , so that the total accelation d v d t \frac{dv}{dt} becomes zero. The equation of motion can be simplified to

0 = m a 1 2 c w ρ A v 2 c w = 2 m a ρ A v 2 = 2 800 1 1.25 2 1600 = 0.4 0 = m a - \frac{1}{2} c_w \rho A v_\infty^2 \qquad \Rightarrow \qquad c_w = \frac{2 m a}{\rho A v_\infty^2} = \frac{2 \cdot 800 \cdot 1}{1.25 \cdot 2 \cdot 1600} = 0.4

It seems we have two different values for the limiting velocity. 144 in the problem, and 40 in the solution.

Steven Chase - 3 years, 9 months ago

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The velocity in the problem should reads 144 km/h = 40 m/s. Thanks for your comment, I have corrected the units.

Markus Michelmann - 3 years, 9 months ago

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