prove that LHS equals RHS
please help me only a mastermind can solv it it's my challenge

Answer:
See below
Step-by-step explanation:
We'll start with the left-hand side (LHS) and manipulate it to arrive at the right-hand side (RHS).
LHS:
[tex]\sf \sec^2(\theta) \left(1 - \dfrac{\sin^2(\theta)}{\sin^2(A)}\right) [/tex]
Express [tex]\sf \sec^2(\theta) [/tex] in terms of [tex]\sf \sin^2(\theta) [/tex] and [tex]\sf \cos^2(\theta) [/tex]:
[tex]\sf = \dfrac{1}{\cos^2(\theta)} \left(1 - \dfrac{\sin^2(\theta)}{\sin^2(A)}\right) [/tex]
Distribute the [tex]\sf \dfrac{1}{\cos^2(\theta)} [/tex] term:
[tex]\sf = \dfrac{1}{\cos^2(\theta)} - \dfrac{\sin^2(\theta)}{\cos^2(\theta)\sin^2(A)} [/tex]
Rewrite [tex]\sf \dfrac{\sin^2(\theta)}{\cos^2(\theta)} [/tex] as [tex]\sf \tan^2(\theta) [/tex]:
[tex]\sf = \dfrac{1}{\cos^2(\theta)} - \dfrac{\tan^2(\theta)}{\sin^2(A)} [/tex]
Express [tex]\sf \dfrac{1}{\cos^2(\theta)} [/tex] as [tex]\sf 1 + \tan^2(\theta) [/tex]:
Here is how it becomes: we know that:
[tex]\sf sin^2 \theta + cos^2 \theta = 1 [/tex]
using this,
[tex]\boxed{\boxed{\begin{aligned} \dfrac{1}{cos^2 \theta } & = \dfrac{sin^2 \theta + cos^2 \theta}{ cos^2 \theta } \\\\ & = \dfrac{sin^2\theta }{cos^2 \theta } + \dfrac{cos^2\theta }{cos^2 \theta } \\\\ & = tan^2\theta + 1 \\\\ & = 1+ tan^2\theta \end{aligned}}}[/tex]
Replace the value of [tex]\sf \dfrac{1}{cos^2 \theta }[/tex]
[tex]\sf = \left(1 + \tan^2(\theta)\right) - \dfrac{\tan^2(\theta)}{\sin^2(A)} [/tex]
Combine like terms:
[tex]\sf = 1 - \tan^2(\theta) \left(1/\sin^2(A) - 1\right) [/tex]
Express [tex]\sf 1/\sin^2(A) [/tex] as [tex]\sf \csc^2(A) [/tex]:
[tex]\sf = 1 - \tan^2(\theta)\left(\csc^2(A) - 1\right) [/tex]
Recognize that [tex]\sf \csc^2(A) - 1 = \cot^2(A) [/tex]:
Here is how it is:
[tex]\boxed{\boxed{\begin{aligned} csc ^2 A - 1 & = \dfrac{1}{sin^2 A} - 1 \\\\ & = \dfrac{ 1- sin^2 A }{ sin^2 A}\\\\ &= \dfrac{ (sin^2 A + cos^2 A) - sin^2 A}{sin^2 A} \\\\ & = \dfrac{cos^2 A}{sin^2 A}\\\\ & = cot^2 A \end{aligned}}}[/tex]
Now, replace the value of [tex]\sf csc ^2 A - 1 [/tex]
[tex]\sf = 1 - \tan^2(\theta)\cot^2(A) [/tex]
Express [tex]\sf \cot^2(A) [/tex] as [tex]\sf 1/\tan^2(A) [/tex]:
[tex]\sf = 1 - \dfrac{\tan^2(\theta)}{\tan^2(A)} [/tex]
This matches the right-hand side (RHS), so the identity is proven.
Therefore:
[tex]\sf \sec^2(\theta) \left(1 - \dfrac{\sin^2(\theta)}{\sin^2(A)}\right) = 1 - \dfrac{\tan^2(\theta)}{\tan^2(A)} [/tex]