Question #51858

An observer can describe the motion of an object as "translational" if
the axes of the reference frame imagined to be attached to the object
x′
,
y′
and
z′
always remain parallel to the axes of his own reference frame
x
,
y
and
z
the object moves in a curved path in such a way that
x′
,
y′
and
z′
may rotate about their origin
O′
the motion of the object may not be represented by the motion of its centre of mass
all the constituent particles of the object undergo different displacements at the same time
1

Expert's answer

2015-04-16T03:07:50-0400

Answer on Question 51848, Physics, Other

18. A ray of light travels from air to glass. The incident ray makes an angle 4545{}^{\circ} while the refracted ray makes an angle of 3030{}^{\circ} with the normal to the interface. The speed of light in air is 3.0108m/s3.0 \cdot 10^{8} \, \text{m/s}. What is the speed of light in glass?

a) 2.12108m/s2.12 \cdot 10^{8} \, \text{m/s}

b) 4.24108m/s4.24 \cdot 10^{8} \, \text{m/s}

c) 3.73108m/s3.73 \cdot 10^{8} \, \text{m/s}

d) 3.0108m/s3.0 \cdot 10^{8} \, \text{m/s}

Solution:

From the Snell’s law we have:


sinθ1sinθ2=n2n1=v1v2,\frac{\sin \theta_1}{\sin \theta_2} = \frac{n_2}{n_1} = \frac{v_1}{v_2},


where, θ1=45\theta_1 = 45{}^{\circ} is the angle of incidence, θ2=30\theta_2 = 30{}^{\circ} is the angle of refraction, v1v_1 is the speed of light in air, v2v_2 is the speed of light in glass, n1n_1 is the refractive index of air, n2n_2 is the refractive index of glass.

Thus, we can find the speed of light in glass:


v2=v1sinθ2sinθ1=3.0108mssin30sin45=3.0108ms0.50.707=2.12108ms.v_2 = v_1 \frac{\sin \theta_2}{\sin \theta_1} = 3.0 \cdot 10^{8} \frac{\text{m}}{\text{s}} \cdot \frac{\sin 30{}^{\circ}}{\sin 45{}^{\circ}} = 3.0 \cdot 10^{8} \frac{\text{m}}{\text{s}} \cdot \frac{0.5}{0.707} = 2.12 \cdot 10^{8} \frac{\text{m}}{\text{s}}.

Answer: a) $2.12 \cdot 10^{8} \frac{\text{m}}{\text{s}}$

19. A 9V9V battery is short-circuited. The potential difference across the battery is found to be 8V8V, and the current is 5A5A. What is the internal resistance of the battery?

a) 0.1Ω0.1\Omega

b) 0.2Ω0.2\Omega

c) 0.3Ω0.3\Omega

d) 0.4Ω0.4\Omega

Solution:


Let us consider the short-circuited battery in the figure. The voltage VV of the battery is defined as the difference in electric potential between its positive and negative terminals – the points AA and BB , respectively. As we move from BB to AA , the electric potential increases by +E+\mathcal{E} volts as we cross the electromotive force, but then decreases by IrIr volts as we cross the internal resistor. The voltage drop across the resistor follows from Ohm's law, which implies that the drop in voltage across a resistor RR , carrying a current II , is IRIR in the direction in which the current flows. Therefore, the voltage VV of the battery is related to its electromotive force E\mathcal{E} and internal resistance rr as:


V=EIr,V = \mathcal {E} - I r,r=EVI=9V8V5A=1V5A=0.2Ω.r = \frac {\mathcal {E} - V}{I} = \frac {9 V - 8 V}{5 A} = \frac {1 V}{5 A} = 0. 2 \Omega .


Answer: b) 0.2Ω0.2\Omega

20. Ohm's law relates potential difference with?

a) power

b) energy

c) current

d) time

Answer: Ohm's law states that the current through a conductor between two points is directly proportional to the potential difference across the two points. So, the answer is c) current.

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