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Nimfa-mama [501]
3 years ago
13

An airplane has wings, each with area A, designed so that air flows over the top of the wing at 265 m/s and underneath the wing

at 234 m/s. If the mass of the airplane is 7.2×10^3 kg then what is the area of each wing needed to produce enough lift? (air = 1.29 kg/m^3 )
Physics
1 answer:
exis [7]3 years ago
7 0

Answer

given,

Pressure on the top wing = 265 m/s

speed of underneath wings = 234 m/s

mass of the airplane =  7.2 × 10³ kg

density of air =  1.29 kg/m³

using Bernoulli's equation

 P_1 + \dfrac{1}{2}\rho v_1^2 = P_2 + \dfrac{1}{2}\rho v_2^2

 \Delta P =\dfrac{1}{2}\rho (v_2^2-v_1^2)

 \Delta P =\dfrac{1}{2}\times 1.29\times (265^2-234^2)

 \Delta P =9977.5 Pa

Applying newtons second law

2 Δ P x A - mg = 0

A =\dfrac{mg}{2\Delta P}

A =\dfrac{7.2\times 10^3 \times 9.8}{2\times 9977.5}

    A = 3.53 m²

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Cerrena [4.2K]

Answer:

a

The pressure will increase

b

T_2 =  576^oC

Explanation:

From the ideal gas law we have that

     PV  =  nRT

We see that the temperature varies directly with the pressure so if there is an increase in temperature that pressure will increase

   The initial  temperature is T_i  =  10^oC = 10 + 273 =  283 \  K

The objective of this solution is to obtain the temperature of the gas where the pressure is tripled

Now from the above equation given that nR and V  are constant  we have that

    \frac{P}{T}  =  constant

=>  \frac{P_1}{T_1}  =\frac{P_2}{T_2}

Let assume the initial  pressure is P_1 =  1 Pa

So tripling it will result  to the pressure being P_2 =  3 Pa

So

     \frac{1}{283}  =\frac{3}{T_2}  

=>   T_2  =  3 *  283

=>    T_2  =  3 *  283

=>    T_2  = 849 \ K

Converting back to ^oC

   T_2  =  849 -  273

=>  T_2 =  576^oC

8 0
2 years ago
The H line in Calcium is normally at 396.9nm. however, in a star’s spectrum it is measured at 398,1 nm. How fast is the star mov
konstantin123 [22]

H line of Calcium spectrum is normally given as 396.9 nm

Now from a distant star we measured it as 398.1 nm

So here this change in the wavelength of distant star is due to Doppler's effect of light as per which when source of light moves towards the observer then the frequency of light received will appear different from its actual frequency

So here we can say as per Doppler's effect of light

\frac{\Delta \nu}{\nu_0} = \frac{v}{c}

\frac{\nu' - \nu}{\nu_0} = \frac{v}{c}

\frac{\frac{1}{\lambda} - \frac{1}{\lambda'}}{\frac{1}{\lambda}} = \frac{v}{c}

\frac{\lambda' - \lambda}{\lambda'} = \frac{v}{c}

given that

\lambda' = 398.1 nm

\lambda = 396.9 nm

c = 3 * 10^8 m/s

\frac{398.1 - 396.9}{398.1} = \frac{v}{3*10^8}

v = 3*10^8 * \frac{1.2}{398.1}

v = 9.04 * 10^5 m/s

so the start is moving away with speed 9.04 * 10^5 m/s because when wavelength is more than the real wavelength then its frequency is less which mean it is moving away from the Earth

5 0
3 years ago
A 10 g bullet is fired into, and embeds itself in, a 2 kg block attached to a spring with a force constant of 19.6 n/m and whose
dmitriy555 [2]

Answer:

x=0.478\ m is the compression in the spring

Explanation:

Given:

  • mass of the bullet, m=10\ g=0.01\ kg
  • mass of block, M=2\ kg
  • stiffness constant of the spring, k=19.6\ N.m^{-1}
  • initial velocity of the spring just before it hits the block, u=300\ m.s^{-1}

<u>Now since the bullet-mass gets embed into the block, we apply the conservation of momentum as:</u>

m.u=(M+m).v

0.01\times 300=(2+0.01)\times v

v=1.4925\ m.s^{-1}

Now this kinetic energy of the combined mass gets converted into potential energy of the spring.

\rm Kinetic\ energy=Spring\ potential\ energy

\frac{1}{2} (M+m).v^2=\frac{1}{2} k.x^2

\frac{1}{2} \times (2+0.01)\times 1.4925^2=\frac{1}{2} \times 19.6\times x^2

x=0.478\ m is the compression in the spring

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