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s344n2d4d5 [400]
3 years ago
11

Ablok slides on ahorizonted sur fors which has been lubricated with heavy oil such that the blok soffers a viscous resistance th

at vories as the square root of the speed f(v)=-cv^1/2 if the initial speed of the blok is v° at time t=0 find the volues of (v) and (x) as afanctions of the time (t)
Physics
1 answer:
svetoff [14.1K]3 years ago
7 0

Answer:

v = (v_0^{\frac{3}{2}}-\frac{3cx}{2m})^\frac{2}{3}

x = \frac{2m}{c}*v_0^{\frac{3}{2}}

Explanation:

Given

f(v) =- cv^\frac{1}{2}

To start with, we begin with

F = ma

Substitute the expression for F

-cv^\frac{1}{2} = ma

-ma = cv^\frac{1}{2}

Acceleration (a) is:

a = \frac{dv}{dt}

So, the expression becomes:

m\frac{dv}{dt} = -cv^\frac{1}{2}

-----------------------------------------------------------------------------------------

Velocity (v) is:

v = \frac{dx}{dt} --- distance/time

v * \frac{dv}{dx}= \frac{dx}{dt}* \frac{dv}{dx}

v * \frac{dv}{dx}= \frac{dv}{dt}

\frac{dv}{dt} = v * \frac{dv}{dx}

--------------------------------------------------------------------------------------------

So, we have:

m\frac{dv}{dt} = -cv^\frac{1}{2}

mv * \frac{dv}{dx} = -cv^\frac{1}{2}

Divide both sides by v^\frac{1}{2}

mv^{1-\frac{1}{2}} * \frac{dv}{dx} = -c

mv^{\frac{1}{2}} * \frac{dv}{dx} = -c

Divide both sides by m

v^{\frac{1}{2}} * \frac{dv}{dx} = -\frac{c}{m}

v^{\frac{1}{2}} * dv = -\frac{c}{m} * dx

Integrate:

\int\limits^v_{v_0} {v^{\frac{1}{2}}} \, dv  = -\frac{c}{m}\int\limits^x_0 {}} \, dx

\frac{2}{3}v^{\frac{3}{2}}|\limits^v_{v_0}  = -\frac{c}{m}x|\limits^x_0

\frac{2}{3}(v^{\frac{3}{2}} - v_0^{\frac{3}{2}} ) = -\frac{cx}{m}

v^{\frac{3}{2}} - v_0^{\frac{3}{2}} = -\frac{3cx}{2m}

v^{\frac{3}{2}} = v_0^{\frac{3}{2}}-\frac{3cx}{2m}

v = (v_0^{\frac{3}{2}}-\frac{3cx}{2m})^\frac{2}{3}

Next, is to get the maximum velocity by distance x.

To do this, we find the derivation by x

\frac{dv}{dx} = 0

\frac{2}{3}(v_0^{\frac{3}{2}}-\frac{3cx}{2m})^{\frac{2}{3} - 1} * -\frac{3c}{2m} = 0

\frac{2}{3}(v_0^{\frac{3}{2}}-\frac{3cx}{2m})^{\frac{2-3}{3}} * -\frac{3c}{2m} = 0

\frac{2}{3}(v_0^{\frac{3}{2}}-\frac{3cx}{2m})^{\frac{-1}{3}} * -\frac{3c}{2m} = 0

(v_0^{\frac{3}{2}}-\frac{3cx}{2m})^{\frac{-1}{3}} * -\frac{c}{m} = 0

Divide both sides by -\frac{c}{m}

(v_0^{\frac{3}{2}}-\frac{3cx}{2m})^{\frac{-1}{3}} = 0

Take cube roots of both sides

(v_0^{\frac{3}{2}}-\frac{3cx}{2m})^{-1} = 0

v_0^{\frac{3}{2}}-\frac{3cx}{2m} = 0

\frac{3cx}{2m} = v_0^{\frac{3}{2}}

x = \frac{2m}{c}*v_0^{\frac{3}{2}}

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A 2.20-kg object is attached to a spring and placed on frictionless, horizontal surface. A horizontal force of 29.0 N is require
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Answer:

a. 145 N/m b. 1.29 Hz c. 1.62 m/s d.  0 m e. 13.2 m/s² f. ± 0.2 m g. 2.9 J h. 0.54 m/s i. 4.39 m/s²

Explanation:

a. The force constant of the spring

The spring force F = kx and k = F/x where k is the spring constant. F = 29.0 N and x = 0.200 m

k = 29.0 N/0.200 m = 145 N/m

b. The frequency of oscillations, f

f = 1/2π√(k/m)    m = mass = 2.20 kg

f = 1/2π√(145 N/m/2.20 kg) = 1.29 Hz

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The maximum elastic potential energy of the spring = maximum kinetic  energy of the object

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v = (√k/m)x where v is the maximum speed of the object

v = (√145/2.2)0.2 = 1.62 m/s

d Where does the maximum speed occur?

The maximum speed occurs at  0 m

e. The maximum acceleration

a = kx/m = 145 × 0.2/2.2 = 13.2 m/s²

f. The maximum acceleration occurs at x = ± 0.2 m

g. The total energy of the system is the maximum elestic potential energy of the system

E = 1/2kx² = 1/2 × 145 × 0.2² = 2.9 J

h. When x = x₀/3

1/2k(x₀/3)² = 1/2mv²

kx₀²/9 = mv²

v = 1/3(√k/m)x₀ = 1/3(√145/2.2)0.2 = 0.54 m/s

i When x = x₀/3

a = kx₀/3m =  145 × 0.2/(2.2 × 3)= 4.39 m/s²

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An Olympic discus thrower (~100 kg) launches the 2.0 kg discus by spinning rapidly (~4 times per second) with arm outstretched (
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Answer:

F = 1263.03 N

Explanation:s

given,                      

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mass of the disk = 2 Kg                

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ω = 4 x 2 x π        

ω = 25.13 rad/s

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F = 2 x 25.13² x 1

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Answer:

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