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jonny [76]
4 years ago
10

The coefficient of static friction between car's tires and a level road is 0.80 If car to be stopped in time of 3.0 sec its spee

d is
Physics
1 answer:
Vlad1618 [11]4 years ago
4 0

Answer:

23.5 m/s

Explanation:

The velocity of the car in decelerated motion is given by

v = u + at

where

v = 0 is the final velocity

u is the initial velocity

a is the acceleration of the car

t = 3.0 s is the time it takes for the car to stop

The acceleration of the car is given by the frictional force, which is the only force acting on the car along the direction of motion, so:

ma = -\mu mg\\a = -\mu g = -(0.80)(9.8 m/s^2)=-7.84 m/s^2

where

\mu=0.80 is the coefficient of friction

Solving the previous equation for u, we find the initial velocity:

u=v-at=0-(-7.84 m/s^2)(3.0 s)=23.5 m/s

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Answer:

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Explanation:

To solve this problem we apply the following formulas:

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d= piston diameter

Nomenclature:

Fp= Force on the primary piston

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As= Secondary piston area

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Calculation of the force Fp necessary to support the weight of the car.

Pascal principle: Fp=P*Ap (Equation1)

In (Equation1) we know Ap and we don't know P.

Pressure calculation:

We apply Newton's first law for a balanced Secondary piston -automobile system

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P=\frac{W}{As}

We replace P=\frac{W}{As}in equation 1:

Fp=\frac{W}{As} *Ap

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Fp=W*\frac{d_{p}^{2}  }{d_{s}^{2}  }

Fp=2200*\frac{2,1^{2} }{26^{2} }

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1kg=9.8N

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Fp=140.63N

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Answer:

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Explanation:

Given;

number of moles of gas, n = 6.35 moles

temperature of the gas, T = 320 K

initial volume of the gas, V₁ = 1.45 L

final volume of the gas, V₂ = 3.95 L

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Therefore, change in the internal energy of the gas is zero since the gas expanded isothermally (constant temperature).

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Part (c)

the heat flow into or out of the gas

Q = ΔU + W

Q = 0 + 16.93 kJ

Q = 16.93 kJ

Since the heat flow is positive, then it is heat flow into the gas.

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Answer:

if no external force is acting on it so it will remain in motion acoording to inertia ( inertia is a property of matter it continues in existing state either in rest or motion

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