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gtnhenbr [62]
2 years ago
7

The train is accelerated from rest at a speed of 0.11 m/s2 to reach a speed of 15.6 m/s. After reaching that speed the train mov

es at a constant speed for the rest of its journey. How far does the train travel after 5 minutes and the average speed entering the 5 minute time interval.
Physics
1 answer:
9966 [12]2 years ago
7 0

Answer:

cliff

Explanation:

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A 12 cm diameter piston-cylinder device contains air at a pressure of 100 kPa at 24oC. The piston is initially 20 cm from the ba
lina2011 [118]

Answer:

ΔQ = 0.1 kJ

\mathbf{v_f = 1.445*10^{-3}  m^3}

\mathbf{P_f = 156.5 \ kPa}

ΔS = -0.337 J/K

The value negative is due to the fact that there is need to be the same amount of positive change in surrounding as a result of compression.

Explanation:

GIven that:

Diameter of the piston-cylinder = 12 cm

Pressure of the piston-cylinder = 100 kPa

Temperature =24 °C

Length of the piston = 20 cm

Boundary work ΔW = 0.1 kJ

The gas is compressed and The temperature of the gas remains constant during this process.

We are to find ;

a. How much heat was transferred to/from the gas?

According to the first law of thermodynamics ;

ΔQ = ΔU + ΔW

Given that the temperature of the gas remains constant during this process; the isothermal process at this condition ΔU = 0.

Now

ΔQ = ΔU + ΔW

ΔQ = 0 + 0.1 kJ

ΔQ = 0.1 kJ

Thus; the amount of heat that was transferred to/from the gas is : 0.1 kJ

b. What is the final volume and pressure in the cylinder?

In an isothermal process;

Workdone W = \int dW

W = \int pdV \\ \\ \\W = \int \dfrac{nRT}{V}dv \\ \\ \\ W = nRt \int  \dfrac{dv}{V}  \\ \\ \\ W  = nRT In V |^{V_f} __{V_i}}  \\ \\ \\ W = nRT \ In \dfrac{V_f}{V_i}

Since the gas is compressed ; then v_f< v_i

However;

W =- nRT \ In \dfrac{V_f}{V_i}

W =- P_1V_1  \ In \dfrac{V_f}{V_i}

The initial volume for the cylinder is calculated as ;

v_1 = \pi r^2 h \\ \\   v_1 = \pi r^2 L \\ \\ v_1 = 3.14*(6*10^{-2})^2*(20*10^{-2}) \\ \\ v_1 = 2.261*10^{-3} \ m^3

Replacing over values into the above equation; we have :

100 =  - ( 100*10^3 *2.261*10^{_3}) In (\dfrac{v_f}{v_i}) \\ \\ - In (\dfrac{v_f}{v_i})= \dfrac{100}{(100*10^3*2.261*10^{-3})} \\ \\ - In \ v_f  + In \  v_i = \dfrac{100}{226.1} \\ \\   - In \ v_f  = - In \ v_i + \dfrac{100}{226.1}  \\ \\  - In \ v_f  = - In (2.261*10^{-3} + \dfrac{100}{226.1 } \\ \\  - In \ v_f  = 6.1 + 0.44 \\ \\  - In \ v_f  = 6.54 \\ \\  - In \ v_f  = -6.54 \\ \\ v_f = e^{-6.54} \\ \\ \mathbf{v_f = 1.445*10^{-3}  m^3}

The final pressure can be calculated by using :

P_1V_1 = P_2V_2 \\ \\ P_iV_i = P_fV_f

P_f =\dfrac{P_iV_i}{V_f}

P_f =\dfrac{100*2.261*10^{-3}}{1.445*10^{-3}}

P_f = 1.565*10^2 \ kPa

\mathbf{P_f = 156.5 \ kPa}

c. Find the change in entropy of the gas. Why is this value negative if entropy always increases in actual processes?

The change in entropy of the gas is given  by the formula:

\Delta S=\dfrac{\Delta Q}{T}

where

T =  24 °C = (24+273)K

T = 297 K

\Delta S=\dfrac{-100 \ J}{297 \ K}

ΔS = -0.337 J/K

The value negative is due to the fact that there is need to be the same amount of positive change in surrounding as a result of compression.

4 0
3 years ago
A monochromatic light of wavelength 506 nm from a distant source is incident on a single slit 0.075 mm wide. Diffraction pattern
sladkih [1.3K]

Answer:

first minimum distance from the center = 0.417 m m

Explanation:

given,

wavelength (λ) = 506 nm

d = 0.075 mm  = 0.000075 m

tanθ = x /2

d sinθ = m λ

m=1 ( 1 st minimum  )  

0.000075 × sin θ = 506 × 10⁻⁹

sin θ =\dfrac{506 × 10⁻⁹}{0.000075}

sin θ = 0.00675

θ = sin⁻¹(0.00675)

θ = 0.00675

x =  0.000417 m

hence, the first minimum distance from the center = 0.417 m m

5 0
3 years ago
Why is the law of gravity an example of a universal law
ella [17]
Its an example of a universal law because gravity occurs in every place of the world 
Hoped I helped!!!!!
8 0
3 years ago
A VHF television station assigned to channel 4 transmits its signal using radio waves with a frequency of 66.0 MHz. Calculate th
soldi70 [24.7K]

Answer:

The wavelength is 4.55 m.

Explanation:

Given data

  • Frequency (ν): 66.0 MHz = 66.0 × 10⁶ Hz = 66.0 × 10⁶ s⁻¹
  • Speed of light (c): 3.00 × 10⁸ m/s
  • Wavelength (λ): To be found

We can determine the wavelength of the radio waves using the following expression.

c = λ × ν

λ = c / ν

λ = (3.00 × 10⁸ m/s)/66.0 × 10⁶ s⁻¹

λ = 4.55 m

6 0
3 years ago
With full explaniation
zzz [600]

A. The ball's (vertical) velocity v at time t is

v(t) = 30\dfrac{\rm m}{\rm s} - gt

so that after 4 seconds, the ball's speed is

|v(4\,\mathrm s)| = \left|30\dfrac{\rm m}{\rm s} - \left(10\dfrac{\rm m}{\mathrm s^2}\right) (4\,\mathrm s)\right| = \boxed{10\frac{\rm m}{\rm s}}

(The velocity is -10 m/s, so the ball is falling back down at this point.)

B. At maximum height, the ball has zero velocity, so it takes

30\dfrac{\rm m}{\rm s} - gt = 0 \implies t = \dfrac{30\frac{\rm m}{\rm s}}g = \boxed{3\,\mathrm s}

for the ball to reach this height.

C. The height of the ball y at time t is

y(t) = \left(30\dfrac{\rm m}{\rm s}\right) t - \dfrac g2 t^2

The maximum height is attained by the ball at 3 seconds after it's thrown, so

y_{\rm max} = \left(30\dfrac{\rm m}{\rm s}\right) (3\,\mathrm s) - \dfrac{10\frac{\rm m}{\mathrm s^2}}2 (3\,\mathrm s)^2 = \boxed{45\,\mathrm m}

D. The time it takes for the ball to reach its maximum height is half the time it spends in the air. So the total airtime is \boxed{6\,\mathrm s}.

Put another way: When the ball returns to the height from which it was thrown, its final velocity has the same magnitude as its initial velocity but points in the opposite direction. This is to say, after the total time the ball is in the air, it's final velocity will be -30 m/s. Then the total airtime is

30\dfrac{\rm m}{\rm s} - gt = -30\dfrac{\rm m}{\rm s} \implies t = \dfrac{60\frac{\rm m}{\rm s}}g = \boxed{6\,\mathrm s}

Put yet another way: Solve y(t) = 0 for t. I don't see a need to elaborate...

5 0
2 years ago
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