THE GAS-ELECTRIC HYBRID DEMYSTIFIED
BY: SARA R. HOWERTH
Summary:
The gas- electric hybrid demystified article written by Sara R. Howerth
published in 2015 states that as oil resources decline and gas
Child Poverty
Samuel Kunda
7422025
Issues In World Affairs
Thursday December 14, 2017 8:00A.M.
1) UNICEF REPORT CARD 10 2016https:/www.unicef.ca/en/our-work/article/unicef-reportcard-10
This article d
Small bookstore owner
Seller: Hi how are you, my names Sam nice to meet you!
Buyer: my names Cam nice to meet you, how can I help you today?
Seller: im currently selling a new book series called . , i
SECURITY ON TERRORISM- The Shock Doctrine
Samuel Kunda
7422025
Issues In World Affairs
Due: Thursday Dec 7, 11:00 A.M.
On September 11th, 2001 one of the most shocking events occurred in history
that
CHILD POVERTY IN CANADA
Samuel Kunda
7422025
Issues In World Affairs
Due: Thursday January 4th, 2018
Beginning in the late 1990 to early 2000 the child poverty rates drastically
increased, it is estim
The math and stats help centre offers drop-in tutoring for current U of S
students. You are welcome to bring your homework and questions to
Murray Library Rm. 144 to get help from our tutors.
Math and
his quiz is designed to help you review your knowledge of elementary trigonometry and
algebra and to identify any gaps in preparation you may have in these areas. All of the
questions represent materi
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If y
The Mathematics Assistance Centre has been created to aid in
your transition from secondary to university-level
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Content is presented in various modes, both online and
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Statistics Canada indicates that up to one third of post-secondary students feel
overwhelmed by the number of courses most programs ask that they take.
Additionally, university students are asked to b
30
By Theorem 3.3.4, we have that ker(L) = Null([L]). Hence, dim ker(L) = dim Null([L]). Similarly, by Theorem
3.3.6, we have Range(L) = Col([L]). Hence, dim Range(L) = dim Col([L]) = rank[L]. Thus, b
17
3.4 Exercise Solutions
3.4.1 For any ~x Rn we have
c(dL)(~x) = c[dL(~x)]
= (cd)L(~x)
= (cd)L)(~x)
Thus, c(dL) = (cd)L.
by definition of dL
by Theorem 1.1.1 V7
by definition of (cd)L
1.3
Algebraic Expressions
Variable
A variable is:
A letter that can represent any number from
a given set of numbers.
An algebraic expression is:
Variables (e.g. x, y, z) and some real numbers,
comb
Coordinate Geometry
The Coordinate Plane
The Distance and Midpoint Formulas
Graphs of Equations In Two Variables
1.9
Intercepts
Circles
Symmetry
Coordinate Geometry
The coordinate plane is the link be
2
Functions
Chapter Overview
In this chapter, we will learn:
How functions are used to model
real-world situations.
How to find such functions.
We will be covering sections
2.1
2.2
2.3
2.5
Foc
1.10
Lines
The Slope of a Line
Equations of Lines
Parallel and Perpendicular Lines
Applications: Slope as Rate of Change
Lines
In this section, we find equations
for straight lines lying in a coordina
Integumentary System
ANAT 1008
Integumentary System
Made up of:
Skin
Waterproof covering for the body
Protection from UV light, chemicals, etc
Appendages
sweat glands
oil glands
hair and nails
Blood vessels
Blood is transported in different types of vessels:
Arteries carry blood away from the heart
Veins carry blood toward the heart
Capillaries allow for exchange between the
bloodstream
11/17/2014
The Endocrine System
ANAT 1008
Endocrine Function
Endocrine
Nervous
Chemical extension of nervous system which
monitors, regulates & integrates the internal
activities of body.
Endocrine
Electrocardiography
The electrical impulses associated with
contractions of heart muscle also spread
throughout surrounding tissue (skin)
Detectable by an electrocardiograph
through electrical leads
Name_
Date_
Topic 2.1-B Function notation
Our goal in this lesson is to follow up on the function notation lecture with some
experience.
HINTS: (a+b)2 = a2 + 2ab + b2
(a+b)3 = a3 + 3a2b + 3ab2 + b3
1)
The relativistic train spacetime diagram
REFERENCE: None
The first thing we will determine
is how the Lorentz boost will be
drawn in each coordinate system.
(ct)
The Lorentz
We found the analytic solu
Name_
Date_
Topic 2.1-F Derivative shortcuts
Our goal in this lesson is to follow up on the derivative shortcuts lecture and practice
using the rules. Here they are, for your reference.
BASIC RULES:
d
Zero rest mass particles
REFERENCE: Hartle
You may have gleaned from problems and lessons that no particle having a
non-zero rest mass can ever reach the speed of light. The equation for
the energy-mo
Topic 2.2 Extension 03
Differential equations
1)
Recall that the process of finding the derivative has the symbolic
representation d/dt. Thus the derivative of y with respect to t is
represented as dy
Name_
Date_
Topic 2.1-D The derivative
Our goal in this lesson is to follow up on the derivative lecture and develop a shortcut for
finding the derivative. In order to do so, you will have to go throu
Four-vectors
REFERENCE: Hartle
Perhaps you've begun to think about vectors in
(ct)
four-dimensional space - after all, vectors are a
major part of the language of physics. We will
b
call these vectors