Initially a satellite of 100 kg is in a circular orbit of radius 1.5RE$1.5R_{E}$. This satellite can be moved to a circular orbit of radius 3RE$3R_{E}$ by supplying α × 10⁶J$\alpha \times 10^{6}J$ of energy. The value of α$\alpha$ is ____.
(Take Radius of Earth RE = 6 × 10⁶ m$R_{E} = 6 \times 10^{6}\text{ m}$ and g = 10 m/s²$g = 10\text{ m/s}^{2}$)
A.150
B.500
C.100
D.1000
Solution & Explanation
Related Formula
E = (-GME m)/(2r)$$E = \frac{-GM_E m}{2r}$$Δ E = Ef - Eᵢ$$\Delta E = E_f - E_i$$g = (GME)/(RE²) GME = g RE²$$g = \frac{GM_E}{R_E^2} \implies GM_E = g R_E^2$$
Core Logic
Energy of a satellite in a circular orbit is given as E = (-GME m)/(2r)$E = \frac{-GM_E m}{2r}$ where r is the radius of the circular orbit.
Required energy to be supplied Δ E = Ef - Eᵢ$\Delta E = E_f - E_i$:
Substitute GME = g RE²$GM_E = g R_E^2$ into the expression:
Δ E = ((g RE²) m)/(6RE) = (1)/(6) m g RE$$\Delta E = \frac{(g R_E^2) m}{6R_E} = \frac{1}{6} m g R_E$$= (1)/(6) × 100 × 10 × (6 × 10⁶)$$= \frac{1}{6} \times 100 \times 10 \times (6 \times 10^6)$$= 1000 × 10⁶ J$$= 1000 \times 10^6\text{ J}$$
Comparing with α × 10⁶ J$\alpha \times 10^6\text{ J}$, we get α = 1000$\alpha = 1000$.
Pattern Recognition
Orbital transition energy is always Δ E = (GMm)/(2) ((1)/(rᵢ) - (1)/(rf))$\Delta E = \frac{GMm}{2} (\frac{1}{r_i} - \frac{1}{r_f})$. Never forget the factor of 2 in the denominator (which accounts for kinetic energy contribution in orbit).
Keywords:#Initially a satellite of 100 kg#JEE Main 2026 Morning Q44#Gravitation JEE Main 2026#Satellite Energy JEE Main 2026
More Gravitation Previous-Year Questions — Page 5
Q46jee_main_2024_31_jan_eveningEscape Velocity
The mass of the moon is 1/144$1/144$ times the mass of a planet and its diameter 1/16$1/16$ times the diameter of a planet. If the escape velocity on the planet is v, the escape velocity on the moon will be:
For the planet: v = √((2GMₚ)/(Rₚ))$v = \sqrt{\frac{2GM_p}{R_p}}$
For the moon: Mm = (Mₚ)/(144)$M_m = \frac{M_p}{144}$ and Rm = (Rₚ)/(16)$R_m = \frac{R_p}{16}$.
Four identical particles of mass m$m$ are kept at the four corners of a square. If the gravitational force exerted on one of the masses by the other masses is ( 2√(2) + 132) Gm²L²$\left(\frac{2\sqrt{2} + 1}{32}\right)\frac{\mathrm{Gm}^2}{\mathrm{L}^2}$, the length of the sides of the square is
A.L2$\frac{\mathrm{L}}{2}$
B.4 L$4 L$
C.3L$3L$
D.2 L$2 L$
Solution
Related Formula
F = (G m₁ m₂)/(r²)$$F = \frac{G m_1 m_2}{r^2}$$
Core Logic
Superposition Principle diagram for Q37 - JEE Main 2024 Morning
Let the side length of the square be a$a$. Considering one corner mass, it experiences forces from the adjacent two masses (distance a$a$) and the diagonally opposite mass (distance √(2)a$\sqrt{2}a$).
The forces from the two adjacent masses are at 90^°$90^\circ$ to each other:
F = (Gm²)/(a²)$$F = \frac{Gm^2}{a^2}$$
The resultant of these two is √(2)F = √(2) (Gm²)/(a²)$\sqrt{2}F = \sqrt{2} \frac{Gm^2}{a^2}$, directed along the diagonal.
Step 2: Total Force Equation
The force from the diagonal mass is:
F' = Gm²(√(2)a)² = (Gm²)/(2a²)$$F' = \frac{Gm^2}{(\sqrt{2}a)^2} = \frac{Gm^2}{2a^2}$$
Total resultant force Fₙₑₜ = √(2)F + F'$F_{\text{net}} = \sqrt{2}F + F'$:
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