MCQMediumJEE 2026Satellites & Orbital Velocity

JEE Physics 2026 Question with Solution

Initially a satellite of 100kg100 \, \text{kg} is in a circular orbit of radius 1.5RE1.5R_E. This satellite can be moved to a circular orbit of radius 3RE3R_E by supplying a×106Ja \times 10^6 \, \text{J} of energy. The value of aa is _____ . (Take Radius of Earth RE=6×106mR_E = 6 \times 10^6 \, \text{m} and g=10m/s2g = 10 \, \text{m/s}^2).

  • A

    10001000

  • B

    150150

  • C

    100100

  • D

    500500

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: Satellite mass is 100kg100 \, \text{kg}. Initial orbit radius is r1=1.5REr_1 = 1.5R_E and final orbit radius is r2=3REr_2 = 3R_E. Also, RE=6×106mR_E = 6 \times 10^6 \, \text{m} and g=10m/s2g = 10 \, \text{m/s}^2.

Find: The value of aa in the energy expression a×106Ja \times 10^6 \, \text{J}.

For a satellite in a circular orbit, the total mechanical energy is

E=GMm2rE = -\frac{GMm}{2r}

Using g=GMRE2g = \frac{GM}{R_E^2}, we get

GM=gRE2GM = gR_E^2

So the energy can be written as

E=gRE2m2rE = -\frac{gR_E^2 m}{2r}

Initial energy for r1=1.5REr_1 = 1.5R_E is

E1=gRE2m2(1.5RE)=gREm3E_1 = -\frac{gR_E^2 m}{2(1.5R_E)} = -\frac{gR_E m}{3}

Final energy for r2=3REr_2 = 3R_E is

E2=gRE2m2(3RE)=gREm6E_2 = -\frac{gR_E^2 m}{2(3R_E)} = -\frac{gR_E m}{6}

Energy supplied is the increase in total energy:

ΔE=E2E1\Delta E = E_2 - E_1 ΔE=(gREm6)(gREm3)\Delta E = \left(-\frac{gR_E m}{6}\right) - \left(-\frac{gR_E m}{3}\right) ΔE=gREm(16+13)=gREm6\Delta E = gR_E m\left(-\frac{1}{6} + \frac{1}{3}\right) = \frac{gR_E m}{6}

Substituting the values:

ΔE=(10)(6×106)(100)6\Delta E = \frac{(10)(6 \times 10^6)(100)}{6} ΔE=1000×106J\Delta E = 1000 \times 10^6 \, \text{J}

Comparing with a×106Ja \times 10^6 \, \text{J}, we get a=1000a = 1000.

Therefore, the correct option is A.

Energy Change Interpretation

Given: The satellite is moved from a lower circular orbit to a higher circular orbit.

Find: Whether energy must be supplied and how much.

The total energy of a satellite in orbit is negative. When the orbital radius increases, the total energy becomes less negative. That means the satellite gains energy, so external energy must be supplied.

Using

E=GMm2rE = -\frac{GMm}{2r}

a larger value of rr gives a numerically smaller negative value. Hence E2>E1E_2 > E_1, and the required supplied energy is positive:

ΔE=E2E1>0\Delta E = E_2 - E_1 > 0

Evaluating this gives

ΔE=gREm6=1000×106J\Delta E = \frac{gR_E m}{6} = 1000 \times 10^6 \, \text{J}

So the required value is a=1000a = 1000.

Common mistakes

  • Using gravitational potential energy alone instead of total mechanical energy. For a circular orbit, the required change must be found from total energy E=GMm2rE = -\frac{GMm}{2r}, not only from U=GMmrU = -\frac{GMm}{r}.

  • Assuming energy decreases when the satellite moves higher because the formula is negative. In fact, the energy becomes less negative, so ΔE\Delta E is positive and energy must be supplied.

  • Substituting GMGM incorrectly. From g=GMRE2g = \frac{GM}{R_E^2}, we get GM=gRE2GM = gR_E^2. Missing one factor of RER_E gives an incorrect result.

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