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Phantasy [73]
4 years ago
10

One end of a horizontal rope is attached to a prong of anelectrically driven tuning fork that vibrates at 120 Hz. The otherend p

asses over a pulley and supports a 1.70 kg mass. The linear mass density of the rope is0.0590 kg/m.(a) What is the speed of a transverse wave onthe rope?v1.70 kg =1 m/s(b) What is the wavelength?λ1.70 kg =2 m(c) How would your answers to parts (a) and (b) be changed if themass were increased to 2.80 kg?v2.80 kg = 3v1.70 kgλ2.80kg = 4λ1.70 kg
Physics
1 answer:
Elenna [48]4 years ago
7 0

Answer:

(a) v=16.804\ m.s^{-1}

(b) \lambda=1.4875\ cm

(c)

  • F_T=27.44\ N
  • v=21.57\ m.s^{-1}

and

  • \lambda=17.97\ cm

Explanation:

Given:

  • frequency of vibration, f=120\ Hz
  • mass of object attached to the rope, m=1.7\ kg
  • linear mass density of rope, \mu=0.059\ kg.m^{-1}

(a)

<u>We have the expression for velocity as:</u>

v=\sqrt{\frac{F_T}{\mu} } .................(1)

where:

F_T= tension force in the rope

<em>Now for tension force we balance the forces acting on the rope:</em>

T=m.g

T=1.7\times 9.8

T=16.66\ N

<u>Now using eq. (1)</u>

v=\sqrt{\frac{16.66}{0.059} }

v=16.804\ m.s^{-1}

(b)

<u>Wavelength is given by:</u>

\lambda=\frac{v}{f}

\lambda=\frac{16.66}{120}

\lambda=1.4875\ cm

(c)

  • On increasing the mass to 2.8 kg

<u>We get :</u>

F_T=27.44\ N

v=21.57\ m.s^{-1}

and

\lambda=17.97\ cm

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A thin, uniformly charged insulating rod has a linear charge density λ = 3 nC/m and lies along the x axis from x = 1m to x = 3m.
Contact [7]

Answer:

A) V_A = 11.93~V

B) The vector definition of E-field is

\vec{E} = -1.13\^x + 2.41\^y

where magnitude is E = 2.66 N/m.

Explanation:

The potential of a uniformly charged rod can be found by the method of integration. We will first choose an infinitesimal part on the rod. We will compute the potential of this part at point A. Then we will integrate this potential over the entire rod.

We will use the following formula for electric potential:

V = \frac{1}{4\pi \epsilon_0}\frac{Q}{r}

Let us choose the infinitesimal part a distance 'x' from the origin. Then the distance between this point and point A is

r = \sqrt{x^2+4^2}

The infinitesimal length is 'dx', and the potential of this length is dV. Let's apply the formula:

dV = \frac{1}{4\pi\epsilon_0}\frac{\lambda dx}{\sqrt{x^2 + 4^2}}

Here, the charge Q is equal to the charge density multiplied by the length. Q = λdx

Now we have to integrate this infinitesimal potential over the rod:

V = \int\limits^3_1 {dV} \, dx = \frac{1}{4\pi \epsilon_0}\int\limits^3_1 {\frac{\lambda}{\sqrt{x^2 + 16}} \, dx

By using an integral table, this can be calculated:

V = \frac{3\times 10^{-9}}{4\pi\epsilon_0}\ln(|\sqrt{x^2+16}+x|)\left \{ {{x=3} \atop {x=1}} \right. \\V = 11.93~V

B) The electric field can be found by a similar approach, but a different formula:

\vec{E} = \frac{1}{4\pi \epsilon_0}\frac{Q}{r^2}\^r

Let's apply this formula to the infinitesimal part we have chosen.

dE_x = \frac{1}{4\pi\epsilon_0}\frac{\lambda dx}{x^2 + 4^2}\cos(\theta)\\dE_y = \frac{1}{4\pi\epsilon_0}\frac{\lambda dx}{x^2 + 4^2}\sin(\theta)

By the geometry sine and cosine terms can be found:

\sin(\theta) = \frac{4}{\sqrt{x^2+16}}\\\cos(\theta) = \frac{x}{\sqrt{x^2 + 16}}

The x- and y-components of the E-field can be found separately by integrating the infinitesimal parts over the entire rod.

E_x = \int\limits^3_1 {dE_x} \, dx = \frac{\lambda}{4\pi\epsilon_0}\int\limits^3_1 {\frac{x}{(x^2+16)^{3/2}}} \, dx  = 1.13(-\^x)\\E_y = \int\limits^3_1 {dE_y} \, dx = \frac{4\lambda}{4\pi\epsilon_0}\int\limits^3_1 {\frac{1}{(x^2+16)^{3/2}}} \, dx  = 2.41(\^y)

So, the final E-field is

\vec{E} = -1.13\^x + 2.41\^y

The magnitude of the E-field is

E = 2.66 N/m

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A heat engine has a maximum possible efficiency of 0.780. If it operates between a deep lake with a constant temperature of-24.8
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Answer : The temperature of the hot reservoir (in Kelvins) is 1128.18 K

Explanation :

Efficiency of carnot heat engine : It is the ratio of work done by the system to the system to the amount of heat transferred to the system at the higher temperature.

Formula used for efficiency of the heat engine.

\eta =1-\frac{T_c}{T_h}

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T_h = Temperature of hot reservoir = ?

T_c = Temperature of cold reservoir = -24.8^oC=273+(-24.8)=248.2K

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