Gravitational Field and Orbits

15 questions

Question 1Question

Two point masses are separated by a distance rr and exert a gravitational force FF on each other. If the distance between them is doubled while keeping their masses constant, what is the new gravitational force between them?

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Answer: F4\frac{F}{4}

Answer

The new gravitational force between the two masses is F4\frac{F}{4}.
Gravitational force obeys an inverse-square law with respect to distance (F1r2F \propto \frac{1}{r^2}). When separation distance is multiplied by 2, the force decreases by a factor of 22=42^2 = 4, yielding F4\frac{F}{4}.

Step-by-Step Solution

1
Write down Newton's Law of Universal Gravitation
F=Gm1m2r2F = \frac{G m_1 m_2}{r^2}
Establish the mathematical relationship governing gravitational force and separation distance.
2
Substitute the new distance r=2rr' = 2r into the gravitational force equation
F=Gm1m2(2r)2=Gm1m24r2F' = \frac{G m_1 m_2}{(2r)^2} = \frac{G m_1 m_2}{4r^2}
Evaluate how doubling the separation distance affects the magnitude of the force.
3
Express the new force FF' in terms of the initial force FF
F=14(Gm1m2r2)=F4F' = \frac{1}{4}\left(\frac{G m_1 m_2}{r^2}\right) = \frac{F}{4}
Relate the calculated force directly to the original force FF.

Key Concept

Inverse-Square Law of Gravitation
Estimated Time:45s
Question 2Question

A satellite of mass mm moves in a circular orbit around a uniform spherical planet of radius RR. If the height of the satellite above the planet's surface is h=2Rh = 2R and the acceleration due to gravity at the planet's surface is gg, which of the following expressions represents the orbital speed of the satellite?

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Answer: gR3\sqrt{\frac{gR}{3}}

Answer

The orbital speed of the satellite is gR3\sqrt{\frac{gR}{3}}.
The total orbital radius from the center of the planet is r=R+h=R+2R=3Rr = R + h = R + 2R = 3R. Since surface gravity is g=GMR2g = \frac{GM}{R^2}, we have GM=gR2GM = gR^2. Substituting these into the orbital velocity expression v=GMrv = \sqrt{\frac{GM}{r}} yields v=gR23R=gR3v = \sqrt{\frac{gR^2}{3R}} = \sqrt{\frac{gR}{3}}, which makes the expression gR3\sqrt{\frac{gR}{3}} correct.

Step-by-Step Solution

1
Determine the total orbital radius from the center of the planet.
r=R+h=R+2R=3Rr = R + h = R + 2R = 3R
Gravitational attraction and circular orbital radii are always measured from the center of mass of the primary body, not its surface.
2
Relate the gravitational constant GG and planet mass MM to surface gravity gg.
g=GMR2    GM=gR2g = \frac{GM}{R^2} \implies GM = gR^2
At the surface of a spherical planet of radius RR, the gravitational field strength is gg.
3
Substitute r=3Rr = 3R and GM=gR2GM = gR^2 into the circular orbital velocity equation v=GMrv = \sqrt{\frac{GM}{r}}.
v=gR23R=gR3v = \sqrt{\frac{gR^2}{3R}} = \sqrt{\frac{gR}{3}}
Equating centripetal force to gravitational force mv2r=GMmr2\frac{m v^2}{r} = \frac{G M m}{r^2} yields v=GMrv = \sqrt{\frac{GM}{r}}.

Key Concept

Orbital velocity of a satellite in terms of surface gravitational acceleration and orbital radius
Question 3Question

A uniform spherical planet has twice the mass and twice the radius of the Earth. If the acceleration due to gravity at the Earth's surface is gg, what is the acceleration due to gravity at the surface of this planet?

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Answer: 0.5g0.5g

Answer

The acceleration due to gravity at the surface of the planet is 0.5g0.5g.
The acceleration due to gravity at a planet's surface is given by g=GMR2g = \frac{GM}{R^2}. Doubling the mass doubles the field strength, but doubling the radius reduces the field strength by a factor of 22=42^2 = 4 due to the inverse-square law. Combining these changes results in 24g=0.5g\frac{2}{4}g = 0.5g.

Step-by-Step Solution

1
Write the general expression for surface acceleration due to gravity.
g=GMR2g = \frac{GM}{R^2}, where GG is the gravitational constant, MM is planetary mass, and RR is planetary radius.
Establishes the fundamental formula relating gravity to mass and radius.
2
Substitute the given parameters for the new planet (Mp=2MM_p = 2M and Rp=2RR_p = 2R).
gp=G(2M)(2R)2=2GM4R2g_p = \frac{G(2M)}{(2R)^2} = \frac{2GM}{4R^2}.
Applies the proportional changes to mass and radius into the formula.
3
Simplify the expression to find gpg_p in terms of gg.
gp=24(GMR2)=0.5gg_p = \frac{2}{4} \left(\frac{GM}{R^2}\right) = 0.5g.
Evaluates the fractional change relative to Earth's surface gravity.

Key Concept

Dependence of surface gravitational field strength on planetary mass and radius via the inverse-square law.
Estimated Time:1m 15s
Question 4Question

A spherical planet has a radius of 7.2×106 m7.2 \times 10^{6} \text{ m} and an acceleration due to gravity of 10 m/s210 \text{ m/s}^2 at its surface. What is the escape velocity for an object launched from the surface of this planet, in km/s\text{km/s}?

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Answer: 12

Answer

The escape velocity from the surface of the planet is 12 km/s.
The escape velocity vev_e from the surface of a spherical planet of radius RR with surface gravity gg is given by ve=2gRv_e = \sqrt{2gR}. Substituting g=10 m/s2g = 10 \text{ m/s}^2 and R=7.2×106 mR = 7.2 \times 10^6 \text{ m} yields ve=2×10×7.2×106=1.44×108=12000 m/sv_e = \sqrt{2 \times 10 \times 7.2 \times 10^6} = \sqrt{1.44 \times 10^8} = 12000 \text{ m/s}, which equals 12 km/s12 \text{ km/s}.

Step-by-Step Solution

1
Identify the relationship between surface gravity, planetary radius, and escape velocity
The escape velocity formula is ve=2gRv_e = \sqrt{2gR}.
Escape velocity is the minimum initial speed required for an object to overcome the gravitational pull of a celestial body.
2
Substitute the given numerical values into the formula
ve=2×10 m/s2×7.2×106 m=144×106 m/sv_e = \sqrt{2 \times 10 \text{ m/s}^2 \times 7.2 \times 10^6 \text{ m}} = \sqrt{144 \times 10^6} \text{ m/s}.
Plugging in the given values allows direct calculation of the velocity in standard SI units.
3
Simplify the square root and convert units to km/s
ve=12000 m/s=12 km/sv_e = 12000 \text{ m/s} = 12 \text{ km/s}.
Taking the square root of 144×106144 \times 10^6 gives 12000 m/s12000 \text{ m/s}, which corresponds to 12 km/s12 \text{ km/s}.

Key Concept

Escape Velocity from a Planet's Surface
Question 5Question

A satellite orbits the Earth at an altitude equal to three times the radius of the Earth, RR. If the acceleration due to gravity at the Earth's surface is gg, what is the gravitational field strength experienced by the satellite at its orbit?

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Answer: g16\frac{g}{16}

Answer

The gravitational field strength at the orbital position is g16\frac{g}{16}.
The total distance from the center of the Earth to the satellite is r=R+3R=4Rr = R + 3R = 4R. Since gravitational field strength is inversely proportional to the square of the distance from the center of mass, increasing the distance by a factor of 44 reduces the field strength by a factor of 42=164^2 = 16, giving g16\frac{g}{16}.

Step-by-Step Solution

1
Determine the total distance from the center of the Earth to the satellite.
The orbital radius is r=R+h=R+3R=4Rr = R + h = R + 3R = 4R.
Gravitational calculations must be measured from the center of mass of the attracting body, not its surface.
2
Apply Newton's law of universal gravitation for gravitational field strength.
At the surface (r=Rr = R), g=GMR2g = \frac{GM}{R^2}. At orbit (r=4Rr = 4R), g=GM(4R)2=GM16R2g' = \frac{GM}{(4R)^2} = \frac{GM}{16R^2}.
Gravitational field strength follows an inverse-square law with respect to distance from the center of mass.
3
Express the orbital gravitational field strength in terms of the surface gravity gg.
g=116(GMR2)=g16g' = \frac{1}{16} \left(\frac{GM}{R^2}\right) = \frac{g}{16}.
Substituting the surface value g=GMR2g = \frac{GM}{R^2} yields the simplified ratio.

Key Concept

Gravitational Field Strength and Inverse-Square Law
Question 6Question

Planet PP has a mean uniform density that is twice that of Planet QQ, and a radius that is half that of Planet QQ. What is the ratio of the escape velocity at the surface of Planet PP to the escape velocity at the surface of Planet QQ?

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Answer: 12\frac{1}{\sqrt{2}}

Answer

12\frac{1}{\sqrt{2}}
The correct answer is derived by substituting the planet's mass in terms of radius and density (M=43πR3ρM = \frac{4}{3}\pi R^3 \rho) into the escape velocity equation ve=2GMRv_e = \sqrt{\frac{2GM}{R}}. Simplifying gives ve=R83πGρv_e = R\sqrt{\frac{8}{3}\pi G \rho}, which means escape velocity is proportional to RρR\sqrt{\rho}. Halving the radius and doubling the density yields a factor of 12×2=22=12\frac{1}{2} \times \sqrt{2} = \frac{\sqrt{2}}{2} = \frac{1}{\sqrt{2}}.

Step-by-Step Solution

1
Express the mass of a uniform spherical planet in terms of its radius RR and density ρ\rho.
M=43πR3ρM = \frac{4}{3}\pi R^3 \rho
Mass equals volume multiplied by mean density.
2
Substitute mass into the escape velocity formula ve=2GMRv_e = \sqrt{\frac{2GM}{R}}.
ve=2G(43πR3ρ)R=R83πGρv_e = \sqrt{\frac{2G \left(\frac{4}{3}\pi R^3 \rho\right)}{R}} = R\sqrt{\frac{8}{3}\pi G \rho}
This establishes the proportionality veRρv_e \propto R\sqrt{\rho}.
3
Set up the ratio of escape velocity for Planet PP to Planet QQ using RP=12RQR_P = \frac{1}{2}R_Q and ρP=2ρQ\rho_P = 2\rho_Q.
\frac{v_{e,P}}{v_{e,Q}} = \frac{R_P\sqrt{\rho_P}}{R_Q\sqrt{\rho_Q}} = \frac{\left(\frac{1}{2}R_Q\right)\sqrt{2\rho_Q}}{R_Q\sqrt{\rho_Q}} = \frac{1}{2}\sqrt{2} = \frac{1}{\sqrt{2}}
Evaluating the ratio of proportional quantities yields the final scale factor.

Key Concept

Dependence of Escape Velocity on Planet Density and Radius
Estimated Time:2m 0s
Question 7Question

A satellite revolves around a planet in a circular orbit of radius 1.0×104 km1.0 \times 10^4 \text{ km} with an orbital period of 12 hours12 \text{ hours}. Calculate the orbital period, in hours, of a second satellite orbiting the same planet in a circular path of radius 4.0×104 km4.0 \times 10^4 \text{ km}.

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Answer: 96

Answer

96 hours
According to Kepler's Third Law (T2r3T^2 \propto r^3), the orbital period TT scales with radius rr as Tr3/2T \propto r^{3/2}. Increasing the orbital radius by a factor of 4 increases the period by a factor of 43/2=84^{3/2} = 8. Multiplying the original period of 12 hours by 8 yields 96 hours.

Step-by-Step Solution

1
Set up Kepler's Third Law equation relating orbital period and orbital radius.
T22T12=r23r13\frac{T_2^2}{T_1^2} = \frac{r_2^3}{r_1^3}
Kepler's Third Law states that the square of the orbital period of a body in circular orbit is directly proportional to the cube of the radius of its orbit.
2
Substitute the given orbital radii and evaluate the scaling factor.
\frac{r_2}{r_1} = \frac{4.0 \times 10^4 \text{ km}}{1.0 \times 10^4 \text{ km}} = 4
Simplifying the ratio of the two orbital radii gives a factor of 4 increase in radius.
3
Calculate the period multiplier by taking the ratio to the power of 3/2.
4^{3/2} = (\sqrt{4})^3 = 2^3 = 8
Taking T2=T1×(r2r1)3/2T_2 = T_1 \times \left(\frac{r_2}{r_1}\right)^{3/2} shows the period scales by a factor of 8.
4
Multiply the initial orbital period by the scaling factor to find the final answer.
T_2 = 12 \text{ hours} \times 8 = 96 \text{ hours}
Multiplying the baseline period of 12 hours by 8 yields the new orbital period.

Key Concept

Kepler's Third Law of Planetary Motion
Estimated Time:1m 30s
Question 8Question

A satellite of mass 500 kg500\text{ kg} orbits a spherical planet of radius R=6.0×106 mR = 6.0 \times 10^6\text{ m} with surface gravitational acceleration g=10 m/s2g = 10\text{ m/s}^2. The satellite is transferred from an initial circular orbit of radius 2R2R to a higher circular orbit of radius 3R3R. What is the minimum energy required, in megajoules (MJ\text{MJ}), to perform this transfer?

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Answer: 2500

Answer

The minimum energy required to perform the orbital transfer is 2500 MJ2500\text{ MJ}.
The minimum energy needed to move a satellite between circular orbits is equal to the change in its total mechanical energy (E=GMm2rE = -\frac{GMm}{2r}). Expressing GMGM as gR2gR^2, the energy difference between radii 2R2R and 3R3R simplifies to ΔE=gRm12\Delta E = \frac{gRm}{12}, which evaluates to 2500 MJ2500\text{ MJ}.

Step-by-Step Solution

1
Relate surface acceleration due to gravity to planet mass and radius.
GM=gR2GM = gR^2
At the planet's surface (r=Rr = R), gravitational acceleration is g=GMR2g = \frac{GM}{R^2}.
2
Formulate the total mechanical energy equation for a circular orbit.
E=GMm2r=gR2m2rE = -\frac{GMm}{2r} = -\frac{gR^2 m}{2r}
Total energy is kinetic energy GMm2r\frac{GMm}{2r} plus gravitational potential energy GMmr-\frac{GMm}{r}.
3
Calculate initial and final total energies.
E1=gRm4E_1 = -\frac{gRm}{4} and E2=gRm6E_2 = -\frac{gRm}{6}
Substitute the orbit radii r1=2Rr_1 = 2R and r2=3Rr_2 = 3R into the total energy equation.
4
Determine the net work required for the transfer.
ΔE=E2E1=gRm12\Delta E = E_2 - E_1 = \frac{gRm}{12}
The energy required equals the difference in total mechanical energy between the final and initial orbits.
5
Substitute given numerical values and convert joules to megajoules.
ΔE=10×(6.0×106)×50012=2.5×109 J=2500 MJ\Delta E = \frac{10 \times (6.0 \times 10^6) \times 500}{12} = 2.5 \times 10^9\text{ J} = 2500\text{ MJ}
Dividing 2.5×109 J2.5 \times 10^9\text{ J} by 10610^6 converts the value to megajoules.

Key Concept

Total Mechanical Energy of a Satellite in Circular Orbit and Orbital Transfer Energy
Estimated Time:3m 0s
Question 9Question

An astronaut has a weight of 720 N720\text{ N} on the surface of the Earth. Calculate the weight of the astronaut, in Newtons (N\text{N}), at an altitude equal to twice the radius of the Earth (h=2Rh = 2R).

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Answer: 80

Answer

The weight of the astronaut at an altitude of 2R2R is 80 N80\text{ N}.
At an altitude of 2R2R, the total distance from the center of the Earth is r=R+2R=3Rr = R + 2R = 3R. Because gravitational force follows the inverse-square law (W1/r2W \propto 1/r^2), tripling the distance reduces the gravitational force and weight by a factor of 32=93^2 = 9. Dividing the surface weight of 720 N720\text{ N} by 99 yields 80 N80\text{ N}.

Step-by-Step Solution

1
Determine the total distance from the center of the Earth
r=R+2R=3Rr = R + 2R = 3R
Gravitational force depends on the distance measured from the center of mass of the Earth, which is the sum of Earth's radius RR and altitude hh.
2
Apply the inverse-square law of gravitation to find field strength at altitude
g=g32=g9g' = \frac{g}{3^2} = \frac{g}{9}
Acceleration due to gravity is inversely proportional to the square of the distance from the planet's center (g1r2g \propto \frac{1}{r^2}).
3
Calculate the astronaut's weight at altitude
W=7209=80 NW' = \frac{720}{9} = 80\text{ N}
Weight is directly proportional to gravitational field strength (W=mgW = mg).

Key Concept

Variation of Acceleration due to Gravity with Altitude (Inverse Square Law)
Question 10Question

Two point masses of 4.0 kg4.0\text{ kg} and 9.0 kg9.0\text{ kg} are separated by a distance of 5.0 m5.0\text{ m} in free space. At what distance from the 4.0 kg4.0\text{ kg} mass along the line joining them is the net gravitational field strength equal to zero?

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Answer: 2.0 m2.0\text{ m}

Answer

The distance from the 4.0 kg4.0\text{ kg} mass where the net gravitational field strength is zero is 2.0 m2.0\text{ m}.
At the point where the net gravitational field strength is zero, the gravitational field intensity produced by the 4.0 kg4.0\text{ kg} mass must equal the intensity produced by the 9.0 kg9.0\text{ kg} mass in magnitude. Equating G(4.0)x2=G(9.0)(5.0x)2\frac{G (4.0)}{x^2} = \frac{G (9.0)}{(5.0 - x)^2} and taking square roots yields 2x=35x\frac{2}{x} = \frac{3}{5 - x}. Cross-multiplying gives 102x=3x10 - 2x = 3x, which yields x=2.0 mx = 2.0\text{ m} from the 4.0 kg4.0\text{ kg} mass.

Step-by-Step Solution

1
Set up the condition for zero net gravitational field strength.
E1=E2    Gm1x2=Gm2(dx)2E_1 = E_2 \implies \frac{G m_1}{x^2} = \frac{G m_2}{(d - x)^2}
At the neutral point, the opposing gravitational field vectors due to both masses are equal in magnitude.
2
Substitute given values m1=4.0 kgm_1 = 4.0\text{ kg}, m2=9.0 kgm_2 = 9.0\text{ kg}, and total distance d=5.0 md = 5.0\text{ m}.
4.0x2=9.0(5.0x)2\frac{4.0}{x^2} = \frac{9.0}{(5.0 - x)^2}
Simplifying by canceling GG from both sides of the equation.
3
Take the square root of both sides and solve for xx.
\frac{2.0}{x} = \frac{3.0}{5.0 - x} \implies 2.0(5.0 - x) = 3.0x \implies 10.0 - 2.0x = 3.0x \implies 5.0x = 10.0 \implies x = 2.0\text{ m}
Taking the square root simplifies the quadratic relationship into a linear ratio.

Key Concept

Gravitational Field Strength Neutral Point
Estimated Time:1m 0s
Question 11Question

Two satellites, XX and YY, move in circular orbits around a planet with orbital radii of rr and 4r4r, respectively. If satellite XX travels at an orbital speed of vv, what is the orbital speed of satellite YY?

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Answer: v2\frac{v}{2}

Answer

The orbital speed of satellite YY is v2\frac{v}{2}.
The orbital speed vv of a satellite in a circular orbit of radius rr around a planet of mass MM is given by v=GMrv = \sqrt{\frac{GM}{r}}. When the radius increases by a factor of 4 from rr to 4r4r, the new speed becomes vY=GM4r=12GMr=v2v_Y = \sqrt{\frac{GM}{4r}} = \frac{1}{2} \sqrt{\frac{GM}{r}} = \frac{v}{2}.

Step-by-Step Solution

1
Write the formula for orbital speed of a satellite
v=GMrv = \sqrt{\frac{GM}{r}}
Orbital speed depends on the gravitational mass MM of the central body and the orbital radius rr.
2
Set up the ratio between the orbital speeds of satellites YY and XX
vYvX=rXrY\frac{v_Y}{v_X} = \sqrt{\frac{r_X}{r_Y}}
Since GG and MM are constant, orbital speed is inversely proportional to r\sqrt{r}.
3
Substitute the given values rX=rr_X = r, rY=4rr_Y = 4r, and vX=vv_X = v
vY=vr4r=v14=v2v_Y = v \sqrt{\frac{r}{4r}} = v \sqrt{\frac{1}{4}} = \frac{v}{2}
Evaluating the square root yields a factor of 12\frac{1}{2}.

Key Concept

Orbital Speed of a Satellite
Estimated Time:1m 0s
Question 12Question

An object of mass mm is projected vertically upwards from the surface of a spherical planet of radius RR and mass MM with an initial speed equal to half of the planet's escape velocity. Neglecting atmospheric friction, what maximum height above the planet's surface will the object reach?

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Answer: R3\frac{R}{3}

Answer

The maximum height above the planet's surface reached by the object is R3\frac{R}{3}.
By mechanical energy conservation, the initial total energy at launch equals the potential energy at maximum height where velocity is zero. The launch velocity v=12ve=122GMRv = \frac{1}{2}v_e = \frac{1}{2}\sqrt{\frac{2GM}{R}} gives an initial kinetic energy of GMm4R\frac{GMm}{4R}. Combined with initial potential energy GMmR-\frac{GMm}{R}, total energy is 3GMm4R-\frac{3GMm}{4R}. Equating this to GMmR+h-\frac{GMm}{R+h} gives R+h=43RR+h = \frac{4}{3}R, yielding a height above the surface of h=R3h = \frac{R}{3}.

Step-by-Step Solution

1
Express the initial speed in terms of gravitational constant GG, mass MM, and radius RR.
The escape velocity is ve=2GMRv_e = \sqrt{\frac{2GM}{R}}. Thus, launch speed v=12ve=122GMRv = \frac{1}{2}v_e = \frac{1}{2}\sqrt{\frac{2GM}{R}}.
Escape velocity is defined as the minimum speed needed to escape the gravitational field.
2
Calculate the initial total mechanical energy at the planet's surface.
Initial kinetic energy Ki=12mv2=12m(2GM4R)=GMm4RK_i = \frac{1}{2}m v^2 = \frac{1}{2}m\left(\frac{2GM}{4R}\right) = \frac{GMm}{4R}. Surface potential energy Ui=GMmRU_i = -\frac{GMm}{R}. Total energy Ei=Ki+Ui=GMm4RGMmR=3GMm4RE_i = K_i + U_i = \frac{GMm}{4R} - \frac{GMm}{R} = -\frac{3GMm}{4R}.
Total mechanical energy is the sum of kinetic energy and gravitational potential energy.
3
Apply energy conservation to find the maximum distance from the planet's center.
At maximum height hh, speed is zero (Kf=0K_f = 0), so distance from center is r=R+hr = R + h. Energy Ef=GMmR+hE_f = -\frac{GMm}{R+h}. Equating Ei=EfE_i = E_f gives 3GMm4R=GMmR+h    R+h=43R    h=R3-\frac{3GMm}{4R} = -\frac{GMm}{R+h} \implies R+h = \frac{4}{3}R \implies h = \frac{R}{3}.
Mechanical energy is conserved in a central gravitational force field.

Key Concept

Conservation of Mechanical Energy in a Gravitational Field
Estimated Time:1m 30s
Question 13Question

A satellite moves in a circular orbit of radius 2R2R around a spherical planet of radius RR and mass MM. It is subsequently shifted to a larger circular orbit of radius 8R8R. What is the ratio of its initial orbital speed to its new orbital speed?

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Answer: 2:12 : 1

Answer

The ratio of the initial orbital speed to the new orbital speed is 2:12 : 1.
Orbital velocity varies inversely with the square root of orbital radius (v1rv \propto \frac{1}{\sqrt{r}}). Moving from radius 2R2R to 8R8R decreases the speed by a factor of 8/2=2\sqrt{8/2} = 2. Therefore, the ratio of initial speed to new speed is 2:12 : 1.

Step-by-Step Solution

1
Write the formula for orbital velocity
v=GMrv = \sqrt{\frac{GM}{r}}, where GG is the gravitational constant, MM is the mass of the planet, and rr is the orbital radius.
Orbital speed is determined by equating gravitational force to centripetal force.
2
Set up expressions for initial and final orbital speeds
Initial speed v1=GM2Rv_1 = \sqrt{\frac{GM}{2R}} and final speed v2=GM8Rv_2 = \sqrt{\frac{GM}{8R}}.
Substitute the given orbital radii r1=2Rr_1 = 2R and r2=8Rr_2 = 8R into the formula.
3
Calculate the ratio v1/v2v_1 / v_2
\frac{v_1}{v_2} = \frac{\sqrt{\frac{GM}{2R}}}{\sqrt{\frac{GM}{8R}}} = \sqrt{\frac{8R}{2R}} = \sqrt{4} = 2
Simplifying the square root fraction gives the exact ratio.

Key Concept

Orbital Velocity and Inverse Square Law Relations
Estimated Time:1m 15s
Question 14Question

Two point masses, each of mass 125 kg125\text{ kg}, are fixed at positions (3.0 m,0)(-3.0\text{ m}, 0) and (3.0 m,0)(3.0\text{ m}, 0) in the xyxy-plane. What is the magnitude of the net gravitational field strength at a point PP located at (0,4.0 m)(0, 4.0\text{ m}), in terms of the universal gravitational constant GG?

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Answer: 8.0G N/kg8.0G\text{ N/kg}

Answer

The magnitude of the net gravitational field strength at point PP is 8.0G N/kg8.0G\text{ N/kg}.
The distance from each mass to the target point is 5.0 m, yielding an individual field magnitude of 5.0G N/kg. Resolving vectors shows that horizontal components cancel out while vertical components add to give 2 × (5.0G × 4/5) = 8.0G N/kg.

Step-by-Step Solution

1
Calculate the distance rr from each mass to point P(0,4.0 m)P(0, 4.0\text{ m}).
r=(3.00)2+(04.0)2=9+16=5.0 mr = \sqrt{(-3.0 - 0)^2 + (0 - 4.0)^2} = \sqrt{9 + 16} = 5.0\text{ m}.
The distance formula in two dimensions gives the hypotenuse of the right triangle formed by the coordinates.
2
Determine the magnitude of the gravitational field EE created by each individual mass at point PP.
E=GMr2=G×1255.02=125G25=5.0G N/kgE = \frac{G M}{r^2} = \frac{G \times 125}{5.0^2} = \frac{125G}{25} = 5.0G\text{ N/kg}.
Newton's law of universal gravitation defines field strength as E=GMr2E = \frac{GM}{r^2}.
3
Resolve the field vectors into horizontal and vertical components.
By symmetry, the horizontal components Ex=EsinθE_x = E \sin\theta are equal in magnitude and opposite in direction, so Ex,net=0E_{x,\text{net}} = 0. The vertical components Ey=EcosθE_y = E \cos\theta point downwards towards the origin.
Gravitational field is a vector quantity, so opposite components cancel while aligned components add together.
4
Calculate the total vertical component of the net gravitational field.
cosθ=4.05.0=0.8\cos\theta = \frac{4.0}{5.0} = 0.8. Thus, Enet=2×Ey=2×(5.0G×0.8)=8.0G N/kgE_{\text{net}} = 2 \times E_y = 2 \times (5.0G \times 0.8) = 8.0G\text{ N/kg}.
Summing the vertical contributions from both identical masses gives the net magnitude.

Key Concept

Vector Addition of Gravitational Field Strengths
Question 15Question

A planet has a mass equal to 88 times the mass of the Earth and a radius equal to 22 times the radius of the Earth. If the acceleration due to gravity on the surface of the Earth is 10 m/s210\text{ m/s}^2, what is the acceleration due to gravity on the surface of the planet in m/s2\text{m/s}^2?

Show answer & explanation

Answer: 20

Answer

The acceleration due to gravity on the surface of the planet is 20 m/s220\text{ m/s}^2.
The acceleration due to gravity at the surface of a spherical body is given by g=GMR2g = \frac{GM}{R^2}. When the mass is multiplied by 88 and the radius is multiplied by 22, the new acceleration becomes gp=G(8M)(2R)2=84GMR2=2gg_p = \frac{G(8M)}{(2R)^2} = \frac{8}{4}\frac{GM}{R^2} = 2g. Substituting g=10 m/s2g = 10\text{ m/s}^2 gives 20 m/s220\text{ m/s}^2.

Step-by-Step Solution

1
Write the expression for acceleration due to gravity at the surface of Earth.
ge=GMeRe2=10 m/s2g_e = \frac{GM_e}{R_e^2} = 10\text{ m/s}^2
Gravitational field strength at the surface depends directly on body mass and inversely on the square of radius.
2
Set up the ratio equation for the planet's gravitational acceleration using relative mass and radius values.
gp=G(8Me)(2Re)2=84(GMeRe2)=2geg_p = \frac{G(8M_e)}{(2R_e)^2} = \frac{8}{4} \left(\frac{GM_e}{R_e^2}\right) = 2g_e
Squaring the radius multiplier of 22 yields 44 in the denominator, while the numerator increases by a factor of 88.
3
Calculate the final numeric value.
gp=2×10 m/s2=20 m/s2g_p = 2 \times 10\text{ m/s}^2 = 20\text{ m/s}^2
Multiplying Earth's value by the combined ratio of 22 gives the answer.

Key Concept

Gravitational field strength on planetary surfaces (g=GMR2g = \frac{GM}{R^2})
Gravitational Field and Orbits Practice Questions — JAMB UTME | Examkin