Given the parametric equations:
π₯
1
β
π‘
2
,
π¦
1
+
π‘
x=1βt
2
,y=1+t
We are to find:
π
π¦
π
π₯
dx
dy
β
β the first derivative of
π¦
y with respect to
π₯
x,
π
2
π¦
π
π₯
2
dx
2
d
2
y
β
β the second derivative of
π¦
y with respect to
π₯
x,
without eliminating the parameter.
Step 1: First Derivative
π
π¦
π
π₯
dx
dy
β
Using parametric differentiation, the first derivative is given by:
π
π¦
π
π₯
π
π¦
π
π‘
π
π₯
π
π‘
dx
dy
β
=
dt
dx
β
dt
dy
β
β
Differentiate
π₯
x and
π¦
y with respect to
π‘
t:
π
π₯
π
π‘
π
π
π‘
(
1
β
π‘
2
)
β
2
π‘
dt
dx
β
=
dt
d
β
(1βt
2
)=β2t
π
π¦
π
π‘
π
π
π‘
(
1
+
π‘
)
1
dt
dy
β
=
dt
d
β
(1+t)=1
So,
π
π¦
π
π₯
1
β
2
π‘
β
1
2
π‘
dx
dy
β
=
β2t
1
β
=β
2t
1
β
Step 2: Second Derivative
π
2
π¦
π
π₯
2
dx
2
d
2
y
β
The second derivative in parametric form is given by:
π
2
π¦
π
π₯
2
π
π
π‘
(
π
π¦
π
π₯
)
Γ·
π
π₯
π
π‘
dx
2
d
2
y
β
=
dt
d
β
(
dx
dy
β
)Γ·
dt
dx
β
We already have
π
π¦
π
π₯
β
1
2
π‘
dx
dy
β
=β
2t
1
β
, so compute its derivative with respect to
π‘
t:
π
π
π‘
(
β
1
2
π‘
)
1
2
π‘
2
dt
d
β
(β
2t
1
β
)=
2t
2
1
β
Now divide by
π
π₯
π
π‘
β
2
π‘
dt
dx
β
=β2t:
π
2
π¦
π
π₯
2
1
2
π‘
2
β
2
π‘
β
1
4
π‘
3
dx
2
d
2
y
β
=
β2t
2t
2
1
β
β
=β
4t
3
1
β
Final Answers:
π
π¦
π
π₯
β
1
2
π‘
,
π
2
π¦
π
π₯
2
β
1
4
π‘
3
dx
dy
β
=β
2t
1
β
,
dx
2
d
2
y
β
=β
4t
3
1
β
Explanation (300 words):
When working with parametric equations, such as
π₯
1
β
π‘
2
x=1βt
2
and
π¦
1
+
π‘
y=1+t, we treat both
π₯
x and
π¦
y as functions of a third variable
π‘
t, known as the parameter. Instead of expressing
π¦
y directly in terms of
π₯
x, we differentiate each with respect to
π‘
t, and use these derivatives to find the derivatives of
π¦
y with respect to
π₯
x.
To find the first derivative
π
π¦
π
π₯
dx
dy
β
, we apply the chain rule of calculus. Since
π
π¦
/
π
π₯
(
π
π¦
/
π
π‘
)
/
(
π
π₯
/
π
π‘
)
dy/dx=(dy/dt)/(dx/dt), we compute the derivatives:
π
π¦
/
π
π‘
1
dy/dt=1, since
π¦
1
+
π‘
y=1+t,
π
π₯
/
π
π‘
β
2
π‘
dx/dt=β2t, because
π₯
1
β
π‘
2
x=1βt
2
.
Substituting, we get
π
π¦
π
π₯
1
β
2
π‘
β
1
2
π‘
dx
dy
β
=
β2t
1
β
=β
2t
1
β
.
To find the second derivative
π
2
π¦
π
π₯
2
dx
2
d
2
y
β
, we use the formula:
π
2
π¦
π
π₯
2
π
π
π‘
(
π
π¦
π
π₯
)
Γ·
π
π₯
π
π‘
dx
2
d
2
y
β
=
dt
d
β
(
dx
dy
β
)Γ·
dt
dx
β
This involves differentiating
β
1
2
π‘
β
2t
1
β
with respect to
π‘
t, which gives
1
2
π‘
2
2t
2
1
β
, and then dividing this result by
β
2
π‘
β2t, the derivative of
π₯
x. Thus:
π
2
π¦
π
π₯
2
1
2
π‘
2
β
2
π‘
β
1
4
π‘
3
dx
2
d
2
y
β
=
β2t
2t
2
1
β
β
=β
4t
3
1
β
This process allows us to compute the derivatives directly from the parametric equations without needing to eliminate the parameter.

The Correct Answer and Explanation is:
Completed Chemistry Worksheet: Exceptions to the Octet Rule
| Molecule or Ion | Lewis Structure | Formula Type | Molecular Shape (Description) | Shape Name (Molecular Geometry) | Polarity – if polar show dipoles |
| Iββ» | [ :Γ β Γ β Γ: ]β» (Central I has 3 lone pairs) | AXβEβ | The central Iodine atom is bonded to two other Iodine atoms in a straight line, with three lone pairs arranged in a plane around the central atom’s equator. | Linear | Nonpolar (The symmetrical arrangement of atoms causes the dipoles to cancel.) |
| PClββ» | [P bonded to 6 Cl]β» (P has no lone pairs) | AXβ | A central Phosphorus atom is bonded to six Chlorine atoms, with four in a square plane and one above and one below the plane. | Octahedral | Nonpolar (The symmetrical octahedral geometry causes all bond dipoles to cancel out.) |
| SFβ | S bonded to 4 F (S has one lone pair) | AXβEβ | A central Sulfur atom is bonded to four Fluorine atoms. The lone pair on the sulfur atom pushes the bonds away, creating a shape that resembles a seesaw. | Seesaw | Polar (The shape is asymmetrical due to the lone pair. There is a net dipole moment pointing towards the fluorine atoms.) |
| BFβ | B bonded to 3 F (B has an incomplete octet) | AXβ | A central Boron atom is bonded to three Fluorine atoms, all lying in the same plane and spaced 120Β° apart. | Trigonal Planar | Nonpolar (The symmetrical arrangement of the B-F bonds in a plane causes the dipoles to cancel.) |
| ClFβ | Cl bonded to 3 F (Cl has two lone pairs) | AXβEβ | A central Chlorine atom is bonded to three Fluorine atoms. Two lone pairs on the chlorine push the bonds into a T-shape. | T-shaped | Polar (The shape is asymmetrical. The bond dipoles do not cancel, resulting in a net dipole moment along the stem of the ‘T’.) |
| ClFββ» | [Cl bonded to 4 F]β» (Cl has two lone pairs) | AXβEβ | A central Chlorine atom is bonded to four Fluorine atoms that lie in a single plane. Two lone pairs are located above and below this plane. | Square Planar | Nonpolar (Although the bonds are polar, the symmetrical arrangement of the four Fluorine atoms around the central Chlorine causes their dipoles to cancel out.) |
| XeFβ | Xe bonded to 2 F (Xe has three lone pairs) | AXβEβ | A central Xenon atom is bonded to two Fluorine atoms. Three lone pairs on the Xenon atom are arranged in a plane, forcing the Fluorine atoms to opposite sides. | Linear | Nonpolar (The two Xe-F bonds are on opposite sides of the central atom, so their dipoles are equal and opposite, and they cancel out.) |
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