AL-WAJID ACADEMY OF SCIENCES
AL-WAJID ACADEMY OF SCIENCES
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Exercise # 1.2 Question # 02 (part-I) | Find f-I (x) and verification of function
Exercise # 1.2 Question # 02 (part-I) | Find f-I (x) and verification of function
zhlédnutí: 33

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Ex #1.2 Q # 1 (Part-I) | Find fog(x), gof(x), fof(x) & gog(x) when f(x) = 2x+1 , g(x) = 3/x-110:35Ex #1.2 Q # 1 (Part-I) | Find fog(x), gof(x), fof(x) & gog(x) when f(x) = 2x+1 , g(x) = 3/x-1
Ex #1.2 Q # 1 (Part-I) | Find fog(x), gof(x), fof(x) & gog(x) when f(x) = 2x+1 , g(x) = 3/x-1
zhlédnutí 7Před 21 dnem
Ex #1.2 Q # 1 (Part-I) | Find fog(x), gof(x), fof(x) & gog(x) when f(x) = 2x 1 , g(x) = 3/x-1
Topic # 2.2 : Vector Addition By Rectangular Components | Resultant Of Vectors By Their Components10:06Topic # 2.2 : Vector Addition By Rectangular Components | Resultant Of Vectors By Their Components
Topic # 2.2 : Vector Addition By Rectangular Components | Resultant Of Vectors By Their Components
zhlédnutí 11Před 21 dnem
Description When adding vectors by their rectangular components, we break each vector into its horizontal (x) and vertical (y) components. Suppose we have two vectors, A and B. The x-components are Ax and Bx​, while the y-components are Ay​ and By​. To find the resultant vector R, we add the x-components and y-components separately: Rx=Ax Bx and Ry=Ay By. The magnitude of the resultant vector i...
Topic # 2.2 : Vector Addition By Rectangular Components | Vector Addition By Their Components8:04Topic # 2.2 : Vector Addition By Rectangular Components | Vector Addition By Their Components
Topic # 2.2 : Vector Addition By Rectangular Components | Vector Addition By Their Components
zhlédnutí 8Před 28 dny
When adding vectors by their rectangular components, we break each vector into its horizontal (x) and vertical (y) components. Suppose we have two vectors, A and B. The x-components are Ax and Bx​, while the y-components are Ay​ and By​. To find the resultant vector R, we add the x-components and y-components separately: Rx=Ax Bx and Ry=Ay By. The magnitude of the resultant vector is calculated...
Topic # 12.16 : Energy Stored In Capacitor part-II | Energy density and its depending factors|8:29Topic # 12.16 : Energy Stored In Capacitor part-II | Energy density and its depending factors|
Topic # 12.16 : Energy Stored In Capacitor part-II | Energy density and its depending factors|
zhlédnutí 16Před 28 dny
Energy stored in a parallel plate capacitor is given by the equation E=1/2CV^2 where C is the capacitance and V is the voltage across the plates. The capacitance C is determined by the area of the plates A, the separation d between them, and the permittivity ϵ of the dielectric material between the plates, as described by C=ϵA/d. Introducing a dielectric medium between the plates increases the ...
Topic # 12.16 : Energy Stored In Capacitor | Energy density and its depending factors|8:26Topic # 12.16 : Energy Stored In Capacitor | Energy density and its depending factors|
Topic # 12.16 : Energy Stored In Capacitor | Energy density and its depending factors|
zhlédnutí 9Před 28 dny
Energy stored in a parallel plate capacitor is given by the equation E=1/2CV^2 where C is the capacitance and V is the voltage across the plates. The capacitance C is determined by the area of the plates A, the separation d between them, and the permittivity ϵ of the dielectric material between the plates, as described by C=ϵA/d. Introducing a dielectric medium between the plates increases the ...
Ex # 1.1 Q # 4 Part (i) , (ii) and (viii) | Questions involving domain & range7:30Ex # 1.1 Q # 4 Part (i) , (ii) and (viii) | Questions involving domain & range
Ex # 1.1 Q # 4 Part (i) , (ii) and (viii) | Questions involving domain & range
zhlédnutí 25Před měsícem
Determining the domain and range of a function involves understanding its input and output values. For instance, consider the linear function f(x) = 2x - 5. The domain of a function is the set of all possible input values (x-values) that the function can accept. For f(x)=2x−5, there are no restrictions on x; hence, the domain is all real numbers, denoted as (−∞,∞). The range of a function is th...
Ex # 1.1 Q # 4 Part (i) , (ii) and (viii) | Questions involving domain & range8:04Ex # 1.1 Q # 4 Part (i) , (ii) and (viii) | Questions involving domain & range
Ex # 1.1 Q # 4 Part (i) , (ii) and (viii) | Questions involving domain & range
zhlédnutí 26Před měsícem
Determining the domain and range of a function involves understanding its input and output values. For instance, consider the linear function f(x) = 2x - 5. The domain of a function is the set of all possible input values (x-values) that the function can accept. For f(x)=2x−5, there are no restrictions on x; hence, the domain is all real numbers, denoted as (−∞,∞). The range of a function is th...
Topic # 12.14 : Capacitance of parallel plate capacito | Dielectric Constant | Prove that C=A𝜖o/d4:23Topic # 12.14 : Capacitance of parallel plate capacito | Dielectric Constant | Prove that C=A𝜖o/d
Topic # 12.14 : Capacitance of parallel plate capacito | Dielectric Constant | Prove that C=A𝜖o/d
zhlédnutí 16Před měsícem
The capacitance of a parallel plate capacitor is influenced by the medium between its plates. When there is no medium (i.e., vacuum or air) between the plates, the capacitance 𝐶 is given by the formula 𝐶=𝜖o𝐴/𝑑, where 𝜖o is the permittivity of free space, 𝐴 is the area of one plate, and 𝑑 is the separation between the plates. Introducing a dielectric medium between the plates changes this capaci...
Topic # 12.14 : Capacitance of parallel plate capacito | Dielectric Constant | Prove that C=A𝜖o/d8:13Topic # 12.14 : Capacitance of parallel plate capacito | Dielectric Constant | Prove that C=A𝜖o/d
Topic # 12.14 : Capacitance of parallel plate capacito | Dielectric Constant | Prove that C=A𝜖o/d
zhlédnutí 18Před měsícem
The capacitance of a parallel plate capacitor is influenced by the medium between its plates. When there is no medium (i.e., vacuum or air) between the plates, the capacitance 𝐶 is given by the formula 𝐶=𝜖o𝐴/𝑑, where 𝜖o is the permittivity of free space, 𝐴 is the area of one plate, and 𝑑 is the separation between the plates. Introducing a dielectric medium between the plates changes this capaci...
Topic # 12.13 : Capacitor | Capacitor and its capacitance | 1Farad = 1Coulomb/1Volt10:32Topic # 12.13 : Capacitor | Capacitor and its capacitance | 1Farad = 1Coulomb/1Volt
Topic # 12.13 : Capacitor | Capacitor and its capacitance | 1Farad = 1Coulomb/1Volt
zhlédnutí 40Před měsícem
A capacitor is an electrical component that stores and releases energy in an electric field. It consists of two conductive plates separated by an insulating material called a dielectric. The ability of a capacitor to store charge is measured by its capacitance, denoted by the symbol C, and is expressed in farads (F). The capacitance depends on the surface area of the plates, the distance betwee...
Topic # 12.12 : Charge On An Electron By Millikan's Method part-II | Millikan's Oil Drop Experiment10:23Topic # 12.12 : Charge On An Electron By Millikan's Method part-II | Millikan's Oil Drop Experiment
Topic # 12.12 : Charge On An Electron By Millikan's Method part-II | Millikan's Oil Drop Experiment
zhlédnutí 32Před měsícem
Millikan's oil drop experiment, conducted by Robert A. Millikan in 1909, was a pivotal scientific endeavor that determined the elementary electric charge, the charge of an electron. In this experiment, tiny oil droplets were sprayed into a chamber where they became electrically charged by friction. The droplets were then subjected to an electric field between two metal plates, and Millikan obse...
Topic # 12.12 : Charge On An Electron By Millikan's Method | Millikan's Oil Drop Experiment8:29Topic # 12.12 : Charge On An Electron By Millikan's Method | Millikan's Oil Drop Experiment
Topic # 12.12 : Charge On An Electron By Millikan's Method | Millikan's Oil Drop Experiment
zhlédnutí 28Před 2 měsíci
Millikan's oil drop experiment, conducted by Robert A. Millikan in 1909, was a pivotal scientific endeavor that determined the elementary electric charge, the charge of an electron. In this experiment, tiny oil droplets were sprayed into a chamber where they became electrically charged by friction. The droplets were then subjected to an electric field between two metal plates, and Millikan obse...
Topic # 4.1 : Work done by a constant force (part-II)| Work and its unit | Work and energy6:56Topic # 4.1 : Work done by a constant force (part-II)| Work and its unit | Work and energy
Topic # 4.1 : Work done by a constant force (part-II)| Work and its unit | Work and energy
zhlédnutí 10Před 2 měsíci
Work, in physics, refers to the transfer of energy that occurs when a force is applied to an object causing it to move. It is defined as the product of the force applied and the displacement of the object in the direction of the force. This relationship is mathematically denoted by the formula 𝑊=𝐹⋅𝑑⋅cos⁡(𝜃), where 𝑊 is work, 𝐹 is the magnitude of the force, 𝑑 is the displacement, and 𝜃 is the a...
Topic # 4.1 : Work done by a constant force | Work and its unit | Work and energy8:06Topic # 4.1 : Work done by a constant force | Work and its unit | Work and energy
Topic # 4.1 : Work done by a constant force | Work and its unit | Work and energy
zhlédnutí 21Před 2 měsíci
Topic # 4.1 : Work done by a constant force | Work and its unit | Work and energy
Exercise # 1.1 Q#06 | Find height of a stone during different time intervals6:11Exercise # 1.1 Q#06 | Find height of a stone during different time intervals
Exercise # 1.1 Q#06 | Find height of a stone during different time intervals
zhlédnutí 12Před 2 měsíci
Exercise # 1.1 Q#06 | Find height of a stone during different time intervals
Exercise # 1.1 Q#05 | Find the values of "a" & "b"8:01Exercise # 1.1 Q#05 | Find the values of "a" & "b"
Exercise # 1.1 Q#05 | Find the values of "a" & "b"
zhlédnutí 10Před 2 měsíci
Exercise # 1.1 Q#05 | Find the values of "a" & "b"
Exercise # 1.1 Q#09 part (i) and (iv) | Even and Odd functions ,Q #098:37Exercise # 1.1 Q#09 part (i) and (iv) | Even and Odd functions ,Q #09
Exercise # 1.1 Q#09 part (i) and (iv) | Even and Odd functions ,Q #09
zhlédnutí 12Před 2 měsíci
Exercise # 1.1 Q#09 part (i) and (iv) | Even and Odd functions ,Q #09
Numerical problem 12.4 & 12.5 | Numerical related to electric field intensity | Zero field location8:48Numerical problem 12.4 & 12.5 | Numerical related to electric field intensity | Zero field location
Numerical problem 12.4 & 12.5 | Numerical related to electric field intensity | Zero field location
zhlédnutí 8Před 2 měsíci
Numerical problem 12.4 & 12.5 | Numerical related to electric field intensity | Zero field location
Numerical problem 12.4 &12.5 12th class physics ch # 12 Electrostatics | zero field location8:31Numerical problem 12.4 &12.5 12th class physics ch # 12 Electrostatics | zero field location
Numerical problem 12.4 &12.5 12th class physics ch # 12 Electrostatics | zero field location
zhlédnutí 16Před 2 měsíci
Numerical problem 12.4 &12.5 12th class physics ch # 12 Electrostatics | zero field location
Exercise # 1.1 Q#08 part (i) and (ii) | Hyperbolic functions ,Q #0811:15Exercise # 1.1 Q#08 part (i) and (ii) | Hyperbolic functions ,Q #08
Exercise # 1.1 Q#08 part (i) and (ii) | Hyperbolic functions ,Q #08
zhlédnutí 10Před 2 měsíci
Exercise # 1.1 Q#08 part (i) and (ii) | Hyperbolic functions ,Q #08
Exercise # 1.1 Q#07 part (i) and (ii) | Parametic functions ,Q #079:45Exercise # 1.1 Q#07 part (i) and (ii) | Parametic functions ,Q #07
Exercise # 1.1 Q#07 part (i) and (ii) | Parametic functions ,Q #07
zhlédnutí 16Před 2 měsíci
Exercise # 1.1 Q#07 part (i) and (ii) | Parametic functions ,Q #07
Topic # 12.9 Electric field as a potential gradient | Prove that E =-∆V/∆r | Prove that V/m = N/C11:29Topic # 12.9 Electric field as a potential gradient | Prove that E =-∆V/∆r | Prove that V/m = N/C
Topic # 12.9 Electric field as a potential gradient | Prove that E =-∆V/∆r | Prove that V/m = N/C
zhlédnutí 14Před 2 měsíci
Topic # 12.9 Electric field as a potential gradient | Prove that E =-∆V/∆r | Prove that V/m = N/C
Topic # 12.9 Electric potential at a point due to a point charge | Prove that V= Kq/r14:54Topic # 12.9 Electric potential at a point due to a point charge | Prove that V= Kq/r
Topic # 12.9 Electric potential at a point due to a point charge | Prove that V= Kq/r
zhlédnutí 10Před 2 měsíci
Topic # 12.9 Electric potential at a point due to a point charge | Prove that V= Kq/r
Exercise # 1.1 Q#3 part (i) and (ii) | Questions related to functions of Ex# 1.18:02Exercise # 1.1 Q#3 part (i) and (ii) | Questions related to functions of Ex# 1.1
Exercise # 1.1 Q#3 part (i) and (ii) | Questions related to functions of Ex# 1.1
zhlédnutí 20Před 2 měsíci
Exercise # 1.1 Q#3 part (i) and (ii) | Questions related to functions of Ex# 1.1
Exercise # 1.1 Q#2 part (i) and (ii) | Questions related to functions of Ex# 1.19:58Exercise # 1.1 Q#2 part (i) and (ii) | Questions related to functions of Ex# 1.1
Exercise # 1.1 Q#2 part (i) and (ii) | Questions related to functions of Ex# 1.1
zhlédnutí 13Před 2 měsíci
Exercise # 1.1 Q#2 part (i) and (ii) | Questions related to functions of Ex# 1.1
Exercise # 1.1 Q#1 part (i) and (iv) | Questions related to functions of Ex# 1.110:39Exercise # 1.1 Q#1 part (i) and (iv) | Questions related to functions of Ex# 1.1
Exercise # 1.1 Q#1 part (i) and (iv) | Questions related to functions of Ex# 1.1
zhlédnutí 17Před 2 měsíci
Exercise # 1.1 Q#1 part (i) and (iv) | Questions related to functions of Ex# 1.1
Topic #2.1 Rectangular or Cartesian coordinate system | Representation of points in 2-D & 3-D11:32Topic #2.1 Rectangular or Cartesian coordinate system | Representation of points in 2-D & 3-D
Topic #2.1 Rectangular or Cartesian coordinate system | Representation of points in 2-D & 3-D
zhlédnutí 25Před 3 měsíci
Topic #2.1 Rectangular or Cartesian coordinate system | Representation of points in 2-D & 3-D
Numerical problem # 6.1 + Example # 6.1 | Problems and examples related to the terminal velocity6:17Numerical problem # 6.1 + Example # 6.1 | Problems and examples related to the terminal velocity
Numerical problem # 6.1 + Example # 6.1 | Problems and examples related to the terminal velocity
zhlédnutí 13Před 3 měsíci
Numerical problem # 6.1 Example # 6.1 | Problems and examples related to the terminal velocity
Topic # 6.2 Terminal velocity and its dependance | Prove that Vt is proportional to r^210:54Topic # 6.2 Terminal velocity and its dependance | Prove that Vt is proportional to r^2
Topic # 6.2 Terminal velocity and its dependance | Prove that Vt is proportional to r^2
zhlédnutí 12Před 3 měsíci
Topic # 6.2 Terminal velocity and its dependance | Prove that Vt is proportional to r^2

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