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brilliants [131]
3 years ago
10

Derivation of Eq. (3): o Basic physics principles: Justify equations (1) and (2) in your own words. . Doing the algebra: From eq

uations (1) and (2), show that equation (3) holds. mu? =eu B This would be nice if we knew the velocity. Fortunately, we know the voltage through which the electrons are accelerated. Setting the change in electrical potential energy equal to the final kinetic energy of the electrons, we find: eV = From this point, some algebra lets us eliminate the velocity variable entirely, giving us: e 2V m (B_T)
Physics
1 answer:
zysi [14]3 years ago
7 0

Answer:

About eq (1)

mv^2/r = eVB

when a charged particle (electron) enters into the magnetic field which is perpendicular to direction of motion than there will be magnetic force on particle and particle will travel in circular path in with constant speed.

So using force balance on charged particle:

F_{net} = Fc - Fm

Since particle is traveling at constant speed, So acceleration is zero, and

F_{net} = 0

Fc - Fm=0

Fc = Fm

Fc = centripetal force on particle = m*v^2/r

Fm = magnetic force on electron = q*VxB = q*V*B*sin \theta

q = charge on electron = e

since magnetic field is perpendicular to the velocity of particle, So theta = 90 deg

sin 90 deg = 1

So,

m*v^2/r = e*v*B

About equation 2:

When this charged particle is released from rest in a potential difference V, and then it enters into above magnetic field, then using energy conservation on charge particle

KEi + PEi = KEf + PEf

KEi = 0, since charged particle started from rest

PEi - PEf = q*dV

PEi - PEf = eV

KEf = final kinetic energy of particle when it leaves = (1/2)*m*v^2

So,

0 + eV = (1/2)*m*v^2

eV = (1/2)*m*v^2

From above equation (1) and (2)

m*v^2/r = evB

e/m = v/(r*B)

Now

eV = (1/2)*m*v^2

v = \sqrt{(2*e*V/m)}

e/m = \sqrt{ (2*e*V/m)/(r*B)}

\frac{e^2}{m^2} = \frac{2*e*V}{(m*r^2*B^2)}

e/m = 2*V/(r^2*B^2)

e/m = 2V/(Br)^2

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Gnoma [55]

Length of the pipe = 0.39 m

Third harmonic frequency = 1400 Hz

For the third harmonic:

Wavelength = \frac{2L}{3}

The center of the open pipe will host a node and the nearest anti - node from the center will be at the 0.25 × wavelength

Distance from center  = 0.25 × wavelength

Distance = 0.25 x \frac{2L}{3}

Plugging the value of the length of the pipe (L) = 0.39 m = 39 cm

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A sinusoidal wave traveling on a string has a period of 0.20 s, a wavelength of 32 cm, and an amplitude of 3 cm. The speed of th
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Answer:

v = 1.6 \frac{m}{s} *\frac{100cm}{1m}= 160 \frac{cm}{s}

Explanation:

If we have a periodic wave we need to satisfy the following basic relationship:

v = \lambda f

From the last formula we see that the velocity is proportional fo the frequency.

For this case we have the following info given by the problem:

T= 0.2 s, \lambda =32 cm* \frac{1m}{100cm} =0.32 m, A= 3cm*\frac{1m}{100 cm}=0.03 m

We know that the frequency is the reciprocal of the period so we have this formula:

f = \frac{1}{T}

And if we replace we got:

f =\frac{1}{0.2 s}= 5Hz

Now since we have the value for the wavelength we can find the velocity like this:

v = 0.32 m * 5Hz = 1.6 \frac{m}{s}

And if we convert this into cm/s we got:

v = 1.6 \frac{m}{s} *\frac{100cm}{1m}= 160 \frac{cm}{s}

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lozanna [386]

Answer:

a=-5.67\ m/s^2

Explanation:

Given that,

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Time, t = 3s

We need to find the acceleration of the car. The formula of it is given by :

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