

InterviewSolution
This section includes InterviewSolutions, each offering curated multiple-choice questions to sharpen your knowledge and support exam preparation. Choose a topic below to get started.
2201. |
A hollow spherical shell is compressed to half its radius. The ggravitational potential at the centreA. increasesB. decreasesC. remains sameD. during the compression increases then returns to the previous value. |
Answer» Correct Answer - B | |
2202. |
A hollow spherical shell is compressed to half its radius. The gravitational potential at the centreA. increasesB. decreasesC. remain sameD. during the compression increase then returns at the previous value. |
Answer» Correct Answer - b Potential inside the shell `=-(GM)/R` |
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2203. |
A satellite moves around the earth in a circular orbit with speed `v`. If `m` is the mass of the satellite, its total energy isA. `1/2mv^(2)`B. `mv^(2)`C. `-1/2 mv^(2)`D. `3/2 mv^(2)` |
Answer» Correct Answer - C `TE=-KE=-1/2mv^(2)` |
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2204. |
A planet is moving in an elliptic orbit. If `T,V,E` and `L` stand, respectively, for its kinetic energy, gravitational potential energy, total energy and angular momentum about the centre of force, thenA. T is conservedB. U is always positiveC. E is always negativeD. L is conserved but direction of vector L changes continuously |
Answer» Correct Answer - C |
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2205. |
The gravitational potential energy of satellite revolving around the earth in circular orbit is `4MJ`. Find the additional energy (in `MJ`) that should be given to the satellite so that it escape from the gravitational field of the earth. |
Answer» Correct Answer - 2 `PE=-4MJ TE=-2MJ` The additional energy required to make the satellite escape `=+2MJ`. |
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2206. |
A seconds pendulum is mounted in a rocket. Its period of oscillation decreases when the rocketA. comes down with uniform acccelerationB. moves round the earth in a geostationaly orbitC. moves up with a uniform veloctiyD. moves up with uniform acceleration |
Answer» Correct Answer - D |
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2207. |
A star can be considered as spherical ball of hot gas of radius `R`. Inside the star, the density of the gas is `rho_(r)` at radius `r` and mass of the gas within this region is `M_(r)`. The correct differential equation for variation of mass with respect to radius is (refer to the adjacent figure)A. `(dM_(1))/(dr)=A/3pirho_(r)r^(3)`B. `(dM_(r))/(dr)=4pirho_(r)r^(2)`C. `(dM_(r))/(dr)=2/3pirho_(r)r^(2)`D. `(dM_(r))/(dr)=1/3pirho_(r)r^(2)` |
Answer» Correct Answer - B `dM_(r)=rho_(r)pir^(2)dr` `(dM_(1))/(dr)=rho_(r)4pir^(2)` |
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2208. |
A black hole is a body from whose surface nothing may ever escape. What is the condition for a uniform spherical mass M to be a black hole? What should be radius of earth if it has to be a black hole? |
Answer» For a body to be a black hole, even light should not escape. So limiting escape velocity is 3 × 108 ms-1 So, for body of Mass M, condition is, \(\sqrt \frac {2GM}{R}\) ≥ 3 × 108 ms-1 For Earth, M = 6 × 1024 kg \(\frac {2 \times 6.67 \times 10^{-11} \times 6 \times 10^{24}}{R}\) = (3 × 108)2 R = 9 × 10-2 m R = 9 cm. |
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2209. |
The condition for a uniform spherical mass `m` of a radius `r` to be a black hole is [`G` =gravitational constant and `g`=acceleration due to gravity]A. `((2Gm)/r)^(1//2) lec`B. `((2Gm)/r)^(1//2)gec`C. `((2gm)/r)^(1//2)=c`D. `((gm)/r)^(1//2)gec` |
Answer» Correct Answer - B A black hole is an object so massive that even light cannot escape from it. This requires the idea of a gravitational mass for a photon, which then allows the calculation of an escape energy for an object of that mass. Escape velocity for that body `v_(e)=sqrt((2Gm)/r)` `v_(e)` should be more than or equal to speed of light i.e., `sqrt((2Gm)/r)gec` |
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2210. |
Figure shows the kinetic energy `(E_(k))` and potential energy (`E_(p)`) curves for a two-particle system. Name the point(s) at which the system is a bound system. A. `A`B. `B`C. `C`D. `D` |
Answer» Correct Answer - A::B::C::D For all points, `E_(P)gtE_(K)` (numerically). So, totally energy is negative. Thus, the system is a bound system corresponding to all the points. |
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2211. |
A spherically symmetric gravitational system of particles has a mass density` rho={(rho_0,for, r,lt,R),(0,for,r,gt,R):}` where`rho_0` is a constant. A test mass can undergo circular motion under the influence of the gravitational field of particles. Its speed v as a function of distahce `r(0ltrltOO)` form the centre of the system is represented byA. B. C. D. |
Answer» Correct Answer - C For `rleR, (mv^(2))/r=(GmM)/(r^(2))to(1)` here, `M=(4/3pir^(3))rho_(0)`substituting in Eq (1) we get `vpropr` i.e., `v-r` graph is a straight line passing through origin, For `rgtR` `(mv^(2))/r=(Gm(3/4piR^(3))rho_(0))/(r^(2))` or `vprop1/r` The corresponding `v-r` graph will be as shown in option (3) |
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2212. |
If a spherically symmetric star of radius `R` collapsed under its own weight, neglecting any forces other than gravitational ones, what is the time required for collapse?A. `(8pi^(2)R^(3))/((GM)^(0.5))`B. `(2pi^(2)R^(3))/((3GM)^(0.5))`C. `(pi^(2)R^(3))/((8GM)^(0.5))`D. `((2R^(3))/(GM))^(0.5)` |
Answer» Correct Answer - A `4pir^(2)dr`=volume of an element of thickness `dr`. The number of particles, `n_(i)=4pir^(2)dr.rho`, assumming `rho` is the number of the particles per unit volume. The acceleration due to gravity `=g/Rxxr` for each particle `n_(j)g=4pir^(2)drrho.g/Rr=4pig/Rrhor^(3)dr` `:.` mean acceleration of the particle due to gravity, `g=(int_(O)^(R)((4pi)/Rr^(3)dr)rho)/((4//3)piR^(3)rho)` Average distance travelled by the particle is `=(sumn_(i)r)/(sumn_(i))rArrbar(r)=3/4R` `:. bar(r)=1/2bar(at^(2))` where `bar(a)` average acceleration `rArr 3/4R=1/2.3/4g.t^(2)rArr t=sqrt((2R)/g)` `g=(GM)/(R^(2))rArr ((2R.R^(2))/(GM))^(1//2)=((2R^(3))/(GM))^(0.5)` |
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2213. |
A stone is thrown vertically upwards with a speed of 20m/s. If g = 10m/s2, find(1) Time is taken by the stone to reach the maximum height.(2) Total distance covered by the stone to reach the maximum height. |
Answer» We are given that: Initial velocity (u) = 20 m/s When an object attain maximum height, then final velocity (ν) = 0 a = g = 10m/s2, time (t) = ? (1) From first equation of motion, we have v = u – gt ⇒ 0 = 20 - 10 x t ⇒ 10t = 20 ⇒ t = 2 sec (2) From third equation of motion, we have ⇒ (0)2 = (20)2 - 2 x 10 x h ⇒ 20h = 20 x 20 ⇒ h = 20 m |
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2214. |
A stone is released from the top of a tower 125 m high. Then find:(1) the time with which the stone strikes the ground.(2) the final velocity of the stone. (Take g = 10 m/s2) |
Answer» We are given that: Height of tower (h) = 125 m Initial velocity (u) = 0 g = 10 m/s2 (1) From 2nd equation of motion For downward motion: h = ut + \(\frac{1}{2}\)gt2 ⇒ 125 = 0 x t + \(\frac{1}{2}\) x 10 x t2 = 125 = 5t2 ⇒ t2 = 25 ⇒ t = 5sec2 (2) From 1st equation of motion, v = u + gt ⇒ u = 0 + 10 x 5 ⇒ v = 50 m/s |
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2215. |
At maximum of the locations the value of ‘g’ is a maximum:A. On the top of Mount EverestB. On the top of Qutab MinarC. At any place on the equatorD. A camp site in Antarctica |
Answer» We know that the value of g is inversely proportional to the square of radius or g ∝ \(\frac{1}{R^2}\). Radius of earth is minimum at poles, so acceleration due to gravity is maximum at poles. Similarly, radius of earth is maximum at equator, so acceleration due to gravity is minimum at equator. Also, acceleration due to gravity decreases as we go higher from the earth surface. Hence, option D is correct. |
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2216. |
A ball is thrown vertically upward, acceleration due to gravity is:A. in the direction opposite to the direction of motionB. in the direction same as the direction motionC. increases as it comes downD. becomes zero at the highest point |
Answer» When a ball is thrown vertically upward, then acceleration due to gravity is directed opposite to the direction of motion since the ball experiences a force of attraction directed towards the center of earth due to earth’s gravity. Direction of acceleration is in the direction of force as, a = \(\frac{F}{m}\) So, from above, we can conclude that acceleration is also directed towards the centre of earth which is opposite to the vertically upward motion of the ball. Hence, option A is correct. |
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2217. |
A stone is dropped from the top of the tower. Its speed after it has fallen 20 m is (Take g = 10 ms-2)A. -10 ms-1B. 10 ms-1C. -20 ms-1D. 20 ms-1 |
Answer» Here, u = Initial velocity = 0 v = Final velocity s = Distance travelled = 20 m a = acceleration = g = 10 ms-2 Now, we know from the equations of motion that v2 = u2 + 2as v = \(\sqrt {u^2\,+\,2as}\) v = \(\sqrt {0\,+\,2\,*\,10\,*\,20}\) v = \(\sqrt {400}ms^{-1}\) v = 20 ms-1 Hence, option D is correct. |
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2218. |
A stone is dropped from the top of a tower 40 metre high. Its velocity after it has fallen for 2s is: (Take g = 10m/s2). (A) – 10 m/s (B) 10 m/s (C) – 20 m/s (D) 20 m/s |
Answer» The answer is (C) – 20 m/s |
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2219. |
A coin and a piece of paper are dropped simultaneously from the same height. Which of the two will touch the ground first ? What will happen if the coin and the piece of paper are dropped in vacuum ? Give reasons for your answer. |
Answer» The coin reaches the ground first as compared to the piece of paper because it experiences lesser resistance from air than that felt by paper. If the coin and the piece of paper are dropped in vacuum, both of them will touch the ground at the same time. |
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2220. |
A body is dropped from a height equal to radius of the earth. The velocity acquired by it before touching the ground isA. `V=sqrt(2gR)`B. `V=3gR`C. `V=sqrt(gR)`D. `V=2gR` |
Answer» Correct Answer - C | |
2221. |
For a planet revolving round the sun, when it is nearest to the sunA. `K.E.` is min and `P.E.` is max.B. both `K.E.` and `P.E.` are minC. `K.E.` is max. and `P.E.` is minD. `K.E.` and `P.E.` are equal |
Answer» Correct Answer - C | |
2222. |
At what depth below the surface of the earth acceleration due to gravity will be half its value at 1600 km above the surface of the earth ?A. `4.3 xx 10^(6)` mB. `2.4 xx 10^(6)` mC. `3.2 xx 10^(6)` mD. `1.6 xx 10^(6)` m |
Answer» Correct Answer - A Given, `g=(1-(d)/(R))=(1)/(2)(g)/((1+(h)/(R))^(2))` or `1-(d)/(R)=(1)/(2(1+(1600)/(6400))^(2))=(16)/(50)rArr(d)/(R)=(34)/(50)` `:. d=(6.4xx10^(6)m)((34)/(50))=4.352 xx10^(6)m` |
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2223. |
The acceleration due to gravity on the planet `A` is `9` times the acceleration due to gravity on planet `B`. A man jumps to a height of `2m` on the surface of `A`. What is the height of jump by the same person on the planet `B`?A. 6 mB. `2//3` mC. `2//9` mD. 18 m |
Answer» Correct Answer - D It is given that acceleratini due to gravity on planet A is 9 times the acceleration due to gravity on planet B i.e `g_(A)=9g` From third equatin of motion `v^(2)=2gh` At planet A `h_(A)=(V^(2))/(23g_(A))` At planet B `h_(B)=(v^(2))/(2g_(B))` for safe jump `v_(1)=v_(2)` Dividing Eq ii by Eq iii we have `(h_(A))/(H_(B))=(g_(B))/(g_(A))` `rarr (h_(A))/(h_(B))=1/9` `rarr h_(B)=9h_(A)=9xx2=18m` |
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2224. |
If g is the acceleration due to gravity on the earth’s surface, the gain in the potential energy of an object of mass m raised from surface of the earth to a height equal to radius R of the earth is - [M = mass of earth]A. 2mgRB. mgRC. `1/2` mgRD. `1/4` mgR |
Answer» Correct Answer - C The potential energy of an object at the surface of the earth `U_(1)=-(GMm)/(R )` The potential energy of the object at a height h =R from the surface of the earth `U_(2)=-(GMm)/(R+h)=-(GMm)/(R+R)` hence the gain in potential energy of the object `triangleU=-(GMm)/(2R)+(GMm)/(R )` `=1/2 . (GMm)/(R )` But we know that `GM=gR^(2)` hence `triangle U =1/2 (gR^(2)m)/(R )=1/2gRm=1/2mgR` |
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2225. |
How much below the surface of the earth does the acceleration due to gravity become `70%` of its value at the surface of the earth ? Radius of the earth is 6400 km |
Answer» Correct Answer - 1920 km |
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2226. |
Calculate the depth below the surface of the earth where acceleration due to gravity becomes half of its value at the surface of the earth . Radius of the earth = 6400 km. |
Answer» Correct Answer - 3200 km |
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2227. |
At what depth below the surface does the acceleration due to gravity becomes 70% of its value in the surface of earth ? |
Answer» Correct Answer - 1920 km | |
2228. |
Find the percentage decrease in the weight of a body when taken 16 km below the surface of the earth. Take radius of the earth is 6400 km. |
Answer» Correct Answer - 0.005 | |
2229. |
Determine the decrease in the weight of a body when it is taken 32 km below the earth surface. Take radius of the earth as 6400 km.A. `1%`B. `2%`C. `1.5%`D. `5%` |
Answer» Correct Answer - A In this case, `h lt lt R " " therefore g_(h)=g(1-(2h)/(R ))=g-(2gh)/(R )` `therefore g-g_(h)=(2gh)/(R )" "` ……..(1) `therefore` Percentage decrease in weight `= (mg-mg_(h))/(mg)xx100` `=((g-g_(h))/(g))xx100=(2gh)/(gR)xx100 " "` ......from (1) `=(2h)/(R )xx100=(2xx32)/(6400)xx100=1%` `therefore` Percentage decrease = 1% |
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2230. |
If the radius of the earth was to shringk by 2% its mass remaining same the acceleraton due to gravity on the earth surface would beA. decrease by 2%B. increased by 2%C. incresed by 4%D. decrease by 4% |
Answer» Correct Answer - C As `Gg=(GM)/(R^(2))` if R decreases then g increases taking logarithm of both the sides we get `log g = log G+log M -2 log R` Differentaiting it we get `(dg)/(g)=0 +0-(2dR)/(r )=-2(-2)/(100)=(4)/(100)` ` therefore` % increasing in `g=(dg)/(g)xx100=4/100xx100=4%` |
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2231. |
If the radius of the earth was to shringk by 2% its mass remaining same the acceleraton due to gravity on the earth surface would beA. increase by 2%B. increase by 4%C. decrease by 2%D. decrease by 4% |
Answer» Correct Answer - B `g=(GM)/(R^(2))therefore log g = log M +log G - 2 log R` `therefore (dg)/(g)=-2(dR)/(R )` `therefore (dg)/(g)xx100=-2xx(-2)/(100)=(4)/(100)` |
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2232. |
A body on the equaotr of a planet weighs half of its weight at the pole. The density of matter of the planet is `3g//cm^(3)`. Determine the peiod of rotation of the planet about its axis. |
Answer» Correct Answer - `3.16 xx 10^(-4) rad//s` |
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2233. |
Will your weight remain constant as you go above the surface of the earth? |
Answer» No. As we go above the surface of the earth, our weight will go on decreasing. |
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2234. |
What is gravitational potential energy?(OR)Define gravitational potential energy. Write the formula for it. |
Answer» The energy stored in a body due to the gravitational force between the body and the earth is called the gravitational potential energy. Gravitational potential energy of a body of mass m = \(-\frac{GMm}{R+h}\), where G = gravitational constant, M = mass of the earth, R = radius of the earth, h = height of the body from the surface of the earth. [Note : As the body is bound to the earth due to the earth’s gravitational froce, the gravitational potential energy of the body is negative. If the body is given kinetic energy equal to \(\frac{GMm}{R+h}\) the body will overcome the earth’s gravitational force. It will then move to infinity and come to rest there.] |
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2235. |
Will the direction of the gravitational force change as we go inside the earth? |
Answer» Answer is No. |
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2236. |
What will be the value of g at the centre of the earth? |
Answer» Answer is Zero. |
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2237. |
What is escape Velocity?(OR)Define escape velocity. |
Answer» When a body is thrown vertically upward from the surface of the earth, the minimum initial velocity of the body for which the body is able to overcome the downward pull by the earth and can escape the earth forever is called the escape velocity. |
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2238. |
Explain the term escape velocity. (OR) Write a short note on escape velocity. |
Answer» In general, when a body is thrown vertically upward from the earth’s surface, its velocity goes on decreasing and after some time the body falls back to the ground. If its initial velocity is increased, the maximum height attained by it is more, but it does fall back to the ground. If the initial velocity is increased continuously, for a particular initial velocity, the body can overcome the earth’s gravitational force and move to infinity and come to rest there. This velocity is called the escape velocity. |
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2239. |
Define gravitational potential and field intensity. Give their units. Also, write relation between them. |
Answer» Gravitational potential at point is defined as the work done in bringing a body of unit mass from infinity to that point. Its unit is J/kg, denoted by V Gravitational field intensity is defined as the force experienced by a unit mass at that point. It is expressed in N/kg, denoted by I. l = -v/R. |
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2240. |
If the earth is one half of its present distance from the sun, How many days will the present one year on the surface will change? |
Answer» We know that, T2 ∝ R3 \((\frac{T_1}{T_2})^2 = \) \((\frac {R_1}{R_2})^3\) T1 = (1/2)3/2T = \(\frac {T}{2\sqrt2}\) T1 = 129 days The year of the new Earth will have 236 days lesser. |
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2241. |
Explain the variation of ‘g’ with 1. height 2. depth |
Answer» Consider M to be mass of Earth and R to be radius of Earth. 1. At a point ‘h’ above the ground New g is gn = \(\frac {GM} {(R+h)^2}\) = \(\frac {GM} {R^2[1+\frac{h}{R}]^2}\) gn = g\([1+\frac {h}{R}]^{-2}\) if h << R, gn = g\([1-\frac {2h}{R}]\) So, g decreases with increase in height, 2. At a depth ‘d’ below the ground. The new g, gd is given by dd = g\([1-\frac {d}{R}]\) So, g also decreases with depth. |
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2242. |
The graph that represents variation of g with depth (d) from the surface of the earth isA. B. C. D. |
Answer» Correct Answer - d `g_(d)=g(1-(d)/(R)),Y=-mx+c`. It is straight line with negative slope. |
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2243. |
A star like the sun has several bodies moving around it at different distances. Consider that all of them are moving in circular orbits. Let r be the distance of the body from the centre of the star and let its linear velocity be v, angular velocity w, kinetic energy K, gravitational potential energy U, total energy E and angular momentum 1. As the radius r of the orbit increases, determine which of the above quantities increases and which ones decreases. |
Answer» Consider a body of mass m is rotating around the star s in circular path of radius r. (i) Orbital velocity – vo = \(\sqrt{\frac{GM}{r}}\) or v ∝ \(\frac{1}{\sqrt r}\) Orbital Velocity decreases (ii) Angular velocity \(\frac{2\pi}{T}\) By Kepler’s III law T2 \(\propto\) r3 or T2 = Kr3 \(\omega\) = \(\frac{2\pi}{Kr^{\frac{3}{2}}}\) or \(\omega\) \(\propto\) \(\frac{1}{\sqrt{r^3}}\) Hence, angular velocity decreases. (iii) Kinetic Energy, K = \(\frac{1}{2}\)m\(\frac{GM}{r}\) or K \(\propto\) \(\frac{1}{r}\) Hence K, decreases on increasing the radius. (iv) Gravitational Potential Energy, U = \(-\frac{GMm}{r}\) or U \(\propto\) \(\frac{-1}{2}\) So, on increasing radius of circular orbit the U increases. (v) Total energy, E = K + U = \(\frac{GMm}{2r}+\big(-\frac{Gmm}{r}\big)\) E = −\(\frac{GMm}{2r}\) So, increasing the radius, E will also be increased. (vi) Angular momentum, L = mvr = mr\(\sqrt{\frac{GM}{r}}\) L = m\(\sqrt{GMr}\) or L \(\propto\) \(\sqrt r\), increases |
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2244. |
Six point masses of mass m each are at the vertices of a regular hexagon of side L. Calculate the force on any of the masses. |
Answer» Let us consider the following diagram in which size point masses are placed at six sides. A, B, C, D, E, F. AC = AG + GC + = 2AG = 2I cos 30º = 2I\(\sqrt{\frac{3}{2}}\) = \(\sqrt3\) I = AE AD = AH + HJ + JD = I sin 30º + I + I sin 30º = 2 I Force on A due to B, F1 = \(\frac{GMm}{I^2}\) along A to B = \(\frac{Gm^2}{I^2}\) Force on A due to C,F2 = \(\frac{Gm.m}{(\sqrt3I)^2}\) = \(\frac{Gm^2}{3I^2}\) along A to C [\(\because\) AC = \(\sqrt3I\)] Force on A due to D,F3 = \(\frac{Gm.m}{(\sqrt2I)^3}\) = \(\frac{Gm^2}{4I^2}\) along A to D [\(\because\) AD = 2I] Force on A due to E,, F4 = \(\frac{Gm.m}{(\sqrt3I)^2}\) = \(\frac{Gm^2}{3I^2}\) along A to E Force on A due to F, F5 = \(\frac{Gm.m}{(I)^2}\) along A to F = \(\frac{Gm^2}{I^2}\) along A to F Resultant force due to F1 and F5, F1 = \(\sqrt{F_1^2+F^2_5+2F_2F_5\cos120^o}\) = \(\frac{Gm^2}{I^2}\) along A to D [Angle b/w F1 and F5= 120º] Resultant force due to F2 and F4, F1 = \(\sqrt{F_1^2+F^2_4+2F_2F_4\cos60^o}\) = \(\frac{\sqrt3Gm^2}{3I^2}\) = \(\frac{Gm^2}{\sqrt3I^2}\) along A to D \(\because\) Net force along A to D = F1 + F2 + F3 = \(\frac{Gm^2}{I^2}+\frac{Gm^2}{\sqrt3I^2}+\frac{Gm^2}{4I^2}\) = \(\frac{Gm^2}{I^2}\)\(\big(1+\frac{1}{\sqrt3}+\frac{1}{4}\big)\) |
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2245. |
What is the angle between the equatorial plane and the orbital plane of (a) Polar satellite? (b) Geostationary satellite? |
Answer» (a) Angle between equatorial plane and orbital plane is 90º . (b) Angle between equatorial and orbital plane is 0º . |
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2246. |
A planet of mass `m` moves around the Sun of mass Min an elliptical orbit. The maximum and minimum distance of the planet from the Sun are `r_(1)` and `r_(2)`, respectively. Find the relation between the time period of the planet in terms of `r_(1)` and `r_(2)`. |
Answer» Correct Answer - `T prop (r_(1) +r_(2))^3//2` |
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2247. |
A planet of mass `m` moves around the Sun of mass Min an elliptical orbit. The maximum and minimum distance of the planet from the Sun are `r_(1)` and `r_(2)`, respectively. Find the relation between the time period of the planet in terms of `r_(1)` and `r_(2)`.A. `(r_(1)+r_(2))`B. `(r_(1)+r_(2))^(1//2)`C. `r_(1)-r_(2))^(3//2)`D. `(r_(1)+r_(2))^(3//2)` |
Answer» Correct Answer - D According to kepler third law `T^(2)` is proportinal to cube of semi major axis of the alliptical orbit Semi major axis `=(r_(1)+r_(2))/(2)` `therefore T^(2) prop [(r_(1)+r_(2))/(2)] rarr T prop (r_(1)r_(2))^(3//2)` |
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2248. |
A planet of mass `m` moves around the Sun of mass Min an elliptical orbit. The maximum and minimum distance of the planet from the Sun are `r_(1)` and `r_(2)`, respectively. Find the relation between the time period of the planet in terms of `r_(1)` and `r_(2)`.A. `r_(1)^(3//2)`B. `(r_(1)+r_(2))^(3//2)`C. `(r_(1)-r_(2))^(3//2)`D. `r_(1)^(3//2)` |
Answer» Correct Answer - B Semi major axis, `a=(r_(1)+r_(2))/(2)` Now, `T^(2)propa^(3)` `rArr T prop a^(3//2)prop ((r_(1)+r_(2))/(2))^(3//2)rArr T prop (r_(1)+r_(2))^(3//2)`. |
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2249. |
A rocket is launched vertical from the surface of the earth of radius R with an initial speed `v`. If atmospheric resistance is neglected, then maximum height attained by the rocket isA. `h=(R)/(((2gR)/(v^(2))-1))`B. `h=(R)/(((2gR)/(v^(2))+1))`C. `h=(R^(2))/(((2gR)/(v^(2))-1))`D. `h=(R^(2))/(((2gR)/(v^(2))+1))` |
Answer» Correct Answer - A `(1)/(2)mv^(2)=(mgh)/(1+(h)/(R))` On solving Eq. (i) for `h`, we get `:. h=(v^(2))/(2g-(v^(2))/(R))=(R)/(((2gR)/(v^(2)))-1)`. |
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2250. |
A rocket is launched vertical from the surface of the earth of radius R with an initial speed `v`. If atmospheric resistance is neglected, then maximum height attained by the rocket isA. `h=(R )/((2gR)/(V^(2))-1)`B. `h=(R )/((2gR)/(V^(2))+1)`C. `h=(R )^(2)/((2gR)/(V^(2))-1)`D. `h=(R )^(2)/((2gR)/(V^(2))+1)` |
Answer» Correct Answer - A `1/2 mv^(2)=(mgR)/(1+(R )/(h)) rarr 1+(R )/(h)=2gR//v^(2)` `therefore (R )/(h=(2gR)/(v^(2))-1` |
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