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iren2701 [21]
3 years ago
13

The car travels along the circular path such that its speed is increased by at = (0.5et ) m/s2 , where t is in seconds. Determin

e the magnitudes of its velocity and acceleration after the car has traveled s =18 m starting from rest. Neglect the size of the carDetermine the magnitude of its acceleration after the car has traveled s = 18 m starting from rest
Engineering
1 answer:
Zolol [24]3 years ago
6 0

Answer:

acceleration = 24.23 ms⁻¹

Explanation:

Let's gather the data:

The acceleration of the car is given by a = 0.5 e^{t}

The acceleration is the change in the speed in relation to time. In other words:

\frac{dv}{dt} = a = a = 0.5 e^{t}            ...1

Solving the differential equation yields:

v = 0.5 e^{t} + C₁

Initial conditions : 0 = 0.5 e^{0} + C₁

                             C₁ = -5

at any time t, the velocity is: v= 0.5e^{t}- 5

Solving for distance, s = 0. 5e^{t} - 0.5 t - 0.5

                                    18 = 0.5 e^{t} - 0.5 t - 0.5

                                       t = 3.71 s

Substitute t = 3.71 s

                   v= 0.5e^{t}- 5

                     = 19.85 m/s

a = 0.5 e^{t}             ...1

 = 20.3531

an = \frac{v^{2} }{p}

     = \frac{(19.853)^{2} }{30}

     = 13.1382

Magnitude of acceleration = \sqrt{ (a)^{2} + (an)^{2} }

                                            = \sqrt{(20.3531)^{2} +(13.1382)^{2}  }

                                            = 24.23 ms⁻¹ Ans

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A building window pane that is 1.44 m high and 0.96 m wide is separated from the ambient air by a storm window of the same heigh
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Answer:

the rate of heat loss by convection across the air space = 82.53 W

Explanation:

The film temperature

T_f = \frac{T_1+T_2}{2} \\\\= \frac{20-10}{2}\\\\= \frac{10}{2}\\\\= 5^0\ C

to kelvin = (5 + 273)K = 278 K

From  the " thermophysical properties of gases at atmospheric pressure" table; At T_f = 278 K ; by interpolation; we have the following

\frac{278-250}{300-250}= \frac{v-11.44(10^{-6})}{15.89(10^{-6})-11.44(10^{-6})}  → v 13.93 (10⁻⁶) m²/s

\frac{278-250}{300-250}= \frac{k-22.3(10^{-3}}{26.3(10^{-3}-22.3(10^{-3})} → k = 0.0245 W/m.K

\frac{278-250}{300-250}= \frac{\alpha - 15.9(10^{-6})}{22.5(10^{-6}-15.9(10^{-6})} → ∝ = 19.6(10⁻⁶)m²/s

\frac{278-250}{300-250}= \frac{Pr-0.720}{0.707-0.720} → Pr = 0.713

\beta = \frac{1}{T_f} \\=\frac{1}{278} \\ \\ = 0.00360 \ K ^{-1}

The Rayleigh number for vertical cavity

Ra_L  = \frac{g \beta (T_1-T_2)L^3}{\alpha v}

= \frac{9.81*0.00360(20-(-10))*0.06^3}{19.6(10^{-6})*13.93(10^{-6})}

= 8.38*10^5

\frac{H}{L}= \frac{1.44}{0.06} \\ \\= 24

For the rectangular cavity enclosure , the Nusselt number empirical correlation:

Nu_L = 0.42(8.38*10^5)^{\frac{1}{4}}(0.713)^{0.012}(24){-0.3}

NU_L= \frac{hL}{k}= 4.878

\frac{hL}{k}= 4.878

\frac{h*0.06}{0.0245}= 4.878

h = \frac{4.878*0.0245}{0.06}

h = 1.99 W/m².K

Finally; the rate of heat loss by convection across the air space;

q = hA(T₁ - T₂)

q = 1.99(1.4*0.96)(20-(-10))

q = 82.53 W

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