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liubo4ka [24]
2 years ago
3

One end of a light spring with spring constant k1 1,250 N/m Is attached to the celling. A second light spring Is attached to the

lower end, with spring constant k2 1,650 N/m. An object of mass 1.50 kg is attached to the lower end of the second spring.
(a) By how much does the pair of springs stretch (In m)? 9E-4 Because the springs are light, you can treat them as essentially massless, so the only downward force acting on them is mg. Use |Flkx to find the amount of stretch,x, for each spring and then find the sum. m
(b) What is the effective spring constant (in N/m) of the spring system?
Physics
1 answer:
Soloha48 [4]2 years ago
5 0

To solve this problem we will apply the concepts related to Hooke's Law for the mentioned system and Newton's second law for the description of the Weight. In turn, applying the equivalent systems of the springs we will find the constant of the equivalent spring of the whole system. To find the net displacement of the system, it will be necessary to start with point B and then return again to point A.

PART B) Let's start with the spring constant, which when connected in series (analog to a circuit for example) would be given by the function

\frac{1}{k_{eq}} = \frac{1}{k_1}+\frac{1}{k_2}

\frac{1}{k_{eq}} = \frac{k_1+k_2}{k_1k_2}

The net value would be

k_{eq}=\frac{k_1k_2}{k_1+k_2}

Therefore the equivalent constant is

k_{eq} = \frac{(1250)(1650)}{1250+1650}

k_{eq} = 711.206N/m

PART A) By equilibrium the force caused by the weight must be equivalent to the force exerted by the spring therefore

F_w = F_s

mg = K_{eq} x

Here,

m = mass

g = Acceleration due to gravity

x = Displacement

Rearranging to find the displacement,

x = \frac{mg}{K_{eq}}

x = \frac{(1.5)(9.8)}{711.206}

x = 0.020669m = 2.06cm

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statuscvo [17]

Answer:

Explanation:

Intensity of unpolarized light = I(o)

Intensity of light after first polarization by polarizer A. = I(o)/2

Angle between A and B = 120 degree.

Intensity of light after second polarization = I Cos² θ

= I(o) /2 x cos²120 = I(o) /8 .

Angle between B and C is 70 degree

Intensity of light after third polarization =

I(o)/8 x Cos² 70 = 0.1156 x I (o) /8 =

Required ratio =.01445

5 0
2 years ago
Part A At t tt = 2.0 s s , what is the particle's position? Express your answer to two significant figures and include the appro
mars1129 [50]

Complete Question

The complete question is shown on the first uploaded image

Answer:

The particle's position is  x_{2} =  10 m

The particle's velocity is  v = 2 \ m/s

Explanation:

From the question we are told that  

       x = 2m  at  t_o = 0 \ sec

        and  from the graph at t = 0  v = 6 /m

Now the acceleration which is the slope of the graph is mathematically represented as

        a = - \frac{6 - 4}{3-2}

        a = - 2 m/s^2

The negative sign shows that it is a negative slope

       Now to obtain the velocity at t = 2 sec

We use the equation of motion as follows

          v = v_o + at

  substituting values '

       v =  6 + (-2)(2)

      v = 2 \ m/s

Now to obtain the position of the particle at   v = 2 m/s

      We use the equation of motion as follows

       v^2 = v_o ^2 + 2 ax

So    2 ^2 = 6^2 + 2(-2)x

       4x = 32

       x = 8 m

From above    x = 2m  at  t_o = 0 \ sec

So the position at t =  2 s

           x_{2} =  x + x_o

          x_{2} =  2 + 8

        x_{2} =  10 m

       

 

7 0
2 years ago
What happens to the particles of a liquid when energy is removed from them?
KonstantinChe [14]

Answer:

D: The distance between the particles decreases

Explanation:

Taking away energy slows down molecules, like how you slow down when you are cold (I think)

3 0
2 years ago
You have a remote-controlled car that has been programmed to have velocity v⃗ =(−3ti^+2t2j^)m/s, where t is in s. At t = 0 s, th
DiKsa [7]

Answer:

The y-component of the car's position vector is 670m/s.

The x-component of the acceleration vector is -3, and the y-component is 40.

Explanation:

The displacement vector of the car with velocity

\boldsymbol{v}= (-3t\boldsymbol{i}+2t^2\boldsymbol{j})m/s

is the integral of the velocity.

Integrating \boldsymbol{v} we get the displacement vector \boldsymbol{d}:

\boldsymbol{d}=(-\dfrac{3}{2}t^2\boldsymbol{i}+\dfrac{2}{3}t^3\boldsymbol{j}  )

Now if the initial position if the car is

\boldsymbol{r}= (3.0\boldsymbol{i}+2.0\boldsymbol{j})

then the displacement of the car at time t is

\boldsymbol{d(t)}= \boldsymbol{r+d}

\boxed{\boldsymbol{d(t)}=(-\dfrac{3}{2}t^2+3.0\boldsymbol{i}+\dfrac{2}{3}t^3+2.0\boldsymbol{j}  )}

Now at t=10s, we have

\boxed{\boldsymbol{d(t)}=(-147\boldsymbol{i}+670\boldsymbol{j}  )}m

The y-component of the car's position vector is 670m/s.

The acceleration vector is the derivative of the velocity vector:

\boldsymbol{a(t)}=\dfrac{d\boldsymbol{v(t)}}{dt} =(-3\boldsymbol{i}+4t\boldsymbol{j})

and at t=10s it is

\boldsymbol{a(t)}=(-3\boldsymbol{i}+40\boldsymbol{j})m/s^2

The x-component of the acceleration vector is -3, and the y-component is 40.

5 0
2 years ago
Air enters the combustor of a jet engine at P1 = 10 atm, T1 = 1000oR, and M1 = 0.2. Fuel is injected and burned, with a fuel-air
GaryK [48]

Answer:

M2 = 0.06404

P2 = 2.273

T2 = 5806.45°R

Explanation:

Given that p1 = 10atm, T1 = 1000R, M1 = 0.2.

Therefore from Steam Table, Po1 = (1.028)*(10) = 10.28 atm,

To1 = (1.008)*(1000) = 1008 ºR

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F/A =???? = FA slugf/slugaq = 4.5 x 108ft-lb/slugfx FA slugf/sluga = (4.5 x 108)FA ft-lb/sluga

For the air q = cp(To2– To1)

(Exit flow – inlet flow) – choked flow is assumed For M1= 0.2

Table A.3 of steam table gives P/P* = 2.273,

T/T* = 0.2066,

To/To* = 0.1736 To* = To2= To/0.1736 = 1008/0.1736 = 5806.45 ºR Gives q = cp(To* - To) = (6006 ft-lb/sluga-ºR)*(5806.45 – 1008)ºR = 28819500 ft-lb/slugaSetting equal to equation 1 above gives 28819500 ft-lb/sluga= FA*(4.5 x 108) ft-lb/slugaFA =

F/A = 0.06404 slugf/slugaor less to prevent choked flow at the exit

3 0
2 years ago
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