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AVprozaik [17]
3 years ago
10

A car is moving 14.4 m/s when it hits the brakes. It slows for 78.8 m, which takes 9.92 s. It then accelerates at 1.83 m/s^2 for

4.50 s. What is its final velocity?
2-part motion
1-D kinematics
Physics
1 answer:
Cloud [144]3 years ago
6 0
This is a 2-part motion.
Part 1 of the motion:
Applying equations of motion;
u = 14.4 m/s, s = 78.8 m, t = 9.92 s

s = ut+1/2at^2
78.8 = 14.4*9.92 + 1/2*a*9.92^2
78.8 = 142.848 + 49.2032a
a = (78.8-142.848)/49.2032 = -1.3 m/s^2 (negative sign indicates a deceleration).
Now,
v = u+at
v = 14.4 -1.3*9.92 = 1.49 m/s

Part 2 of the motion:
Final speed in first motion becomes initial velocity in this second motion.
u = 1.49 m/s, a = 1.83 m/s^2, t = 4.50 s

Now,
v = u + at
Then,
v = 1.49 + 1.83*4.50 = 9.72 m/s

The final speed is 9.72 m/s
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A light source of wavelength λ illuminates a metal with a work function (a.k.a., binding energy) of BE=2.00 eV and ejects electr
slega [8]
<h2>Answer: 1.011 eV</h2>

Explanation:

The described situation is the photoelectric effect, which consists of the emission of electrons (electric current) that occurs when light falls on a metal surface under certain conditions.  

If we consider the light as a stream of photons and each of them has energy, this energy is able to pull an electron out of the crystalline lattice of the metal and communicate, in addition, a <u>kinetic energy. </u>

This is what Einstein proposed:  

Light behaves like a stream of particles called photons with an energy  E:

E=h.f (1)  

So, the energy E of the incident photon must be equal to the sum of the Work function \Phi of the metal and the kinetic energy K of the photoelectron:  

E=\Phi+K (2)  

Where \Phi is the <u>minimum amount of energy required to induce the photoemission of electrons from the surface of a metal, and </u><u>its value depends on the metal.  </u>

In this case \Phi=2eV  and K_{1}=4eV

So, for the first light source of wavelength \lambda_{1}, and  applying equation (2) we have:

E_{1}=2eV+4eV   (3)  

E_{1}=6eV   (4)  

Now, substituting (1) in (4):  

h.f=6eV (5)  

Where:  

h=4.136(10)^{-15}eV.s is the Planck constant

f is the frequency  

Now, the <u>frequency has an inverse relation with the wavelength </u>

\lambda_{1}:  

f=\frac{c}{\lambda_{1}} (6)  

Where c=3(10)^{8}m/s is the speed of light in vacuum  

Substituting (6) in (5):  

\frac{hc}{\lambda_{1}}=6eV (7)  

Then finding \lambda_{1}:  

\lambda_{1}=\frac{hc}{6eV } (8)  

\lambda_{1}=\frac{(4.136(10)^{-15} eV.s)(3(10)^{8}m/s)}{6eV}  

We obtain the wavelength of the first light suorce \lambda_{1}:  

\lambda_{1}=2.06(10)^{-7}m   (9)

Now, we are told the second light source \lambda_{2}  has the double the wavelength of the first:

\lambda_{2}=2\lambda_{1}=(2)(2.06(10)^{-7}m)   (10)

Then: \lambda_{2}=4.12(10)^{-7}m   (11)

Knowing this value we can find E_{2}:

E_{2}=\frac{hc}{\lambda_{2}}   (12)

E_{2}=\frac{(4.136(10)^{-15} eV.s)(3(10)^{8}m/s)}{4.12(10)^{-7}m}   (12)

E_{2}=3.011eV   (13)

Knowing the value of E_{2} and \lambda_{2}, and knowing we are working with the same work function, we can finally find the maximum kinetic energy K_{2} for this wavelength:

E_{2}=\Phi+K_{2} (14)  

K_{2}=E_{2}-\Phi (15)  

K_{2}=3.011eV-2eV  

K_{2}=1.011 eV  This is the maximum kinetic energy for the second light source

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3 years ago
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