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Semenov [28]
2 years ago
14

The G string on a guitar is 69 cm long and has a fundamental frequency of 196 Hz. A guitarist can play different notes by pushin

g the string against various frets, which changes the string's length. The third fret from the neck gives B♭ (233.08 Hz); the fourth fret gives B (246.94 Hz).
How far apart are the third and fourth frets?

Express your answer to two significant figures and include the appropriate units.
Physics
1 answer:
Readme [11.4K]2 years ago
6 0

Answer:

 Δd = 23 cm

Explanation:

When the eta string on the guitar has nodes at its ends, so the waves produced give rise to a standing wave, which can be described by the following expressions

Fundamental      L = ½ λ

1st harmonic       L = 2 ( λ / 2)

2nd harmonic     L = 3 ( λ / 2)

Harmonic n         L = n  λ / 2

Where n is an integer

                     

The speed of the rope is given by the ratio

         v =  λ f

This speed is constant since it depends on the tension and the linear density of the rope

Let's calculate the speed with the initial data

           v = 0.69  196

           v = 135.24 m / s

Let's look for the wavelength for the two frequencies

           λ₁ = v / f₁

           λ₁ = 135.24 / 233.08

           λ₁ = 0.58022 m

           λ₂ = v / f₂

           λ₂ = 135.24 / 246.94

            λ₂ = 0.54766 m

Let's replace in the resonance equation

             Lₙ = n  λ/2

For the third fret

            m = 3

            L₃ = 3 0.58022 / 2

            L₃ = 0.87033 m

For the fourth fret

            m = 4

            L₄ = 4 0.54766 / 2

            L₄ = 1.09532 m

The distance between the two frets is

         Δd = L₄ –L₃

         Δd = 1.09532 - 0.87033

         Δd = 0.22499 m

         Δd = 22.5 cm = 23 cm

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klemol [59]
Let A = i+j+k be a vector and B = 3 be any scalar, 
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Which is a new vector whose direction is same as the old but it's 3 times greater in length  than the old vector(i+j+k).

Now, dividing A and B,
A/B = (i+j+k)/3 = \frac{1}{3}i +  \frac{1}{3}j + \frac{1}{3}k

Which is again a new vector whose direction is same as the old but now it's 1/3 times small in length than the old vector. 

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8 0
2 years ago
Read 2 more answers
A 0.110 kg cube of ice (frozen water) is floating in glycerine. The glycerine is in a tall cylinder that has inside radius 3.70
Sonbull [250]

Answer:

the distance by which the height of the  liquid in the cylinder change after the ice gets melted = 0.528 cm

Explanation:

The change in volume of glycerin when the ice cube is placed on the surface of the glycerin can be represented as:

V = \frac{m}{ \rho}

Given that ;

the mass of the ice cube (m) = 0.11 kg = 0.110 × 10³ g

density of the glycerine (\rho) = 1.260 kg/L = 1.260 g/cm³

Then:

V = \frac{0.110*10^3 \ g}{1.260 \ g/cm^3}

V = 0.0873*10^3 \ cm^3 (\frac{1L}{10^3 cm^3})

V = 0.0873 L

Now;Initially the volume of the glycerin before the ice cube starts to melt is:

V_1 = V_i + V\\\\V_1 = V_i+ 0.0873 \ L

However; the volume of the water produced by the 0.11 kg ice cube = 0.11*10^3 \ cm^3

The expression for change in the volume of glycerin after the ice cube starts to melt is as follows:

V_2 = V_i + V"

replacing V" with 0.11*10^3 \ cm^3 ; we have:

V_2 = V_i (0.11*10^3 \ cm^3 )(\frac{1 \ L }{10^3 \ cm^3})

V_2 = V_i + 0.11 \ L

The overall total change in the volume of the glycerin is illustrated as:

V_f = V_2 - V_1

Now; from the foregoing ; lets replace the respective value of V_2 and V_1 in the above equation ; we have;

V_f = (V_i + 0.11 \ L) - (V_i + \ 00873 \ L)\\ \\V_f = 0.11 L - 0.0873 \ L\\\\V_f = 0.0227 \ L

The formula usually known to be the volume of a cylinder is :

V = \pi r ^2 h

For the question ; we will have:

V_f = \pi r ^2 h

making h the subject of the  formula ; we have:

h = \frac{V_f}{\pi r^2}

replacing 0.0227 L for V_fand the given value of radius which is = 3.70 cm; we have:

h = \frac{0.0227 \ L ( \frac{10^3 \ cm^3}{1\ L})}{\pi * (3.70 cm)^2}

h = \frac{22.7 \ cm^3}{\pi * (3.70 cm)^2}\\\\h = 0.528 \ \ cm

Thus ; the distance by which the height of the  liquid in the cylinder change after the ice gets melted = 0.528 cm

8 0
2 years ago
A student bikes to school by traveling first dN = 1.00 miles north, then dW = 0.600 miles west, and finally dS = 0.200 miles sou
kompoz [17]
Refer to the diagram shown below.

Define unit vectors along the x and y axes as respectively \hat{i} \, and \, \hat{j}.

Then the three successive displacements, written in component form, are respectively
\vec{dN} = 1.0 \, \hat{j} \\
\vec{dW} = -0.6 \, \hat{i} \\  \vec{dS} = -0.2 \, \hat{j}

The total displacement for the first leg of the trip is
\vec{d} = \vec{dN} + \vec{dW} + \vec{dS} \\ \vec{d}= 1.0\hat{j}-0.6\hat{i}-0.2\hat{j} \\ \vec{d}=-0.6\hat{i}+0.8\hat{j}

Answer:
\vec{d} = -0.6\hat{i}+0.8\hat{j}   or  (-0.6, 0.8)


6 0
2 years ago
You are using a hydrogen discharge tube and high quality red and blue light filters as the light source for a Michelson interfer
boyakko [2]

Answer:

final displacement = +24484.5 nm

Explanation:

The path difference when 158 bright spots were observed with red light (λ1 = 656.3 nm) is given as;

Δr = 2d2 - 2d1 = 150λ1

So, 2d2 - 2d1 = 150λ1

Dividing both sides by 2 to get;

d2 - d1 = 75λ1 - - - - eq1

Where;

d1 = distance between the fixed mirror and the beam splitter

d2 = position of moveable mirror from splitter when 158 bright spots are observed

Now, the path difference between the two waves when 114 bright spots were observed is;

Δr = 2d'2 - 2d1 = 114λ1

2d'2 - 2d1 = 114λ1

Divide both sides by 2 to get;

d'2 - d1 = 57λ1

Where;

d'2 is the new position of the movable mirror from the splitter

Now, the displacement of the moveable mirror is (d2 - d'2). To get this, we will subtract eq2 from eq1.

(d2 - d1) - (d'2 - d1) = 75λ1 - 57λ2

d2 - d1 - d'2 + d1 = 75λ1 - 57λ2

d2 - d'2 = 75λ1 - 57λ2

We are given;

(λ1 = 656.3 nm) and λ2 = 434.0 nm.

Thus;

d2 - d'2 = 75(656.3) - 57(434)

d2 - d'2 = +24484.5 nm

5 0
2 years ago
Two uniform, solid cylinders of radius R and total mass M are connected along their common axis by a short, light rod and rest o
sveta [45]

Explanation:

A) To prove the motion of the center of mass of the cylinders is simple harmonic:

System diagram for given situation is shown in attached Fig. 1

We can prove the motion of the center of mass of the cylinders is simple harmonic if

a_{x} = -\omega^{2}  x

where aₓ is acceleration when attached cylinders move in horizontal direction:

<h3>PROOF:</h3>

rotational inertia for cylinders  is given as:

                                  I=\frac{1}{2}MR^{2} -----(1)

Newton's second law for angular motion is:

                                             ∑τ = Iα ------(2)

For linear motion in horizontal direction it is:

                                             ∑Fₓ = Maₓ ------ (3)

By definition of torque:

                                               τ  = RF --------(4)        

Put (4) and (1) in (2)

                                       RF=\frac{1}{2}MR^{2}\alpha

                                       RF=\frac{1}{2}MR^{2}\alpha

from Fig 3 it can be seen that fs is force by which the cylinders roll without slipping as they oscillate

So above equation becomes

                                   f_{s}=\frac{1}{2}MR\alpha------ (5)

As angular acceleration is related to linear by:

                                          a= R\alpha

Eq (5) becomes

                                    f_{s}=\frac{1}{2}Ma_{x}---- (6)

aₓ shows displacement in horizontal direction

From (3)

                                              ∑Fₓ = Maₓ

Fₓ is sum of fs and restoring force that spring exerts:

                                  \sum F_{x} = f_{s} - kx ----(7)

Put (7) in (3)

                                  f_{s} - kx  = Ma_{x}[/tex] -----(8)

Using (6) in (8)

                               \frac{1}{2}Ma_{x} - kx =Ma_{x}

                                     a_{x} = \frac{2k}{3M} x --- (9)

For spring mass system

                                  a= -\omega^{2} x ----- (10)

Equating (9) and (10)

                                  \omega^{2} = \frac{2k}{3M}

\omega = \sqrt{ \frac{2k}{3M}}

then (9) becomes

                                a_{x} = - \omega^{2}x

(The minus sign says that x and  aₓ  have opposite directions as shown in fig 3)

This proves that the motion of the center of mass of the cylinders is simple harmonic.

<h3 /><h3>B) Time Period</h3>

Time period is related to angular frequency as:

                                   T=\frac{2\pi }{\omega}

                                  T = 2\pi \sqrt{\frac{3M}{2k}

                           

 

5 0
2 years ago
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