Class 11th
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New answer posted
2 months agoContributor-Level 10
(0.16)^log? (1/3 + 1/3² + . to ∞)
= (4/25)^log? (1/2)
= ( (5/2)? ² )^log? /? (1/2) = (5/2)^ (-2 log? /? (1/2)
= (5/2)^ (log? /? ( (1/2)? ² ) = 4
New answer posted
2 months agoContributor-Level 10
By the principle of conservation of angular momentum, the total angular momentum of the system (platform + person) remains constant.
L_initial = L_final
I_initial * ω_initial = I_final * ω_final
Initial state: Person is on the rim.
I_initial = I_platform + I_person_rim = (1/2)M_platform R² + M_person R²
Final state: Person is at the center.
I_final = I_platform + I_person_center = (1/2)M_platform R² + 0
[ (1/2) (200)R² + (80)R²] * 5 rpm = [ (1/2) (200)R²] * ω_final
(100R² + 80R²) * 5 = (100R²) * ω_final
180R² * 5 = 100R² * ω_final
ω_final = (180 * 5) / 100 = 9 rpm.
New answer posted
2 months agoContributor-Level 10
lim_ (x→0) (1/x? ) {1 - cos (x²/2) - cos (x²/4) + cos (x²/2)cos (x²/4)} = 2?
⇒ lim_ (x→0) ( (1 - cos (x²/2) (1 - cos (x²/4) / x? ) = 2?
⇒ 2? = 2? ⇒ k = 8
New answer posted
2 months agoContributor-Level 10
∴ center lies on x + y = 2 and in 1st quadrant center = (a, 2-a) where a > 0 and 2-a > 0 ⇒ 0 < a < 2
∴ circle touches x = 3 and y = 2
⇒ |3-a| = |2 - (2-a)| = radius
⇒ |3-a| = |a| ⇒ a = 3/2
∴ radius = a
⇒ Diameter = 2a = 3.
New answer posted
2 months agoContributor-Level 10
After burning, heat exchange occurs between helium and atmospheric. Hence, irreversible, isothermal process.
New answer posted
2 months agoContributor-Level 10
S = (2 . ¹P? - 3 . ²P? + 4 . ³P? upto 51 terms) + (1! - 2! + 3! - . upto 51 terms)
∴ [? ? P_ (n-1) = n!]
= (2! - 3! + 4! + 52!) + (1! - 2! + 3! - 4! + . . + (51)!)
= 1! + 52!
New answer posted
2 months agoContributor-Level 10
LHL : lim_ (x→0? ) |1-x-x|/|λ-x-1| = 1/|λ-1|
RHL: lim_ (x→0? ) |1-x+x|/|λ-x+0| = 1/|λ|
For existence of limit
LHL = RHL
⇒ 1/|λ-1| = 1/|λ| ⇒ λ = 1/2
∴ L = 1/|λ| = 2
New answer posted
2 months agoContributor-Level 10
The mass of the cylinder M = ρV = ρ (πR²L), where ρ is the density of the material.
We can express R² in terms of L: R² = M / (πρL).
The moment of inertia is I = M (R²/4 + L²/12).
Substitute R² into the equation for I:
I (L) = M * [ (M / (4πρL) + (L²/12) ]
To find the minimum possible I, we differentiate I with respect to L and set the derivative to zero.
dI/dL = M * [ -M/ (4πρL²) + 2L/12 ] = 0
M/ (4πρL²) = 2L/12 = L/6
M/ (πρ) = (4/6)L³ = (2/3)L³
Since R² = M/ (πρL), we have R²L = M/ (πρ).
Substitute M/ (πρ) into the differentiated equation:
R²L = (2/3)L³
New answer posted
2 months agoContributor-Level 10
T_r+1 =? C_r (3)^ (n-r)/2) (5)^ (r/8) (n ≥ r)
Clearly r should be a multiple of 8.
∴ there are exactly 33 integral terms
Possible values of r can be
0,8,16, . . .,32 * 8
∴ least value of n = 256
New answer posted
2 months agoContributor-Level 10
Sum of 1st 25 terms = sum of its next 15 terms
? (T? + . + T? ) = (T? + . + T? )
? (T? + . + T? ) = 2 (T? + . + T? )
? 40/2 [2*3 + (39d)] = 2 * 25/2 [2*2 + 24 d]
? d = 1/6
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