Net gravitational force at the centre of a square is found to be F₁$F_{1}$ when four particles having mass M, 2M, 3M and 4M are placed at the four corners of the square as shown in figure and it is F₂$F_{2}$ when the positions of 3M and 4M are interchanged. The ratio F₁F₂$\frac{F_{1}}{F_{2}}$ is α√(5)$\frac{\alpha}{\sqrt{5}}$. The value of α$\alpha$ is \_\_\_\_.
Four point masses placed at the corners of a square.
A.2
B.3
C.1
D.2√(5)$2\sqrt{5}$
Solution & Explanation
Related Formula
F = (G m₁ m₂)/(r²)$$F = \frac{G m_1 m_2}{r^2}$$
Core Logic
Four point masses placed at the corners of a square.
Initial configuration:
F₁ = 2√(2) (Gmm₀)/(r²)$|
New configuration (after interchanging 3M and 4M):
$$F_1 = 2\sqrt{2} \frac{Gmm_0}{r^2}$|
New configuration (after interchanging 3M and 4M):
Sees: Gravitational force vector sum at center of square.
Shortcut: Compute net vector resultants for both mass configurations and take ratio.
Check: Matches option (1). ✓
Chapter Mix
Class 11 Physics: Gravitation
Four point masses placed at the corners of a square.Four point masses placed at the corners of a square.Four point masses placed at the corners of a square.
Keywords:#Net gravitational force at the centre of a square is found#JEE Main 2026 Morning Q35#Gravitation JEE Main 2026#Gravitational Force and Superposition JEE Main 2026#square#masses#gravitational force#centre
More Gravitation Previous-Year Questions — Page 5
Q46jee_main_2024_31_jan_eveningEscape Velocity
The mass of the moon is 1/144$1/144$ times the mass of a planet and its diameter 1/16$1/16$ times the diameter of a planet. If the escape velocity on the planet is v, the escape velocity on the moon will be:
For the planet: v = √((2GMₚ)/(Rₚ))$v = \sqrt{\frac{2GM_p}{R_p}}$
For the moon: Mm = (Mₚ)/(144)$M_m = \frac{M_p}{144}$ and Rm = (Rₚ)/(16)$R_m = \frac{R_p}{16}$.
Four identical particles of mass m$m$ are kept at the four corners of a square. If the gravitational force exerted on one of the masses by the other masses is ( 2√(2) + 132) Gm²L²$\left(\frac{2\sqrt{2} + 1}{32}\right)\frac{\mathrm{Gm}^2}{\mathrm{L}^2}$, the length of the sides of the square is
A.L2$\frac{\mathrm{L}}{2}$
B.4 L$4 L$
C.3L$3L$
D.2 L$2 L$
Solution
Related Formula
F = (G m₁ m₂)/(r²)$$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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