The electronic configuration corresponds to C2, which has a tetrahedral geometry due to sp3 hybridization.

The correct configuration for F2 is (σ1s)²(σ*1s)²(σ2s)²(σ*2s)²(σ2p)²(π2p)⁴(π*2p)².

The correct configuration for O2 is (σ1s)²(σ*1s)²(σ2s)²(σ*2s)²(σ2p)²(π2p)²(π*2p)¹.

The correct configuration for F2 is (σ1s)²(σ*1s)²(σ2s)²(σ*2s)²(σ2p)²(π2p)⁴(π*2p)².

The correct configuration for O2 is (σ1s)²(σ*1s)²(σ2s)²(σ*2s)²(σ2p)²(π2p)²(π*2p)¹.

AX3E indicates three bonding pairs and one lone pair, resulting in a trigonal pyramidal shape.

BF3 has three bonding pairs and no lone pairs, resulting in a trigonal planar shape.

NH3 has three bonding pairs and one lone pair, resulting in a trigonal pyramidal shape.

The molecular weight of water is calculated as (2*1) + (16) = 18 g/mol.

The moment of inertia of a disk about an axis through its center is I = 1/2 MR^2.

The moment of inertia of a solid cylinder about its central axis is given by I = 1/2 MR^2.

The moment of inertia of a solid disk about its central axis is (1/2)MR^2.

The moment of inertia of a solid sphere about an axis through its center is given by I = (2/5)mr^2.

The moment of inertia of a solid sphere about an axis through its center is I = 2/5 MR^2.

The moment of inertia of a thin circular hoop about an axis through its center is I = MR^2.

The moment of inertia of a thin circular plate about an axis through its center is I = 1/2 MR^2.

The moment of inertia of a thin circular ring about an axis through its center is I = MR^2.

The moment of inertia of a thin circular ring about an axis through its center is I = MR^2.

The moment of inertia of a thin circular ring about an axis through its center is I = MR^2.

The moment of inertia of a thin circular ring about an axis through its center is I = MR^2.

The moment of inertia of a thin rod about an axis through its center is given by I = (1/12)ML^2.

The moment of inertia of a thin rod about an end is given by I = (1/3)ML^2.

The moment of inertia of a thin spherical shell about an axis through its center is I = 2/3 MR^2.

The moment of inertia of a thin wire bent in the shape of a semicircle about the diameter is I = 3/8 MR^2.

The moment of inertia of a rectangular plate about an axis through its center and parallel to side a is I = 1/3 Mb^2.

The moment of inertia of a uniform thin circular plate about an axis through its center and perpendicular to its plane is I = 1/2 MR^2.

The moment of inertia of a square plate about an axis through its center and parallel to one side is I = 1/12 Ma².

The moment of inertia of a triangular lamina about an axis through its centroid is I = 1/12 Mb^2.

Momentum (p) = mass × velocity = 3 kg × 4 m/s = 12 kg·m/s.

Nucleotides are the monomers that make up nucleic acids.