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natima [27]
3 years ago
7

Water flows in a 0.15-m-diameter vertical pipe at a rate of 0.20 m3/s and a pressure of 210 kPa at an elevation of 25 m. Determi

ne (a) velocity head at elevation of 20 m, (b) pressure head at elevation of 20 m, (c) velocity head at elevation of 55 m, (d) pressure head at elevation of 55 m.
Physics
1 answer:
madreJ [45]3 years ago
3 0

Answer:

(a). The velocity head at elevation of 20 m is 6.52 m/s.

(b). The pressure head at elevation of 20 m is 26.42 m.

(c). The velocity is 6.52 m/s.

(d). The pressure head at elevation of 55 m is 16.42 m.

Explanation:

Given that,

Vertical diameter = 0.15 m

Rate =0.20 m³/s

Pressure = 210 kPa

Elevation = 25 m

We need to calculate the velocity

Using formula of velocity  

Q=vA

v=\dfrac{Q}{A}

Put the value into the formula

v=\dfrac{0.20}{\pi\dfrac{D^2}{4}}

v=\dfrac{0.20}{\pi\dfrac{0.15^2}{4}}

v=11.31\ m/s

Since, Q is constant, A is constant so v will be constant everywhere.

(a). We need to calculate the velocity head at elevation of 20 m

Using formula of velocity head

v'=\dfrac{v^2}{2g}

Put the value into the formula

v'=\dfrac{11.31^2}{2\times9.8}

v'=6.52\ m/s

The velocity head at elevation of 20 m is 6.52 m/s.

(b). We need to calculate pressure head at elevation of 20 m,

Using Bernoulli equation

h+\dfrac{p}{\rho g}+\dfrac{v^2}{2g}=constant

h+\dfrac{p}{\rho g}=constant

Here, velocity is constant

At h = 20 m

20+P_{H}=25+\dfrac{210\times10^{3}}{1000\times9.8}

P_{H=46.42-20

P_{H}=26.42\ m

The pressure head at elevation of 20 m is 26.42 m.

(c). We need to calculate the velocity head at elevation of 55 m,

The velocity is v'=6.52 m/s.

(d). We need to calculate the pressure head at elevation of 55 m

Using formula again

At h = 55 m

h=55+P_{H}

55+P_{H}=25+46.42

P_{H}=25-55+46.42\ m

P_{H}=16.42\ m

The pressure head at elevation of 55 m is 16.42 m.

Hence, this is the required solution.

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a) the linear density defined as the ratio between the charge per unit length

       λ = q / l

Let's start by reducing the units to the SI system

     L = 8.15 cm (1m / 100cm) = 8.15 10⁻² m

     a = 12 cm (1m / 100cm) = 12 10⁻² m

    q = -4.23 fC (1 C / 10¹⁵ ft) = -4.23 10⁻¹⁵ C

    λ = -4.23 10⁻¹⁵ C / 8.15 10⁻²

    λ = 5.19 10⁻⁴ C/m

b) Let's look for the electric field for a point at a distance a from the end of the bar

      E = k  dq / r²

To simplify the notation, suppose the bar is the x axis. Since the density is constant, we can write it differentially

     λ = dq/dx

     dq = λ dx

     E = k ∫ λ dx / x²

We integrate and evaluate between the lower limits x = a and higher x = L + a. Here we place the test point at the origin of the system

     E = k λ (-1 / x)

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     E = k λ (L /a(L + a)

Let's change the density for its value

     E = k (q / L) (L / a (L + a)

     E = k q  1 /[a(L + a)]

     E = 8.99 10⁹ 4.23 10⁻¹⁵ [1 /12 10⁻²(8.15 10⁻² + ​​12 10⁻²)]

     E = 1,573 10⁻³ N/C  

c) the direction of the field is directed to the bar, because it has a negative charge

d) now we change the distance a = 50 cm = 0.50 m

Bar

      E = 8.99 10⁹ 4.23 10⁻¹⁵ ( 1 /0.5(0.0815 +0.5))

      E = 1,308 10⁻⁴ N/C

Charge point

      q = -4.23 10⁻¹⁵ C

     E = k q / r²

     E = 8.99 10⁹ 4.23 10⁻¹⁵ / 0.5²

     E = 1.521 10⁻⁴ N/C

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