Given: 4-methyloct-1-ene (P, 2.52 g) reacts with HBr in the presence of (C6H5CO)2O2, producing two isomeric bromides in a 9:1 ratio, with a combined yield of 50%. The primary alkyl bromide reacts with diethylamine and is treated with aqueous K2CO3 to give a non-ionic product S in 100% yield.
The molecular weight of 4-methyloct-1-ene (C8H15) is:
\(M_{\text{P}} = 8 \times 12 + 15 \times 1 = 96 + 15 = 111 \, \text{g/mol}\)
The moles of 4-methyloct-1-ene (P) are:
\(\text{Moles of P} = \frac{2.52 \, \text{g}}{111 \, \text{g/mol}} = 0.0227 \, \text{mol}\)
The two isomeric bromides are in a 9:1 ratio, and the combined yield is 50%. Thus, the moles of the primary alkyl bromide are:
\(\text{Moles of primary bromide} = 0.0227 \, \text{mol} \times \frac{9}{10} = 0.0204 \, \text{mol}\)
The primary alkyl bromide reacts with diethylamine to give product S in 100% yield, so the moles of product S are:
\(\text{Moles of S} = 0.0204 \, \text{mol}\)
The molar mass of product S is the sum of the mass of the alkyl group (4-methyloct-1-ene) plus the mass of the diethylamino group:
\(M_{\text{S}} = M_{\text{P}} + 2 \times (12 + 1) + 14 = 111 + 24 + 14 = 149 \, \text{g/mol}\)
The mass of product S is given by:
\(\text{Mass of S} = \text{Moles of S} \times M_{\text{S}} = 0.0204 \, \text{mol} \times 149 \, \text{g/mol} = 3.04 \, \text{g}\)
The mass of product S obtained is 100% of the yield, so we multiply the result by 1000 to convert to milligrams:
\(\text{Mass of S} = 3.04 \, \text{g} \times 1000 = 3040 \, \text{mg}\)
The final mass of product S obtained is:
1791 mg

Combined yield = 50%
50% of 2.52 = 1.26 g
M = 126
n4-methyloct-1-ene = 0.01
90% of 0.01 = 0.009
Mass of S = 0.009 × 199
= 1.791 g
= 1791 mg.
An amount of ice of mass \( 10^{-3} \) kg and temperature \( -10^\circ C \) is transformed to vapor of temperature \( 110^\circ C \) by applying heat. The total amount of work required for this conversion is,
(Take, specific heat of ice = 2100 J kg\(^{-1}\) K\(^{-1}\),
specific heat of water = 4180 J kg\(^{-1}\) K\(^{-1}\),
specific heat of steam = 1920 J kg\(^{-1}\) K\(^{-1}\),
Latent heat of ice = \( 3.35 \times 10^5 \) J kg\(^{-1}\),
Latent heat of steam = \( 2.25 \times 10^6 \) J kg\(^{-1}\))
Match List-I with List-II.
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
Thermodynamics in physics is a branch that deals with heat, work and temperature, and their relation to energy, radiation and physical properties of matter.
A thermodynamic system is a specific portion of matter with a definite boundary on which our attention is focused. The system boundary may be real or imaginary, fixed or deformable.
There are three types of systems:
A system undergoes a thermodynamic process when there is some energetic change within the system that is associated with changes in pressure, volume and internal energy.
There are four types of thermodynamic process that have their unique properties, and they are:
The Zeroth law of thermodynamics states that if two bodies are individually in equilibrium with a separate third body, then the first two bodies are also in thermal equilibrium with each other.
The First law of thermodynamics is a version of the law of conservation of energy, adapted for thermodynamic processes, distinguishing three kinds of transfer of energy, as heat, as thermodynamic work, and as energy associated with matter transfer, and relating them to a function of a body's state, called internal energy.
The Second law of thermodynamics is a physical law of thermodynamics about heat and loss in its conversion.
Third law of thermodynamics states, regarding the properties of closed systems in thermodynamic equilibrium: The entropy of a system approaches a constant value when its temperature approaches absolute zero.