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Ethiopian University Entrance Examination (EUEE)

Physics 2011

2011 E.C. · 2019 G.C. · Booklet 26

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Constants and formulas given with the paper

Constants and formulas given with the paper
ConstantSymbolValue
Acceleration due to gravitygg10 m/s210\ \mathrm{m/s^2}
Permittivity of vacuumε0\varepsilon_08.85×1012 F/m8.85\times10^{-12}\ \mathrm{F/m}
Charge of an electronee1.6×1019 C1.6\times10^{-19}\ \mathrm{C}
Universal Gravitational ConstantGG6.67×1011 Nm2/kg26.67\times10^{-11}\ \mathrm{N\,m^2/kg^2}
Density of waterρ\rho1000 kg/m31000\ \mathrm{kg/m^3}
Planck's constanthh6.63×1034 Js6.63\times10^{-34}\ \mathrm{J\,s}
Electron massmeme9.11×1031 kg9.11\times10^{-31}\ \mathrm{kg}
Elementary (unit charge)ee1.602×1019 C1.602\times10^{-19}\ \mathrm{C}
Trigonometric values givensin30=cos60\sin 30^\circ = \cos 60^\circ0.50.5
sin37=cos53\sin 37^\circ = \cos 53^\circ0.60.6
sin45=cos45\sin 45^\circ = \cos 45^\circ0.7070.707
sin53=cos37\sin 53^\circ = \cos 37^\circ0.80.8
sin60=cos30\sin 60^\circ = \cos 30^\circ0.8660.866
Coulomb's constantkk9×109 Nm2/C29\times10^9\ \mathrm{Nm^2/C^2}
Permeability of free spaceμ0\mu_04π×107 Tm/A4\pi\times10^{-7}\ \mathrm{Tm/A}

Pick an answer and see straight away whether it was right.

Questions 1–5

Page 1 of 10
01
Let C=A×B\vec{C} = \vec{A} \times \vec{B} and θ90\theta \neq 90^\circ, where θ\theta is the smaller angle between A\vec{A} and B\vec{B} when they are drawn with their tails at the same point. Which of the following is not true?

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AnswerDAB=0\vec{A}\cdot\vec{B} = 0

A cross product is always perpendicular to both of its factors, so AC=0\vec{A}\cdot\vec{C}=0 holds for any θ\theta; and C=B×A-\vec{C}=\vec{B}\times\vec{A} and C=ABsinθ|\vec{C}|=|\vec{A}||\vec{B}|\sin\theta are the definition of the product itself, so they hold too.

The dot product is the different case: AB=0\vec{A}\cdot\vec{B}=0 requires the two vectors to be perpendicular. The question fixes θ90\theta\neq90^\circ, so that is the statement which fails.
  • Vectors · G11 U2
02
A driver of an automobile travelling at a constant speed of 20m/s20\,\mathrm{m/s} suddenly applies a brake and the automobile comes to rest in 2.02.0 seconds after skidding for a certain distance. What is the length of the skid distance?

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AnswerC20 m20\ \mathrm{m}

v0=20m/sv_0=20\,\mathrm{m/s}, v=0v=0, t=2.0st=2.0\,\mathrm{s}

The car decelerates uniformly to rest, so the skid distance is the average velocity times the time, d=vˉt=v0+v2td=\bar v\,t=\dfrac{v_0+v}{2}t. d=20+02×2.0=20md=\frac{20+0}{2}\times2.0=20\,\mathrm{m}
  • Kinematics · G11 U3
03
Which of the following is correct about the motion shown in the velocity-time graph below?
2 4 6 8 10 12 14 2 6 8 10 12 14 v(m/s) t(Sec) B(2,4) C(3,12) D(6,12) E(12,0)

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AnswerBTotal displacement is 84m.

Displacement is the area under a velocity-time graph.

Adding the triangle from the origin to B, the trapezoid from B to C, the rectangle from C to D and the triangle from D to E: 4+8+36+36=84m4+8+36+36=84\,\mathrm{m} Between D and E the slope is negative rather than positive, and between B and C it is 8m/s28\,\mathrm{m/s^2} rather than 4m/s24\,\mathrm{m/s^2}, so the total displacement of 84m84\,\mathrm{m} is the only true statement.
  • Kinematics · G11 U3
04
An object of mass M is set in a vertical circular motion. The tension T from the rope keeps the object in a circular path with speed v. Where does the rope experience a maximum tension?

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AnswerAAt the bottom of the circle

At the bottom of the loop the rope must supply the centripetal force and support the object's weight, while at the top gravity itself contributes to the centripetal force: Tbottom=mv2r+mg,Ttop=mv2rmgT_{bottom}=\frac{mv^2}{r}+mg,\qquad T_{top}=\frac{mv^2}{r}-mg

The object is also fastest at the bottom, by conservation of energy, so both effects favour the bottom — the tension is greatest there.
  • Circular motion · G11 U4
05
Two forces F1=3ı^N\vec{F}_1 = 3\hat{\imath}\,\mathrm{N} and F2=4ȷ^N\vec{F}_2 = 4\hat{\jmath}\,\mathrm{N} are acting on a particle of mass m. What is the magnitude and direction of a force that balances the two?

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AnswerDF1Feq=5N\vec{F}_1\vec{F}_{eq} = 5\,\mathrm{N} at 143143^\circ counterclockwise from F2\vec{F}_2

F1=3ı^N\vec{F}_1=3\hat{\imath}\,\mathrm{N}, F2=4ȷ^N\vec{F}_2=4\hat{\jmath}\,\mathrm{N}

A force that balances the two is equal in magnitude and opposite in direction to their resultant R=F1+F2\vec{R}=\vec{F}_1+\vec{F}_2. R=32+42=5N,at tan1(4/3)=53 counterclockwise from F1R=\sqrt{3^2+4^2}=5\,\mathrm{N},\quad\text{at }\tan^{-1}(4/3)=53^\circ\text{ counterclockwise from }\vec{F}_1 The balancing force Feq\vec{F}_{eq} therefore also has magnitude 5N5\,\mathrm{N}, pointing opposite R\vec{R} — which is 53+90=14353^\circ+90^\circ=143^\circ counterclockwise from F2\vec{F}_2.
O F₁ = 3N F₂ = 4N R = 5N Feq = 5N 53°
  • Vectors · G11 U2

Source: Ethiopian University Entrance Examination, Physics, 2011 E.C. (2019), booklet code 26.